The theory of contact interaction of deformable solid bodies with circular boundaries, taking into account the mechanical and microgeometric characteristics of the surfaces of Kravchuk Alexander Stepanovich. Analysis of scientific publications within the mechanics of contact interaction in

1. Analysis of scientific publications within the mechanics of contact interaction 6

2. Analysis of the influence of the physical and mechanical properties of materials of contact pairs on the contact area within the framework of the theory of elasticity when the test task of contact interaction with a known analytical solution is implemented. thirteen

3. The study of the contact intense state of the elements of the spherical reference part in the axisymmetric formulation. 34.

3.1. Numerical analysis of the design of the reference part assembly. 35.

3.2. Study of the influence of grooves with a lubricant material of the spherical slide surface on the stress state of the contact node. 43.

3.3. Numerical study of the intense state of the contact node under different materials of the antifriction layer. 49.

Conclusions .. 54.

References .. 57


Analysis of scientific publications within the framework of mechanics of contact interaction

Many nodes and structures used in mechanical engineering, construction, medicine and other areas work under contact interaction. This is usually expensive, difficult to repairable responsible elements to which increased requirements for strength, reliability and durability are presented. Due to the wide use of the theory of contact interaction in mechanical engineering, construction and other areas of human activity, there was a need to consider the contact interaction of the bodies of a complex configuration (design with antifriction coatings and layers, layered bodies, nonlinear contact, etc.), with complex boundary conditions In the contact zone, in conditions of statics and speakers. The basis of the mechanics of contact interaction was laid down by G. Herz, V.M. Alexandrov, L.A. Galin, K. Johnson, I.Ya. Staperman, L. Gudman, A.I. Lurie and other domestic and foreign scientists. Considering the history of the development of the theory of contact interaction as a foundation, the work of Heinrich Hertz "On the contact of the elastic bodies" can be distinguished. In this case, this theory is based on the classical theory of elasticity and mechanics of continuous media, and was represented by the scientific community in the Berlin Physical Society At the end of 1881, scientists have noted the practical importance of the development of the theory of contact interaction, and the research of Hertz was continued, although the theory did not receive due development. The theory initially did not get spread, as it fastened its time and gained popularity only at the beginning of the last century, during the development of mechanical engineering. In this case, it can be noted that the main disadvantage of the theory of Hertz is its applicability only to ideally elastic bodies on the surfaces of the contact, without taking into account friction on the mating surfaces.

At the moment, the mechanics of contact interaction did not lose its relevance, but is one of the most rapidly fluttering the mechanics of the deformable solid. At the same time, each task of the mechanics of contact interaction carries a huge number of theoretical or applied research. Development and improvement of contact theory, when a large number of foreign and domestic scientists continued to develop a large number of foreign and domestic scientists. For example, Alexandrov V.M. Chebakov M.I. Considers the tasks for an elastic half-plane without taking into account and taking into account friction and clutch, also in their productions, the authors take into account lubricant, the heat allocated from friction and wear. The numerical analytical methods of solving the non-classical spatial problems of the mechanics of contact interactions within the linear theory of elasticity are described. A large number of authors worked on a book, which reflects the work until 1975, covering a large number of knowledge about contact interaction. This book contains the results of solutions of contact static, dynamic and temperature tasks for elastic, viscoelastic and plastic tel. A similar publication was published in 2001 containing updated methods and results of solving problems of contact interaction mechanics. It has works not only in domestic, but also foreign authors. N.Kh.Arutyunyan and A.V. Mandry in their monograph investigated the theory of contact interaction of growing tel. A task was set for non-stationary contact problems depending on the time of the contact area and sets out the methods of solving in .Sames V.N. I studied the dynamic contact interaction, and Sargsyan V.S. Considered tasks for semi-positions and strips. In his monograph, Johnson K. reviewed applied contact tasks with taking into account friction, dynamics and heat exchange. Effects were also described as inelasticity, viscosity, damage accumulation, sliding, clutch. Their studies are fundamental to the mechanics of contact interaction in terms of creating analytical and semi-analytical methods to solve the problems of contact of the band, half-space, space and bodies of the canonical form, they also affect contact for bodies with layers and coatings.

Further development of the mechanics of contact interaction is reflected in the works of Goryacheva I.G., Voronina N.A., Torka E.V., Chebakova M.I., M.I. Porter and other scientists. A large number of works considers contact of the plane, half-space or space with an indenter, contact through a layer or a thin coating, as well as contact with layered half-spaces and spaces. Basically, the solution of such contact problems were obtained using analytical and semi-analytical methods, and mathematical contact models are quite simple and, if they take into account the friction between the mating details, the nature of the contact interaction does not take into account. In real mechanisms, part of the design interact with each other and with the surrounding objects. Contact can occur both directly between the bodies and through various layers and coatings. Due to the fact that machine mechanisms and their elements are often geometrically complex structures that work within the framework of the mechanics of contact interaction, the study of their behavior and deformation characteristics is the actual problem of mechanics of the deformable solid body. As examples of such systems, the sliding bearings with a layer of a composite material, endoprosthesis of the thigh with an antifriction layer, a compound of bone and articular cartilage, road coating, pistons, supporting parts of the span structures of bridges and bridge structures, etc. Mechanisms are complex mechanical systems with a complex spatial configuration, which has more than one slide surface, and often contact coatings and layers. In this regard, it is interesting to develop contact problems, including contact interaction through coatings and layers. Goryacheva I.G. In its monograph, the effect of surface microgeometry, the heterogeneity of the mechanical properties of surface layers, as well as the properties of the surface and the films covering it on the characteristics of the contact interaction, the force of friction and the distribution of stresses in the surface layers under different contact conditions are investigated. In his research Torka E.V. Considers the task of sliding a rigid rough indenter along the border of a two-layer elastic half-space. It is assumed that friction forces do not affect the distribution of contact pressure. For the problem of frictional contact of the indenter with a rough surface, the effect of friction coefficient on the voltage distribution is analyzed. The studies of the contact interaction of rigid stamps and viscoelastic bases with subtle coatings are presented for cases when the surfaces of the stamps and coatings are mutual resourcing, are given in. The mechanical interaction of elastic layered bodies is studied in the works, they consider contact of cylindrical, spherical indesters, system of stamps with a elastic layered half-space. A large number of studies have been published about the insertion of multilayer media. Alexandrov V.M. and Mkhitaryan S.M. The methods and results of research on the effects of stamps on bodies with coatings and layers, tasks are considered in the formulation of the theory of elasticity and viscoelasticity. You can select a number of tasks about contact interaction in which friction is taken into account. The presence of a flat contact problem on the interaction of a moving rigid stamp with a viscoelastic layer is considered. The stamp moves with a constant speed and presses with a constant normal force, while it is assumed that friction in the contact area is absent. This task is solved for two types of stamps: rectangular and parabolic. The authors experimentally investigated the effect of sucks from various materials on the heat transfer process in the contact zone. About six samples were considered and experimentally determined that the effective heat insulator is stainless steel aggregate. In another scientific publication, an axisymmetric contact problem of thermoplasticity was considered about the pressure of a hot cylindrical circular isotropic stamp on the elastic isotropic layer, there was a nonideal thermal contact between the stamp and layer. The above works consider the study of a more complex mechanical behavior on the contact interaction site, but the geometry remains in most cases canonical form. Since often in contact structures there are more than 2 surfaces of contact, complex spatial geometry, complex in its mechanical behavior materials and loading conditions, analytical solution to obtain almost impossible for many practically important contact tasks, therefore effective decision methods are required, including numerical. In this case, one of the most important tasks of modeling the mechanics of contact interaction in modern application software packages is the consideration of the influence of the contact pair materials, as well as the compliance of the results of numerical research by existing analytical solutions.

The rupture of the theory and practice to solve the problems of contact interaction, as well as their complex mathematical formulation and descriptions served to the formation of numerical approaches to solving these problems. The most common methods of numerical solution of problems of contact interaction mechanics is the finite element method (MCE). The iterative algorithm of solutions using the MCE for the task of one-way contact is considered in. The solution of contact problems using an extended MCE, which allows to take into account friction on the surface of contacting contacting bodies and their inhomogeneity. The considered publications on the ICE for the problems of contact interaction are not tied to specific elements of the design and often have canonical geometry. An example of the consideration of contact within the framework of the ICE for a real design is where the contact between the blade and the gas turbine engine shovel is considered. Numerical solutions to the problems of contact interaction of multilayer structures and bodies with antifriction coatings and layers are considered in. Publications mainly considers the contact interaction of layered half-spaces and spaces with interements, as well as the pair of canonical-shaped bodies with layers and coatings. Mathematical models of contact are not enough, and the conditions of contact interaction are described poorly. The contact models rarely consider the possibility of preparing, slippages on the contact surface at the same time, slipping with different types of friction and digs. In most publications, mathematical models of problems of deformation of structures and nodes are described, especially boundary conditions on contact surfaces.

At the same time, the study of the tasks of contact interaction of the bodies of real complex systems and structures involves the presence of a base of physical and mechanical, frictional and operational properties of materials of contacting bodies, as well as antifriction coatings and grounds. Often one of the materials of contact pairs are various polymers, including antifriction polymers. The inadequacy of information on the properties of fluoroplastics, compositions on its basis and ultra-high-molecular weight polyethylene of various brands, which restrains their effectiveness to use in many industries. On the basis of National Material Testing Institute of The Stuttgart University Of The Stuttgart University of Technology, a number of inventive experiments were carried out on the definition of the physicomechanical properties of materials used in Europe in contact nodes: PTFE and MSM ultra-molecular weight polyethylene with supplements of soot and plasticizer. But large-scale studies aimed at determining the physico-mechanical and operational properties of viscoelastic media and a comparative analysis of materials suitable for use as material for the sliding surfaces of responsible industrial structures in difficult conditions for deformation in the world and Russia were not conducted. In this regard, there is a need to study the physico-mechanical, friction and operational properties of viscoelastic environments, the construction of models of their behavior and the choice of determining ratios.

Thus, the tasks of studying the contact interaction of complex systems and structures with one and more sliding surfaces are the actual problem of mechanics of the deformable solid body. To current tasks also include: determining the physicomechanical, frictional and operational properties of materials of contact surfaces of real structures and the numerical analysis of their deformation and contact characteristics; Conducting numerical studies aimed at identifying patterns of influence of the physicomechanical and antifriction properties of materials and geometry of contacting bodies to the contact stress-strain state and based on their basis, the development of the methods for predicting the behavior of structural elements during design and non-project loads. And also relevant research on the influence of the physicomechanical, friction and operational properties of materials entering into contact interaction. The practical implementation of such tasks is possible only with numerical methods focused on parallel computing technologies, with the involvement of modern multiprocessor computing.


Analysis of the influence of the physico-mechanical properties of materials of contact pairs on the contact area within the framework of the theory of elasticity when implementing the test task of contact interaction with a known analytical solution

The influence of the properties of the contact pair materials on the parameters of the contact interaction site will be considered on the example of solving the classical contact problem on the contact interaction of the two in contacts of the splashes (Fig. 2.1.). We will consider the task of the interaction of spheres within the framework of the theory of elasticity, the analytical solution of this problem is considered A.M. Katz in.

Fig. 2.1. Contact scheme

As part of the solution of the problem, it is explained that the theory of Hertz Contribute Pressure is to be in the formula (1):

, (2.1)

where - the radius of the contact site, the coordinate of the contact site, is the maximum contact pressure on the site.

As a result of mathematical calculations, as part of the mechanics of contact interaction, formulas were found for the definition and, presented in (2.2) and (2.3), respectively:

, (2.2)

, (2.3)

where and are the radii of contacting spheres, and, - the coefficients of Poisson and the elastic moduli of contacting spheres, respectively.

It can be noted that in formulas (2-3) the coefficient responsible for the mechanical properties of the contact pair of materials has the same look in this way, we denote it In this case, formula (2.2-2.3) have the form (2.4-2.5):

, (2.4)

. (2.5)

Consider the influence of the properties of the materials in contact in the design on the contact parameters. Consider within the framework of the task of contacting the two contacting areas of the following contact pairs of material: steel - fluoroplastic; Steel - composite antifriction material with spherical bronze inclusions (MAC); Steel - modified fluoroplastic. Such a choice of contact pairs of materials is due to further studies of their work with spherical reference parts. The mechanical properties of materials of contact pairs are presented in Table 2.1.

Table 2.1.

Properties of in contact areas

No. p / p Material 1 of the sphere Material 2 spheth
Steel Fluoroplast
, N / m 2 , N / m 2
2E + 11. 0,3 5,45E + 08. 0,466
Steel POPPY
, N / m 2 , N / m 2
2E + 11. 0,3 0,4388
Steel Modified fluoroplastic
, N / m 2 , N / m 2
2E + 11. 0,3 0,46

Thus, for these three contact steam, you can find the contact pair coefficient, the maximum radius of the contact site and the maximum contact pressure, which are presented in Table 2.2. Table 2.2. The contact parameters are calculated under the condition of validity on the spheres with single radii (, m and, m) of comprehensive forces, N.

Table 2.2.

Parameters of contact area

Fig. 2.2. Contact site parameters:

a), m 2 / n; b), m; c), n / m 2

In fig. 2.2. A comparison of the parameters of the contact zone for three contact pairs of materials of the spheres is presented. It can be noted that pure fluoroplast has less, compared to the 2nd other materials, the value of the maximum contact pressure, while the radius of the contact zone has the greatest. The parameters of the contact zone in the modified fluoroplast and poppy are not significantly significant.

Consider the impact of the radii of contacting spheres on the parameters of the contact zone. It should be noted that the dependence of the contact parameters from the radii of the spheres is the same in formulas (4) - (5), i.e. They are part of the formula of the same type, therefore, in order to investigate the effect of contacting radii, it suffices to change the radius of one sphere. Thus, we consider an increase in the radius of the 2nd sphere with a constant value of the radius of the sphere (see Table 2.3).

Table 2.3.

Radius of contacting spheres

No. p / p , M. , M.

Table 2.4.

Contact zone parameters for different radii of contacting spheres

No. p / p Steel-photoplast Steel-Mak. Steel-Fluoroplast
, M. , N / m 2 , M. , N / m 2 , M. , N / m 2
0,000815 719701,5 0,000707 954879,5 0,000701 972788,7477
0,000896 594100,5 0,000778 788235,7 0,000771 803019,4184
0,000953 0,000827 698021,2 0,000819 711112,8885
0,000975 502454,7 0,000846 666642,7 0,000838 679145,8759
0,000987 490419,1 0,000857 650674,2 0,000849 662877,9247
0,000994 483126,5 0,000863 640998,5 0,000855 653020,7752
0,000999 0,000867 634507,3 0,000859 646407,8356
0,001003 0,000871 629850,4 0,000863 641663,5312
0,001006 0,000873 626346,3 0,000865 638093,7642
0,001008 470023,7 0,000875 623614,2 0,000867 635310,3617

Depending on the parameters of the contact zone (maximum contact zone radius and maximum contact pressure) are presented in Fig. 2.3.

Based on the data presented in Fig. 2.3. It can be concluded that with an increase in the radius of one of the contacting areas as the maximum radius of the contact zone and the maximum contact pressure goes to the asymptot. At the same time, as expected, the permissions of the maximum radius of the contact zone and the maximum contact pressure for the three pairs under consideration of contacting materials are the same: as the maximum radius of the contact zone increases, and the maximum contact pressure decreases.

For a more visible comparing the effect of the properties of contacting materials on the contact parameters, we rebuild the maximum radius for the three-studied contact pairs and is similar to the maximum contact pressure (Fig. 2.4.).

Based on the data shown in Figure 4, a similarly small difference of contact parameters in poppy and a modified fluoroplastic, with a clean fluoroplastic with a significant smaller magnitudes of the contact pressure of the contact site radius more than two other materials.

Consider the distribution of contact pressure for three contact pairs of materials while increasing. The distribution of contact pressure is shown along the radius of the contact site (Fig. 2.5.).




Fig. 2.5. Distribution of contact pressure on the contact radius:

a) steel fluoroplastic; b) steel-poppy;

c) steel-modified fluoroplastic

Next, consider the dependence of the maximum radius of the contact site and the maximum contact pressure from bringing closer areas. Consider the action on spheres with single radii (, m and, m) of forces: 1 H, 10 H, 100 H, 1000 H, 10000 H, 100000 H, 1000000 N. The resulting research parameters of contact interaction are presented in Table 2.5.

Table 2.5.

Contact options for magnification

P, N. Steel-photoplast Steel-Mak. Steel-Fluoroplast
, M. , N / m 2 , M. , N / m 2 , M. , N / m 2
0,0008145 719701,5 0,000707 954879,5287 0,000700586 972788,7477
0,0017548 0,001523 2057225,581 0,001509367 2095809,824
0,0037806 0,003282 4432158,158 0,003251832 4515285,389
0,0081450 0,007071 9548795,287 0,00700586 9727887,477
0,0175480 0,015235 20572255,81 0,015093667 20958098,24
0,0378060 0,032822 44321581,58 0,032518319 45152853,89
0,0814506 0,070713 95487952,87 0,070058595 97278874,77

The dependences of the contact parameters are presented in Fig. 2.6.


Fig. 2.6. The dependences of the contact parameters from

for three contact pairs of materials: a), m; b), n / m 2

For three contact pairs of materials, with the growth of squeezing forces, growth occurs, both the maximum radius of the contact area and the maximum contact pressure of Fig. 2.6. At the same time, analogously previously obtained result in pure fluoroplast with a smaller contact pressure of a larger radius.

Consider the distribution of contact pressure for three contact pairs of materials while increasing. The distribution of contact pressure is shown along the radius of the contact site (Fig. 2.7.).

Similarly, the previously obtained results with an increase in the rapprixing forces occur, both the radius of the contact site and the contact pressure, while the character of the distribution of contact pressure is the same in all options for calculations.

Perform the implementation of the task in the ANSYS software package. When creating a finite element grid, the type of elements of Plane182 was used. This type is the four nodal element and has the second procedure for approximation. The element is used for two-dimensional modeling of tel. Each element node has two degrees of freedom UX and UY. This element is also used to calculate the tasks: axisymmetric, with a flat deformed state and with a flat intense state.

In the studied classic tasks, the type of contact pair was used: "Surface - surface". One of the surfaces are assigned target ( Target.), and another contact ( Conta.). Since a two-dimensional task is considered, TARGET169 and CONTA171 end elements are used.

The task is implemented in an axisimaric formulation using contact elements without taking into account friction on mating surfaces. The design scheme of the problem is shown in Fig. 2.8.

Fig. 2.8. Estimated contact scheme of spheres

The mathematical formulation of tasks about the compression of two contacting spheres (Fig.2.8) is implemented within the framework of the theory of elasticity and includes:

equations equations

geometrical relations

, (2.7)

physical relations

, (2.8)

where and - the parameters of Lama, the stress tensor, the strain tensor, is the vector of movements, the radius-vector of an arbitrary point, the first invariant of the deformation tensor, is a single tensor, an area occupied by the sphere area 1, the area occupied by the sphere 2 area.

Mathematical formulation (2.6) - (2.8) is complemented by boundary conditions and conditions of symmetry on surfaces and. In the sphere 1 is the power

for the sphere 2

. (2.10)

The system of equations (2.6) - (2.10) is also complemented by the conditions of interaction on the contact surface, while the two bodies of the conditional numbers of which are 1 and 2. The following types of contact interaction are considered to contact.

- slipping with friction: for friction

, , , , (2.8)

wherein , ,

- for friction slip

, , , , , , (2.9)

wherein , ,

- Flowing

, , (2.10)

- Full clutch

, , , , (2.11)

where - the friction coefficient - the conventions of the coordinate axes lying in the plane tangent to the surface of the contact - move the normal to the corresponding contact boundary - movement in the tangent plane, is the voltage according to the normal boundary, - tangential voltages on the contact border, - The magnitude of the vector of tangent contact stresses.

The numerical implementation of the solution to the contacting task will be implemented on the example of a contact pair of materials steel-fluoroplastic, while the compressive forces N. Such a load selection is due to the fact that for a smaller load, a smaller breakdown of the gene's end elements is needed, which is problematic due to limited resource computing technology.

In the numerical implementation of the contact task, one of the paramount tasks is to assess the convergence of the finite-elemental solution to the contact parameters of the contact parameters. Below is a table 2.6. In which the characteristics of the finite-element models involved in estimating the convergence of the numerical solution of the breaking option.

Table 2.6.

The number of nodal unknowns with various sizes of elements in the task of contacting spheres

In fig. 2.9. Presented the convergence of the numerical solution of the contacting problem.

Fig. 2.9. The convergence of a numerical solution

You can see the convergence of a numerical solution, while the distribution of the contact pressure of the model from 144 thousand nodal unknown has not significant quantitative and qualitative differences from the model from 540 thousand nodal unknown. At the same time, the program's account time is different several times, which is a significant factor in numerical study.

In fig. 2.10. The comparison of the numerical and analytical solution of the problem of controversial areas is shown. The analytical solution of the problem is compared with a numerical solution of the model from 540 thousand nodal unknown.

Fig. 2.10. Comparison of analytical and numerical solutions

It can be noted that the numerical solution of the problem has small quantitative and qualitative differences from the analytical solution.

Similar results on the convergence of a numerical solution were obtained for two remaining contact pairs of materials.

At the same time, at the Institute of Mechanics of Solid Wednesdays Uro RAS D.F.-M.N. A.A.Adamov was performed by the cycle of experimental studies of the deformation characteristics of antifriction polymer materials of contact pairs with complex multi-stage stories of deformation with unloading. The cycle of experimental studies included (Fig. 2.11.): Tests to determine the hardness of the materials on the brinel; Studies under free compression conditions, as well as constrained compression by pressing in a special adaptation with a rigid steel cylindrical samples with a diameter and a long 20 mm. All tests were carried out on the ZWICK Z100SN5A testing machine at strain levels not exceeding 10%.

Tests for determining the hardness of the bringel materials occurred by pressing the ball with a diameter of 5 mm (Fig. 2.11., A). In the experiment, after installing the sample on the substrate to the ball, a preload is applied 9.8 H, which is maintained for 30 seconds. Next, at the speed of movement, the traverse of the machine 5 mm / min The ball is embedded in the sample until the load is 132 H, which is supported by constant for 30 seconds. Then unloading to 9.8 N. The results of the experiment to determine the hardness of the previously mentioned materials are presented in Table 2.7.

Table 2.7.

Material hardness

Cylindrical samples with a diameter and a height of 20 mm were studied under free compression conditions. To implement a homogeneous stress state in a short cylindrical sample on each end of the sample, three-layer gaskets made of fluoroplastic film with a thickness of 0.05 mm, lubricated with low viscosity grease. Under these conditions, the sample compression occurs without noticeable "barcode" during deformations up to 10%. The results of experiments on free compression are shown in Table 2.8.

Results of free compression experiments

Studies in conditions of cramped compression (Fig. 2.11., B) were carried out by pressing cylindrical samples with a diameter of 20 mm, a height of about 20 mm in a special device with a rigid steel rope with permissible limit pressures of 100-160 MPa. In manual mode, the machine control is loaded with a pre-low load (~ 300 H, the axial compression voltage of ~ 1 MPa) to select all the gaps and extrusion of excess lubricant. After that, the sample is maintained for 5 minutes to attense relaxation processes, then the development of a given sample loading program begins.

The experimental data obtained on nonlinear behavior of composite polymer materials is difficult to compare quantitatively. Table 2.9. The values \u200b\u200bof the tangent module M \u003d σ / ε reflecting the stiffness of the sample under conditions of a uniaxial deformed state are given.

Stiffness of the samples in the conditions of a uniaxial deformed state

From the test results, the mechanical characteristics of the materials are also obtained: the modulus of elasticity, the Poisson coefficient, deformation chart

0,000 0,000 -0,000 1154,29 -0,353 -1,923 1226,43 -0,381 -2,039 1298,58 -0,410 -2,156 1370,72 -0,442 -2,268 2405,21 -0,889 -3,713 3439,70 -1,353 -4,856 4474,19 -1,844 -5,540 5508,67 -2,343 -6,044 6543,16 -2,839 -6,579 7577,65 -3,342 -7,026 8612,14 -3,854 -7,335 9646,63 -4,366 -7,643 10681,10 -4,873 -8,002 11715,60 -5,382 -8,330 12750,10 -5,893 -8,612 13784,60 -6,403 -8,909 14819,10 -6,914 -9,230 15853,60 -7,428 -9,550 16888,00 -7,944 -9,865 17922,50 -8,457 -10,184 18957,00 -8,968 -10,508 19991,50 -9,480 -10,838 21026,00 -10,000 -11,202

Table 2.11

Deformation and stress in samples from antifriction composite material based on fluoroplastic with spherical bronze inclusions and molybdenum disulfide

room Time, sec. Extension,% SLV, MPa
0,00000 -0,00000
1635,11 -0,31227 -2,16253
1827,48 -0,38662 -2,58184
2196,16 -0,52085 -3,36773
2933,53 -0,82795 -4,76765
3302,22 -0,99382 -5,33360
3670,9 -1,15454 -5,81052
5145,64 -1,81404 -7,30133
6251,69 -2,34198 -8,14546
7357,74 -2,85602 -8,83885
8463,8 -3,40079 -9,48010
9534,46 -3,90639 -9,97794
10236,4 -4,24407 -10,30620
11640,4 -4,92714 -10,90800
12342,4 -5,25837 -11,18910
13746,3 -5,93792 -11,72070
14448,3 -6,27978 -11,98170
15852,2 -6,95428 -12,48420
16554,2 -7,29775 -12,71790
17958,2 -7,98342 -13,21760
18660,1 -8,32579 -13,45170
20064,1 -9,01111 -13,90540
20766,1 -9,35328 -14,15230
-9,69558 -14,39620
-10,03990 -14,57500

Deformation and voltage in modified fluoroplastic samples

room Time, sec. Deformation axial,% Conditional voltage, MPa
0,0 0,000 -0,000
1093,58 -0,32197 -2,78125
1157,91 -0,34521 -2,97914
1222,24 -0,36933 -3,17885
2306,41 -0,77311 -6,54110
3390,58 -1,20638 -9,49141
4474,75 -1,68384 -11,76510
5558,93 -2,17636 -13,53510
6643,10 -2,66344 -14,99470
7727,27 -3,16181 -16,20210
8811,44 -3,67859 -17,20450
9895,61 -4,19627 -18,06060
10979,80 -4,70854 -18,81330
12064,00 -5,22640 -19,48280
13148,10 -5,75156 -20,08840
14232,30 -6,27556 -20,64990
15316,50 -6,79834 -21,18110
16400,60 -7,32620 -21,69070
17484,80 -7,85857 -22,18240
18569,00 -8,39097 -22,65720
19653,20 -8,92244 -23,12190
20737,30 -9,45557 -23,58330
21821,50 -10,00390 -24,03330

According to the data presented in Tables 2.10.-2.12. Deformation diagrams (Fig. 2.2) are constructed.

According to the results of the experiment, it can be assumed that the description of the behavior of materials is possible within the framework of the deformation theory of plasticity. On test problems, the influence of the elastoplastic properties of the materials was not checked in view of the absence of an analytical solution.

The study of the impact of the physicomechanical properties of materials when working as a contact pair material is considered in Chapter 3 on the real design of the spherical reference part.


1. Modern problems of contact mechanics

Interaction

1.1. Classic hypothesis used when solving contact problems for smooth bodies

1.2. The influence of solid creep on their forming in the area of \u200b\u200bcontact

1.3. Evaluation of ragged rough surfaces

1.4. Analysis of contact interaction of multilayer structures

1.5. Relationship of mechanics and friction and wear problems

1.6. Features of the application of modeling in tribology 31 conclusions on the first chapter

2. Contact interaction of smooth cylindrical bodies

2.1. Solution of the contact problem for smooth isotropic disks and plates with cylindrical cavity

2.1.1. General formulas

2.1.2. Conclusion of the regional condition for movements in the area of \u200b\u200bcontact

2.1.3. The integral equation and its decision 42 2.1.3.1. Study of the obtained equation

2.1.3.1.1. Bringing a singular integrational equation to an integral equation with a kernel with a logarithmic feature

2.1.3.1.2. Rate of the norm of the linear operator

2.1.3.2. Approximate solution of the equation

2.2. Calculation of a fixed connection of smooth cylindrical bodies

2.3. Determination of movement in the movable connection of cylindrical bodies

2.3.1. Solving auxiliary problem for an elastic plane

2.3.2. Solving auxiliary task for an elastic disk

2.3.3. Determination of the maximum normal radial movement

2.4. Comparison of theoretical and experimental data of the study of contact stresses with internal tapping cylinders of close radii

2.5. Simulation of the spatial contact interaction of the system of coaxial cylinders of final sizes

2.5.1. Formulation of the problem

2.5.2. Solution of auxiliary two-dimensional tasks

2.5.3. Solution of the original problem 75 Conclusions and basic results of the second chapter

3. Contact tasks for rough bodies and their solution by adjusting the curvature of the deformed surface

3.1. Spatial nonlocal theory. Geometrical assumptions

3.2. Relative rapprochement of two parallel circles determined by the deformation of roughness

3.3. Method of analytical assessment of roughness deformation

3.4. Determination of movements in the contact area

3.5. Determination of auxiliary coefficients

3.6. Determination of the size of the elliptic area of \u200b\u200bcontact

3.7. Equations for determining the contact area close to circular

3.8. Equations for determining the contact area close to line

3.9. Approximate definition of coefficient A in the case of a contact area in the form of a circle or strip

3.10. Features of the averaging of pressures and deformations when solving a two-dimensional problem of internal contact of rough cylinders of close radii

3.10.1. The output of the integro-differential equation and its solution in the case of internal contact of the rough cylinders

3.10.2. Determination of reprimising coefficients ^ ^

3.10.3. Stressed landing of rough cylinders ^ ^ Conclusions and main results of the third chapter

4. Solution of contact tasks of viscoelasticity for smooth bodies

4.1. Basic provisions

4.2. Analysis of the principles of conformity

4.2.1. Principle of Volterra

4.2.2. Permanent transverse expansion coefficient during creep deformation

4.3. Approximate solution of a two-dimensional contact problem of linear creep for smooth cylindrical tel ^^

4.3.1. Common case of viscoelastic operators

4.3.2. Solution for the monotonous increasing area of \u200b\u200bcontact

4.3.3. Fixed connection solution

4.3.4. Simulation of contact interaction in the case of a uniformly aging isotropic plate

Conclusions and main results of the fourth chapter

5. Creeping surface

5.1. Features of contact interaction bodies with low yield strength

5.2. Construction of a model of deformation of the surface, taking into account the creep in the case of the elliptic area of \u200b\u200bthe contact

5.2.1. Geometrical assumptions

5.2.2. Surveys model model

5.2.3. Determination of medium deformations of the rough layer and medium pressures

5.2.4. Determination of auxiliary coefficients

5.2.5. Determination of the size of the elliptic area of \u200b\u200bcontact

5.2.6. Determination of the size of the circular area of \u200b\u200bcontact

5.2.7. Determination of the width of the contact area in the form of a strip

5.3. The solution of a two-dimensional contact task for the internal touch of rough cylinders, taking into account the creep surface

5.3.1. Setting the problem for cylindrical bodies. INTEGRO-DIFFERENTIAL EQUATION

5.3.2. Determination of reprimising coefficients 160 Conclusions and main results of the fifth chapter

6. Mechanics of the interaction of cylindrical bodies, taking into account the presence of coatings

6.1. Calculation of efficient modules in the theory of composites

6.2. Construction of a self-consistent method for calculating the effective coefficients of inhomogeneous media, taking into account the scatter of physicomechanical properties

6.3. Solution of the contact task for disk and plane with elastic composite coating on the hole circuit

6.3.1. Statement of the task and basic formulas

6.3.2. Conclusion of the regional condition for movements in the area of \u200b\u200bcontact

6.3.3. Integral equation and its decision

6.4. Solution of the problem in the case of orthotropic elastic coating with cylindrical anisotropy

6.5. Determination of the influence of viscoelastic aging coating on changing contact parameters

6.6. Analysis of the features of contact interaction of multicomponent coating and disk roughness

6.7. Modeling contact interaction with taking into account thin metal coatings

6.7.1. Contact ball with plastic coating and rough half-space

6.7.1.1. The main hypotheses and the model of interaction of solid bodies

6.7.1.2. Approximate solution of the task

6.7.1.3. Determination of the maximum contact convergence

6.7.2. Solution of the contact problem for a rough cylinder and a thin metal coating on the opening circuit

6.7.3. Determination of contact hardness with internal contact of cylinders

Conclusions and main results of the sixth chapter

7. Solution of mixed boundary value problems taking into account the wear of surfaces

Interacting tel

7.1. Features of the solution of the contact problem, taking into account the wear of the surfaces

7.2. Setting and solving the problem in the case of elastic deformation of roughness

7.3. Method of theoretical wear assessment, taking into account the creep surface

7.4. Method of wear evaluation, taking into account the effects of coverage

7.5. Final comments on the formulation of flat tasks taking into account the wear

Conclusions and main results of the seventh chapter

Recommended list of dissertations

  • On the contact interaction between thin-walled elements and viscoelastic bodies when cutting and axisymmetric deformation, taking into account the aging factor 1984, Candidate of Physical and Mathematical Sciences Davtyan, Zavena Azibekovich

  • Static and dynamic contact interaction of plates and cylindrical shells with rigid bodies 1983, Candidate of Physical and Mathematical Sciences Kuznetsov, Sergey Arkadyevich

  • Technological support for the durability of machines based on hardening processing with simultaneous application of antifriction coatings 2007, Doctor of Technical Sciences Bersudsky, Anatoly Leonidovich

  • Thermoplastic contact tasks for coatings 2007, Candidate of Physical and Mathematical Sciences of Gubareva, Elena Aleksandrovna

  • Methods of solving contact problems for arbitrary bodies, taking into account the surface roughness by the end element method 2003, Candidate of Technical Sciences Olshevsky, Alexander Alekseevich

The dissertation (part of the author's abstract) on the topic "The theory of contact interaction of deformable solids with circular boundaries, taking into account the mechanical and microgeometric characteristics of surfaces"

The development of technology puts new challenges in the field of the study of the operability of cars and their elements. The increase in their reliability and durability is the most important factor determining the increase in competitiveness. In addition, the elongation of the service life of machinery and equipment, even to a small extent with a large saturation of technology, is equivalent to entering significant new production facilities.

The current state of the work processes of machines in combination with extensive experimental technique to determine the workloads and a high level of development of the applied theory of elasticity, with the existing knowledge of the physicomechanical properties of materials, allow the overall strength of the parts of the machines and devices with a sufficiently large warranty from breakdowns in normal conditions Services. At the same time, the tendency to reduce the largerness of the latter simultaneously with the simultaneous increase in their energy saturation is forced to revise well-known approaches and assumptions when determining the intense state of details and require the development of new settlement models, as well as the improvement of experimental research methods. Analysis and classification of the failures of mechanical engineering products showed that the main reason for the failure under operating conditions is not a breakdown, but wear and damage to their working surfaces.

Increased wear of parts in articulations in some cases violates the tightness of the working space of the machine, in others - the normal lubrication mode, in the third, leads to the loss of kinematic accuracy of the mechanism. Wear and damage to the surfaces reduce the fatigue strength of the parts and can cause their destruction after a certain service life with minor structural and technological concentrators and low rated voltages. Thus, elevated wear violate the normal interaction of parts in nodes, can cause significant additional loads and cause accidental destruction.

All this attracted to the problem of increasing the durability and reliability of cars a wide range of scientists of various specialties, designers and technologists, which allowed not only to develop a number of activities to improve the service life of the machine and create rational methods of care for them, but also on the basis of physics, chemistry, and Metal science to lay the foundations of teaching on friction, wear and lubrication in conjugation.

Currently, the significant efforts of engineers in our country and abroad are aimed at finding ways to solve the problem of determining the contact stresses of interacting parts, because To move on the calculation of the wear of materials to the tasks of structural wear resistance, the contact tasks of the mechanics of the deformable solid body have a decisive role. Significant importance for engineering practice are the solutions of contact problems of the theory of elasticity for bodies with circular boundaries. They constitute the theoretical basis for calculating such elements of machines as bearings, hinged connections, some types of gears, connections with tension.

The widest studies are made using analytical methods. It is the presence of fundamental bonds of modern integrated analysis and the theory of potential with such a dynamic region, as a mechanic, determined their rapid development and use in applied studies. The use of numerical methods is significantly expanding the ability to analyze the stress state in the contact area. At the same time, the bulky of the mathematical apparatus, the need to use powerful computing means significantly restrains the use of existing theoretical developments in solving applied tasks. Thus, one of the actual directions of development of mechanics is to obtain explicit approximate solutions of the tasks of the tasks that provide simplicity of their numerical implementation and with sufficient to practice the accuracy of the described phenomenon. However, despite the progress achieved, while it is difficult to obtain satisfactory results, taking into account local design features and microgeometry of interacting bodies.

It should be noted that the properties of contact have a significant impact on the wear processes, since due to the discreteness of contact with the touch of micronether, only on the individual sites forming the actual area. In addition, the protrusions formed during technological processing are diverse in shape and have different allocation of heights. Therefore, when modeling the topography of surfaces, it is necessary to introduce parameters characterizing the real surface into the statistical laws of distribution.

All this requires the development of a single approach to solving contact problems, taking into account the wear, the most fully taking into account both the geometry of interacting parts, microgeometric and rheological characteristics of surfaces, characteristics of their wear resistance and the possibility of obtaining an approximate solution with the least amount of independent parameters.

Communication of work with major scientific programs, themes. Studies were carried out in accordance with the following themes: "Develop a method for calculating contact stresses with an elastic contact interaction of cylindrical bodies, not described by the theory of Hertz" (Ministry of Education of the Republic of Belarus, 1997, No. 19981103); "The influence of micronics of contacting surfaces on the distribution of contact stresses in the interaction of cylindrical bodies having close in the magnitude of the radii" (Belarusian Republican Foundation Fund, 1996, No. GR 19981496); "Develop a method for predicting the wear of the suspension supports, taking into account the topographic and rheological characteristics of surfaces of interacting parts, as well as the presence of antifriction coatings" (Ministry of Education of the Republic of Belarus, 1998, No. 2009929); "Modeling the contact interaction of machine parts taking into account the randomness of the rheological and geometric properties of the surface layer" (Ministry of Education of the Republic of Belarus, 1999 No. 20001251)

The purpose and objectives of the study. Development of a single method of theoretical prediction of the effect of geometric, rheological characteristics of the roughness of the solid surfaces and the presence of coatings on the stress state in the contact area, as well as the establishment on this basis the patterns of changing the contact rigidity and wear resistance of conjugations on the example of the interaction of bodies with circular boundaries.

To achieve the goal required to solve the following problems:

Develop a method of approximate solution of problems of the theory of elasticity and viscoelasticity on the contact interaction of the cylinder and the cylindrical cavity in the plate using the minimum number of independent parameters.

Develop a nonlocal model of contact interaction of bodies, taking into account the microgeometric, rheological characteristics of surfaces, as well as the presence of plastic coatings.

Enough an approach that allows you to adjust the curvature of interacting surfaces by deformation of roughness.

Develop a method of approximate solution of contact problems for a disk and isotropic, orthotropic with cylindrical anisotropy and viscoelastic aging coatings on the hole in the plate, taking into account their transverse deformability.

Build a model and determine the effect of microgeometric features of the solid surface on the contact interaction with plastic coating on the counter.

Develop a method for solving problems taking into account the wear of cylindrical bodies, the quality of their surfaces, as well as the presence of antifriction coatings.

The object and subject of the study are non-classical mixed objectives of the theory of elasticity and viscoelasticity for bodies with circular boundaries, taking into account the nonlocality of the topographic and rheological characteristics of their surfaces and coatings, on the example of which in this paper developed a comprehensive method for analyzing the intense state in the area of \u200b\u200bcontact depending on the quality indicators their surfaces.

Hypothesis. When solving the boundary challenges, taking into account the quality of the surface of the bodies, a phenomenological approach is used, according to which the roughness deformation is considered as deformation of the intermediate layer.

Tasks with time-changing regional conditions are treated as quasistatic.

Methodology and methods of research conducted. When conducting research, the main equations of the mechanics of the deformable solid body, tribology, functional analysis were used. The method has been developed and substantiated to correct the curvature of loaded surfaces due to the deformations of micronovalities, which significantly simplifies the conducted analytical transformations and allows you to obtain analytical dependencies for the size of the contact area and contact voltages, taking into account the specified parameters without using the assumption about the smallness of the basic measurement of the roughness of the roughness of the roughness Contact area.

When developing a method of theoretical prediction of surface wear, observed macroscopic phenomena were considered as a result of the manifestation of statistically averaged relations.

The accuracy of the results obtained in the work is confirmed by comparisons of the resulting theoretical solutions and the results of experimental studies, as well as comparison with the results of some solutions found by other methods.

Scientific novelty and significance of the results obtained. For the first time, the example of the contact interaction of bodies with circular boundaries was summarizing, and a single method of comprehensive theoretical prediction of the influence of nonlocal geometric, rheological characteristics of rough surfaces of interacting bodies and the presence of coatings on the stress state, contact rigidity and wear resistance of conjugations were developed.

A comprehensive research complex allowed the theoretically substantiated method of solving the problems of solid mechanics, based on a consistent consideration of macroscopically observed phenomena, as the result of the manifestation of microscopic links statistically averaged at a significant portion of the contact surface.

As part of solving the problem:

A spatial nonlocal model of contact interaction of solid bodies with an isotropic surface roughness is proposed.

A method has been developed for determining the effect of the characteristics of the surface of solid bodies on the distribution of stresses.

An integro-differential equation obtained in contact problems for cylindrical bodies was investigated, which made it possible to determine the conditions for the existence and uniqueness of its solution, as well as the accuracy of the constructed approximations.

Practical (economic, social) significance of the results obtained. The results of theoretical studies are brought to acceptable techniques for practical use and can be directly applied during engineering calculations of bearings, sliding supports, gears. The use of the proposed solutions will reduce the time of creating new machine-building structures, as well as with great accuracy to predict their official characteristics.

Some results of the research performed were introduced on the NLP "Cycloprod", Altech NGOs.

The main provisions of the dissertation endowed with the defense:

Approximate solution of the problem of the mechanics of the deformed solid body on the contact interaction of the smooth cylinder and the cylindrical cavity in the plate, with sufficient accuracy of the described phenomenon when using the minimum number of independent parameters.

The solution of nonlocal boundary value problems of the mechanics of the deformable solid, taking into account the geometric and rheological characteristics of their surfaces based on the method, allowing you to correct the curvature of interacting surfaces by deformation of roughness. The absence of assumptions about the smallness of the geometric sizes of the basic lengths of roughness measurement compared with the size of the contact area makes it possible to move to the development of multi-level models for deformation of the surface of solids.

The construction and substantiation of the method for calculating the movements of the boundaries of cylindrical bodies caused by the deformation of the surface layers. The results obtained allow you to develop a theoretical approach that determines the contact stiffness of the conjugation, taking into account the joint influence of all the features of the state of the surfaces of real tel.

Modeling the viscoelastic disk interaction and cavity in a plate of aging material, simplicity of the implementation of the results of which allows them to use them for a wide range of applied tasks.

Approximate solution of contact problems for disk and isotropic, orthotropic with cylindrical anisotropy, as well as viscoelastic aging coatings on the hole in the plate, taking into account their transverse deformability. This makes it possible to assess the effect of composite coatings with a low modulus of elasticity on the loading of conjugates.

Construction of a nonlocal model and determination of the effect of the characteristics of the roughness of the solid surface on the contact interaction with plastic coating on the counter.

Development of the method of solving boundary value problems, taking into account the wear of cylindrical bodies, the quality of their surfaces, as well as the presence of antifriction coatings. On this basis, a methodology that focuses mathematical and physical methods is proposed in the study of wear resistance, which makes it possible instead of research of real friction units to make the main emphasis on the study of the phenomena occurring in the area of \u200b\u200bcontact.

Personal contribution of the applicant. All results endowed with protection are obtained by the author personally.

Approbation of the dissertation results. The results of the research given in the thesis were presented at 22 international conferences and congresses, as well as conferences of the CIS countries and the Republican, among them: "Pontryaginian readings - 5" (Voronezh, 1994, Russia), "Mathematical models of physical processes and their properties" ( Taganrog, 1997, Russia), NordTrib "98 (EBELTOFT, 1998, Denmark), Numerical Mathematics and Computational Mechanics -" NMCM "98" (Miskolc, 1998, Hungary), "Modelling" 98 "(Praha, 1998, Czech Republic), 6th International Symposium on Creep and Coupled Processes (Bialowieza, 1998, Poland), "Computational Methods and Production: Reality, Problems, Perspectives" (Gomel, 1998, Belarus), "Polymer Composites 98" (Gomel, 1998, Belarus), " Mechanika "99" (Kaunas, 1999, Lithuania), II Belarusian Congress on theoretical and applied mechanics

Minsk, 1999, Belarus), INTERNAT. Conf. On Engineering Rheology, Icer "99 (Zielona Gora, 1999, Poland)," TRANSPORT STRENGROUT TRANSPORT TRANSFERS "(St. Petersburg, 1999, Russia), International Conference on MultiField Problems (Stuttgart, 1999, Germany).

Published results. According to the dissertation materials published 40 printed works, among them: 1 monograph, 19 articles in magazines and collections, including 15 articles under personal authorship. The total number of pages of published materials is 370.

Structure and scope of the dissertation. The thesis consists of introduction, seven chapters, conclusions, the list of used sources and applications. A full amount of the thesis is 275 pages, including the volume occupied by illustrations - 14 pages, tables - 1 page. The number of sources used includes 310 items.

Similar dissertation work in the specialty "Mechanics of the deformable solid body", 01.02.04 CIFRA VAC

  • Development and study of the process of smoothing the surface of gas-thermal coatings of textile machine parts in order to increase their performance 1999, Candidate of Technical Sciences Mnatsakanyan, Victoria Uzodovna

  • Numerical simulation of dynamic contact interaction of elastoplastic bodies 2001, Candidate of Physical and Mathematical Sciences Sadovskaya, Oksana Viktorovna

  • Solution of contact problems of the theory of plates and flat non-mersetse contact problems by the method of boundary elements 2004, Candidate of Physical and Mathematical Sciences Malkin, Sergey Aleksandrovich

  • Discrete modeling of rigidity of jammed surfaces with an automated assessment of the accuracy of technological equipment 2004, Candidate of Technical Sciences Korzakov, Alexander Anatolyevich

  • Optimal Design of Contact Couple Parts 2001, Doctor of Technical Sciences Hajiyev Vahid Jalal oglu

Conclusion of dissertation on the topic "Mechanics of the deformable solid body", Kravchuk, Alexander Stepanovich

Conclusion

In the course of the studies, a number of static and quasistatic problems of the mechanics of the deformable solid were also resolved. This allows you to formulate the following conclusions and indicate the results:

1. Contact voltages and surface quality are one of the main factors determining the durability of machine-building structures, which, in combination with a tendency to reduce the mass-darkened machines, the use of new technological and structural solutions leads to the need to revise and clarify the approaches and assumptions used in determining the stress state. , movements and wear in pairing. On the other hand, the bulky of the mathematical apparatus, the need to use powerful computing means is significantly contained by the use of existing theoretical developments in solving applied tasks and determine as one of the main directions of development of mechanics to obtain explicit approximate solutions of the tasks delivered, providing simplicity of their numerical implementation.

2. The approximate solution of the problem of the mechanics of the deformable solid body on the contact interaction of the cylinder and the cylindrical cavity in the plate with a minimum number of independent parameters is constructed, with sufficient accuracy describing the studied phenomenon.

3. For the first time, nonlocal boundary value problems of the theory of elasticity were solved, taking into account the geometric and rheological characteristics of roughness based on a method, allowing to correct the curvature of interacting surfaces. The absence of assumptions about the smallness of the geometric sizes of the basic measurement lengths of roughness compared with the size of the contact area makes it possible to correctly supply and solve the problem of the interaction of solid tel, taking into account the microgeometry of their surfaces with relatively small contact sizes, as well as go to the creation of multi-level roughness deformation models.

4. A method for calculating the highest contact displacements in the interaction of cylindrical tel is proposed. The results obtained allowed us to construct a theoretical approach that determines the contact rigidity of the conjugation taking into account the microgeometric and mechanical features of the surfaces of real tel.

5. Modeling the viscoelastic disk interaction and cavity in the plate made of aging material, the simplicity of the implementation of the results of which allows them to use them for a wide range of applied tasks.

6. Contact problems for the disk and isotropic, orthotropic, with cylindrical anisotropy and viscoelastic aging coatings on the hole in the plate, taking into account their transverse deformability, are solved. This makes it possible to assess the effect of composite antifriction coatings with a low modulus of elasticity.

7. The model was constructed and the effect of the surface microgeometry of one of the interacting bodies and the presence of plastic coatings on the surface of the counter. This makes it possible to emphasize the leading effect of the characteristics of the surface of real composite bodies in the formation of the area of \u200b\u200bcontact and contact stresses.

8. A general method of solving cylindrical bodies, the quality of their antifriction coatings has been developed. boundary value problems with the wear of surfaces, as well as availability

References dissertation research doctor of Physical and Mathematical Sciences Kravchuk, Alexander Stepanovich, 2004

1. Ainbinder S.B., Tunina E.L. Introduction to the theory of friction of polymers. Riga, 1978. - 223 p.

2. Alexandrov V.M., Mkhitaryan S.M. Contact tasks for bodies with thin coatings and layers. M.: Science, 1983. - 488 p.

3. Alexandrov V.M., Romanis B.L. Contact tasks in mechanical engineering. -M.: Mechanical Engineering, 1986. 176 p.

4. Alekseev V.M., Tumanova Oh. Alekseeva A.B. Characteristics of contact of unit irregularities in the conditions of elastic-plastic deformation friction and wear. - 1995. - T.16, N 6. - P. 1070-1078.

5. Alekseev N.M. Metal coatings of sliding supports. M: Mechanical engineering, 1973. - 76 p.

6. Alekhin V.P. Physics of the strength and plasticity of surface layers of materials. M.: Science, 1983. - 280 p.

7. Aliz M.I., Lipanov A.M. Creating mathematical models and methods for calculating hydrogeodynamics and deformation of polymeric materials. // Problems Mechan. and material scientist. Vol. 1 / RAS URO. In-ts fur. - Izhevsk, 1994. P. 4-24.

8. Amosov I.S., Scrana V.A. Accuracy, vibrations and surface cleanliness with turning. M.: Mashgiz, 1953. - 150 s.

9. Andreykiv A.E., Chernets M.V. Evaluation of contact interaction of rubbing parts of machines. Kiev: Nukova Dumka, 1991. - 160 p.

10. ANTONEVICH AB, Radino Ya.V. Functional analysis and integral equations. MN: Publishing House "University", 1984. - 351 p.

11. P.Arutyunyan N.Kh., Zevin A.A. Calculation of building structures, taking into account creep. M.: Stroyzdat, 1988. - 256 p.

12. Harutyunyan N.Kh. Kolmanovsky V.B. The theory of creep inhomogeneous bodies. -M.: Science, 1983.-36 p.

13. Atopov V.I. Contact system hardness control. M: Mechanical engineering, 1994. - 144 p.

14. Buckley D. Surface phenomena with adhesion and friction interaction. M.: Mechanical Engineering, 1986. - 360 p.

15. Bowls N.S. Panasenko G.P. Averaging processes in periodic tasks. Mathematical problems of mechanics of composite materials. -M.: Science, 1984. 352 p.

16. Bowls N.S., Egohlist M.E. Effective modules of thin-walled structures // Bulletin of Moscow State University, Ser. 1. Mathematics, mechanics. 1997. - № 6. -s. 50-53.

17. Belokon A.B., Vorovich I.I. Contact problems of the linear theory of viscoelasticity without taking into account the forces of friction and clutch // Izv. Academy of Sciences of the USSR. MTT. -1973, -№6.-C. 63-74.

18. Belousov V.Ya. Durability of machine parts with composite materials. Lviv: Summing up School, 1984. - 180 s.

19. Berestenev O.V., Kravchuk A.C., Yankevich N.S. Development of the method for calculating the contact strength of the magazine gearing of planetary vegetables gearboxes // Progressive gears: Sat. Dokl., Izhevsk, June 28-30, 1993 / or. Izhevsk, 1993. - P. 123-128.

20. Berestenev O.V., Kravchuk A.C., Yankevich N.S. Contact strength of highly loaded parts of planetary retardant gearboxes // Gear Transmissions-95: Proc. Oftern. Congress, Sofia, 26-28 september, 1995. P. 6870.

21. Beretnev O.B., Kravchuk A.C., Yankevich H.C. Contact interaction of cylindrical bodies // Reports of the NAM. 1995. - T. 39, No. 2. - P. 106-108.

22. Blend D. Theory of linear viscoelasticity. M.: Mir, 1965. - 200 p.

23. Bobkov V.V., Krylov V.I., Monastery P.I. Computational methods. In 2 volumes. Tom I. M.: Science, 1976. - 304 p.

24. B. B. B. B. Novichkov Yu.N. Mechanics of multilayer structures. M.: Mechanical Engineering, 1980. - 375 p.

25. Bondarev E.A., Bugaeva V.A., E.JI Gusev. Synthesis of layered shells from a finite set of viscoelastic materials // Izv. RAS, MTT. 1998. - № 3. -C. 5-11.

26. Bronstein I.N., Semeseseev A.C. Mathematics reference for engineers and student atys. M.: Science, 1981. - 718 p.

27. Bryzgalin G.I. Tests for creep plastic plates // Journal of applied mathematics and technical physics. 1965. - No. 1. - P. 136-138.

28. Bulgakov I.I. Remarks on the hereditary theory of creep metal // Journal of Applied Mathematics and Technical Physics. 1965. - No. 1. - P. 131-133.

29. Burya A.I. The influence of the nature of the fiber friction and wear of the carbon fiber // On the nature of the friction of solids: Tez. Dokl. International Symposium, Gomel 8-10 June, 1999 / IMMS NANB. Gomel, 1999. - P. 44-45.

30. Bushuev V.V. Basics of designing machine tools. M.: Stankin, 1992. - 520 p.

31. Weinstein VE, Trojanovskaya G.I. Dry lubricants and self-lubricating materials. - M.: Mechanical engineering, 1968. 179 p.

32. Van Fo Fa G.A. Theory of reinforced materials. Kiev: Sciences, Dum., 1971.-230 p.

33. Vasiliev A.A. Continual modeling of deformation of a two-row finite discrete system, taking into account boundary effects // Bulletin of Moscow State University, Ser. 1 Mat., Fur, - 1996. No. 5. - P. 66-68.

34. Wittenberg Yu.R. Surface roughness and methods of its assessment. M.: Shipbuilding, 1971.- 98 p.

35. Vityaz V.A., Ivashko B.C., Ilyushenko A.F. Theory and practice of applying protective coatings. MN: Belarusian Nauguka, 1998. - 583 p.

36. Vlasov V.M., Nechaev Ji.M. The performance of high-strength thermal diffusion coatings in machine friction nodes. Tula: Priokskoye KN. Publishing house, 1994. - 238 p.

37. Volkov S.D., Stavrov V.P. Statistical mechanics of composite materials. Minsk: Publishing House BSU. IN AND. Lenin, 1978. - 208 p.

38. Volterra V. Theory of functionals, integral and integro differential equations. M.: Nauka, 1982. - 302 p.

39. Questions of analysis and approximation: Sat. scientific papers / Academy of Sciences of the Institute of Mathematics; Rate: Korneychuk N.P. (Avd. Ed.) and others. Kiev: Institute of Mathematics Academy of Sciences of the USSR, 1989, - 122 p.

40. Voronin V.V., Tsetskocho V.A. Numerical solution of the integral equation of the first kind with a logarithmic feature of the interpolation and collocation method // Vyshl magazine. mat. and mat. Physics. 1981. - T. 21, No. 1. - P. 40-53.

41. Galin L.A. Contact tasks of the theory of elasticity. M.: Gostichizdat, 1953.264 p.

42. Galin L.A. Contact tasks of the theory of elasticity and viscoelasticity. M.: Science, 1980, - 304 p.

43. Garkunov D.N. Tribological engineering. M.: Mechanical Engineering, 1985. - 424 p.

44. Gartman E.V., Mironovich L.L. Wear-resistant protective polymer coatings // friction and wear. -1996, t. 17, No. 5. P. 682-684.

45. Gafner S.L., Proshydn M.N. To the calculation of the angle of contact with the internal contact of cylindrical bodies, the radii of which is almost equal // Machine studies. 1973. - № 2. - P. 69-73.

46. \u200b\u200bHakhov F.D. Regional tasks. M.: Science, 1977. - 639 p.

47. Gorshkov A.G., Tarlakovsky D.V. Dynamic contact tasks with movable boundaries. -M.: Science: Fizmatlit, 1995.-351 p.

48. Goryacheva I.G. Calculation of contact characteristics, taking into account the parameters of the macro and microgeometry of surfaces, friction and wear. 1999. - t. 20, No. 3. - pp. 239-248.

49. Goryacheva I.G., Goryachev A.P., Sadiei F. Contacting elastic bodies with thin viscoelastic coatings under conditions of rolling or slipping // Golf. Mat. And fur. t. 59, vol. 4. - pp. 634-641.

50. Goryacheva I.G., Proshydn N.M. Contact tasks in tribology. M.: Mechanical Engineering, 1988. - 256 p.

51. Goryacheva I.G., Makhovskaya Yu.Yu. Adhesion in the interaction of elastic tel // On the nature of friction of solids: Tez. Dokl. International Symposium, Gomel 8-10 June, 1999 / IMMS NANB. Gomel, 1999. - P. 31-32.

52. Goryacheva I.G., Torka E.V. The intense state of a two-layer elastic base with incomplete clutch of layers // friction and wear. 1998. -t. 19, №3, -s. 289-296.

53. Mushroom V.V. The solution of tribotechnical problems with numerical methods. M.: Science, 1982. - 112 p.

54. Grigoluk E.I., Tolkachev V.M. Contact tasks, theory of plates and shells. M.: Mechanical Engineering, 1980. - 416 p.

55. Grigoluk E.I., Filyptinsky L.A. Perforated plates and shells. M.: Science, 1970. - 556 p.

56. Grigoluk E.I., Filyptinsky L.A. PERIODICAL CUTTING STRUCTURES. M.: Science, 1992. - 288 p.

57. Gromov V.G. On the mathematical content of the Volterra principle in the boundary task of viscoelasticity // Golf. Mat. And fur. 1971. - T. 36., No. 5, - P. 869-878.

58. Gusev E.L. Mathematical methods of synthesis of layered structures. -Nosbirsk: Science, 1993. 262 p.

59. Danilyuk I.I. Irregular boundary tasks on the plane. M.: Science, 1975. - 295С.

60. Demkin N.B. Contacting rough surfaces. M.: Science, 1970.- 227 p.

61. Demkin N.B. The theory of contact of real surfaces and tribology // friction and wear. 1995. - T. 16, No. 6. - P. 1003-1025.

62. Demkin N.B., Izmailov V.V., Kurova M.S. Determination of the statistical characteristics of a rough surface based on the profilograms // Stiffness of machine-building structures. Bryansk: NTO Mashprom, 1976.-s. 17-21.

63. Demkin N.B., Short M.A. Evaluation of the topographic characteristics of a rough surface using profilograms // Mechanics and physics of contact interaction. Kalinin: KSU, 1976. - with. 3-6.

64. Demkin N.B., Ryzhov E.V. Surface quality and contact of machine parts. -M., 1981, - 244 p.

65. Johnson K. Mechanics of contact interaction. M: Mir, 1989. 510 p.

66. Zen I.Ya. Change the coefficient of Poisson with a complete cycle of one-dimensional creep // Mechan. Polymers. 1968. - № 2. - P. 227-231.

67. Dinarov O.Yu., Nikolsky V.N. Determination of relations for viscoelastic medium with microwaves // Blind. Mat. And fur. 1997. - t. 61, vol. 6.-s. 1023-1030.

68. Dmitriev T.V. Sirovatka L.A. Antifriction composite coatings obtained using tribological equipment // Sat. Tr. interddes scientific and technical conf. "Polymer composites 98" Gomel on September 29-30 1998 / IMS NSB. Gomel, 1998. - P. 302-304.

69. PROJECT MN, GAFNER C.JL The influence of friction on the contact parameters of the shaft shaft // Problems of friction and wear. Kiev: Technique. - 1976, No. 3, -s. 30-36.

70. Dotsenko V.A. Wear solids. M.: Qintichimneftemash, 1990. -192 p.

71. Drozdov Yu.N., Kovalenko E.V. Theoretical study of the bearing resource of sliding bearings with the liner // friction and wear. 1998. - T. 19, No. 5. - P. 565-570.

72. Drozdov Yu.N., Naumova N.M., Ushakov B.N. Contact voltages in hinge compounds with sliding bearings // Problems of mechanical engineering and reliability of machines. 1997. - № 3. - P. 52-57.

73. Dunin-Barkovsky I.V. The main directions of the surface quality of the surface in mechanical engineering and instrument making // Bulletin of Mechanical Engineering. -1971. No. 4. - p.49-50.

74. Dyachenko P.E., Jacobson M.O. Surface quality during metal processing cutting. M.: Mashgiz, 1951.- 210 p.

75. Efimov AB, Smirnov V.G. Asymptotically accurate solution of the contact problem for a subtle multilayer coating // Izv. Wounds MTT. -1996. # 2. -C.101-123.

76. Zharin A.Ji. The method of contact difference potentials and its use in tribology. MN: Bestprint, 1996. - 240 s.

77. Zharin A.L., Shipitsa H.A. Methods for studying the surface of metals to register changes in the operation of an electron output // On the nature of friction of solids: Tez. Dokl. International Symposium, Gomel 8-10 June, 1999. / Immsnan. Gomel, 1999. - P. 77-78.

78. Zhdanov GS, Khundjua A.G. Lectures in solid body physics. M: ed-MSU. 1988.-231 p.

79. Zhdanov GS Physics of a solid body. - M MSU, 1961.-501 p.

80. Hemochkin N.B. Theory of elasticity. M., Gosstroyisdat, 1957. - 255 p.

81. Zaitsev V.I., Schavelin V.M. The method of solving contact problems, taking into account the real properties of roughness of surfaces of interacting tel // MTT. -1989. No. 1. - P.88-94.

82. Zakharenko Yu.A., Saplat A.A., Plyashkevich V.Yu. Analytical solution of the equations of the linear theory of viscoelasticity. Application to fuel lines of nuclear reactors. Moscow, 1994. - 34c. - (Preprint / Russian Scientific Center "Kurchatov Institute"; IEE-5757/4).

83. Zengui E. Surface Physics. M.: Mir, 1990. - 536 p.

84. Zolotoshevsky B.C. Mechanical properties of metals. M.: Metallurgy, 1983. -352c.

85. Ilyushin I.I. The method of approximation of structures on the linear theory of thermo-visco-elasticity // Mechan. Polymers. 1968.-№2.-C. 210-221.

86. Inyutin I.S. Electrotenzometric measurements in plastic parts. Tashkent: State. Extras of Uzssr, 1972. 58 p.

87. Karasik I.I. Tribological testing methods in national standards of the countries of the world. M.: Center "Science and Technology". - 327 p.

88. Kalaland A.I. To the contact tasks of the theory of elasticity // Golf. Mat. And fur. 1957. - T. 21, No. 3. - P. 389-398.

89. Kalaland A.I. Mathematical methods of the two-dimensional theory of elasticity // M.: Science, 1973. 304 p.

90. Kalaland A.I. On a direct method of solving the wing equation and its use in the theory of elasticity // Mathematical compilation. 1957. - T.42, # 2. - C.249-272.

91. Kaminsky A.Y., Ruschsky Ya.y. On the applicability of the Volterra principle in the study of the movement of cracks in hereditfully elastic media // Bed. fur. 1969. - t. 5, vol. 4. - P. 102-108.

92. Canav S.K. The method of the self-consistent field in the problem of the effective properties of the elastic composite // Blind. fur. and those. Phys. 1975. - № 4. - P. 194-200.

93. Canav S.K., Levin V.M. The effective field method. Petrozavodsk: Petrozavodsky State. University, 1993. - 600 p.

94. Kachanov L.M. The theory of creep. M: Fizmatgiz, 1960. - 455 p.

95. Kobzev A.B. Construction of a nonlocal model of a different-forming viscoelastic body and a numerical solution of a three-dimensional convection model in the depths of the Earth. Vladivostok. - Khabarovsk.: UFO DVO RAS, 1994. - 38 p.

96. Kovalenko E.V. Mathematical modeling of elastic bodies bounded by cylindrical surfaces // friction and wear. 1995. - T. 16, No. 4. - P. 667-678.

97. Kovalenko E.V., Zelentsov V.B. Asymptotic methods in nonstationary dynamic contact tasks // Blind. fur. and those. Phys. 1997. - T. 38, No. 1. - p.111-119.

98. Kovpack V.I. Prediction of long-term performance of metal materials under creep conditions. Kiev: Academy of Sciences of the USSR, In-t. Strength problems, 1990. - 36 p.

99. Koltunov MA Creep and relaxation. M.: Higher School, 1976. - 277 p.

100. Kolubaev A.B., Fadin V.V., Panin V.E. Friction and wear of composite materials with a multi-level damping structure // friction and wear. 1997. - t. 18, No. 6. - P. 790-797.

101. Combals B.C. The effect of rough solid bodies for friction and wear. M.: Science, 1974. - 112 p.

102. Combals B.C. The development of the theory and methods of increasing the wear resistance of the friction surfaces of machine parts // Problems of engineering and reliability of machines. 1998. - № 6. - P. 35-42.

103. Composite materials. M: Science, 1981. - 304 p.

104. Kravchuk A.C., Chigarev A.B. Mechanics of contact interaction bodies with circular boundaries. Minsk: Technoprint, 2000 - 198 p.

105. Kravchuk A.C. About the intense landing of parts with cylindrical surfaces // New technologies in mechanical engineering and computing technology: Proceedings of X scientific. Conf., Brest 1998 / BPI Brest, 1998. - P. 181184.

106. Kravchuk A.C. Determination of wear of rough surfaces in conjugates of cylindrical sliding supports // Materials, technologies, tools. 1999. - T. 4, No. 2. - s. 52-57.

107. Kravchuk A.C. Contact task for composite cylindrical tel // Mathematical modeling of a deformable solid: Sat. Articles / Ed. O.JI. Swede. Minsk: NTK HAH Belarus, 1999. - P. 112120.

108. Kravchuk A.C. Contact interaction of cylindrical bodies, taking into account the parameters of the roughness of their surface // Applied mechanics and technical physics. 1999. - T. 40, No. 6. - P. 139-144.

109. Kravchuk A.C. Noncast contact of a rough curvilinear body and a body with plastic coating // Theory and practice of mechanical engineering. № 1, 2003 - s. 23 - 28.

110. Kravchuk A.C. Influence of electroplating coatings on the strength of stress planting of cylindrical tel // Mechanics "99: Materials of the II of the Belarusian Congress on theoretical and Applied Mechanics, Minsk, June 28-30, 1999 / IMS Nanb. Gomel, 1999. - 87 p.

111. Kravchuk A.C. The nonlocal contact of the rough bodies according to the elliptical region // Izv. Wounds MTT. 2005 (in print).

112. Kravelsky I.V. Friction and wear. M.: Mechanical Engineering, 1968. - 480 p.

113. Kravelsky I.V, Predychin M.N., Kombals B.C. Basics of calculations for friction and wear. M: Mechanical engineering, 1977. - 526 p.

114. Kuzmenko A.G. Contact tasks taking into account wear for cylindrical slip supports // friction and wear. -1981. T. 2, No. 3. - P. 502-511.

115. Kunin I.A. The theory of elastic media with a microstructure. A nonlocal theory of elasticity, - M.: Science, 1975. 416 p.

116. LANKS A.A. Compression of rough bodies, the contact surfaces of which have a spherical shape // friction and wear. 1995. - T. 16, No. 5. - P.858-867.

117. Levina Z.M., Reshetov D.N. Contact hardness of machines. M: Mechanical engineering, 1971. - 264 p.

118. Lomakin V.A. Flat task of the theory of elasticity of micro-cell phone // Ing. Magazine, MTT. 1966. - № 3. - P. 72-77.

119. Lomakin V.A. The theory of elasticity of heterogeneous bodies. -M.: Publishing House of Moscow State University, 1976. 368 p.

120. Lomakin V.A. Statistical problems of solid mechanics. M.: Science, 1970. - 140 s.

121. Lurie S.A., Yusdi Shahra. On the determination of the effective characteristics of inhomogeneous materials // Fur. compos. Mater, and designs. 1997. - T. 3, No. 4. - P. 76-92.

122. Lyubarsky I.M., Palatnik L.S. Metalophysics friction. M.: Metallurgy, 1976. - 176 p.

123. Malinin H.H. Creeping in the processing of metals. M. Mechanical Engineering, 1986.-216 p.

124. Malinin H.H. Calculations to the creep of the elements of machine-building structures. M.: Mechanical Engineering, 1981. - 221 p.

125. Manevich L.I., Pavlenko A.B. Asymptotic method in micromechanics of composite materials. Kiev: Sleep Sk., 1991. -131 p.

126. Martynenko MD, Romance B.C. On solving the integral equations of the contact problem of the theory of elasticity for rough bodies // Blind. fur. and Mat. 1977. - T. 41, №2. - P. 338-343.

127. Marchenko V.A., Khrulov E.Ya. Regional tasks in areas with a fine-grained boundary. Kiev: sciences. Dumka, 1974. - 280 s.

128. Matvienko V.P., Yurova H.A. Identification of effective elastic permanent composite shells based on statistical and dynamic experiments // Izv. Wounds MTT. 1998. - №3. - S. 12-20.

129. Maharskaya E.I., Gorokhov V.A. Basics of mechanical engineering technology. -Mn.: Higher. Shk., 1997. 423 p.

130. Interlayer effects in composite materials / ed. N. Pegano -M.: Mir, 1993, 346 p.

131. Mechanics of composite materials and structural elements. In 3 tons. T. 1. Mechanics of materials / Guza A.N., Goodune L.P., Vanin G.A. et al. -kiev: Sciences, Dumka, 1982. 368 p.

132. Mechanical properties of metals and alloys / Tikhonov L.V., Kononenko V.A., Prokopenko G.I., Rafalovsky V.A. Kiev, 1986. - 568 p.

133. Milashinovy \u200b\u200bDragan D. Rosioloshko-dynamics of analogue. // fur. Mater, and Design: 36. Rad. Scientific SUCE, 17-19 Apr., 1995, Bograd, 1996. P. 103110.

134. Milov A.B. On the calculation of the contact rigidity of cylindrical compounds // Problems of strength. 1973. - № 1. - P. 70-72.

135. Mozharovsky B.B. Methods for solving contact problems for layered orthotropic tel // Mechanics 95: Sat. Tez. Dokl. Belarusian Congress on theoretical and applied mechanics, Minsk 6-11 February 1995 / BGPA -Gomel, 1995. - P. 167-168.

136. Mozharovsky V.V., Wishkhenko I.V. Mathematical modeling of the interaction of a cylindrical indenter with a fibrous composite material // friction and wear. 1996. - t. 17, No. 6. - P. 738742.

137. Mozharovsky V.V., Starzhinsky V.E. Applied mechanics of layered bodies from composites: flat contact tasks. MN: Science and Technology, 1988. -271 p.

138. Morozov E.M., Grain M.V. Contact problems of destruction mechanics. -M: Mechanical Engineering, 1999. 543 p.

139. Morozov E.M., Kolesnikov Yu.V. Mechanics of contact destruction. M: Science, 1989, 219c.

140. Mushelishvili N.I. Some of the main tasks of the mathematical theory of elasticity. M.: Science, 1966. - 708 p.

141. Mushelishvili N.I. Singular integral equations. M.: Science, 1968. -511c.

142. People's MZ. On a contact task // Dan of the USSR. 1943. - T. 41, No. 6. - P. 244-247.

143. Neemish Yu.N. Spatial boundary problem of mechanics of piecewise homogeneous bodies with non-canonical surfaces of the section // Golf. fur. -1996.-T. 32, №10. - P. 3-38.

144. Nikishin B.C., Shapiro G.S. The tasks of the theory of elasticity for multilayer media. M.: Science, 1973. - 132 p.

145. Nikishin B.C., Kitoroaga T.V. Flat contact tasks of the theory of elasticity with one-sided bonds for multilayer media. Valley Center RAS: Reports on Applied Mathematics, 1994. - 43 p.

146. New substances and products from them as objects of inventions / pancakes

147. B.I., Jermalian V.Yu., Erofeeva S.B. and others. M.: Metallurgy, 1991. - 262 p.

148. Pavlov V.G. Development of tribology at the Institute of Engineering RAS // Problems of Mechanical Engineering and Reliability of Machines. 1998. - № 5. - P. 104-112.

149. Panasyuk V.V. Contact task for a circular hole // Questions of machining and strength in mechanical engineering. 1954. - T. 3, №2. - P. 59-74.

150. Panasyuk V.V., Teply M.I. Ryepodsh dummy in cyclical tshah with an IX inside contact! Dan Ursr, Ser1ya A. - 1971. - № 6. - P. 549553.

151. Pankov A.A. The generalized method of self-consumption: modeling and calculating the effective elastic properties of composites with random hybrid structures // Fur. compos. Mater, and Const. 1997. - T. 3, No. 4.1. C. 56-65.

152. Pankov A.A. Analysis of the effective elastic properties of composites with random structures with a generalized self-consistency method // Izv. Wounds MTT. 1997. - № 3. - P. 68-76.

153. Pankov A.A. Averaging the heat conduction processes in composites with random structures from composite or hollow inclusions with a common method of self-consumption // Fur. compos. Mater, and Const. 1998. - T. 4, No. 4. - P. 42-50.

154. Patone V.Z., Perlin P.I. Methods of mathematical theory of elasticity. -M.: Science, 1981.-688 p.

155. Pelh B.L., Maksimuk A.B., Kowachuk I.M. Contact tasks for layered structural elements. Kiev: sciences. Dum., 1988. - 280 s.

156. Petrokovts M.I. Development of discrete contact models in relation to the metal-polymer friction assemblies: author. diss. . Dokt. those. Sciences: 05.02.04 / IMMS. Gomel, 1993. - 31 s.

157. Petrokovts M.I. Some problems of mechanics in tribology // Mechanics 95: Sat. Tez. Dokl. Belarusian Congress on theoretical and applied mechanics Minsk, February 6-11, 1995 / BGPA. - Gomel, 1995. -s. 179-180.

158. Pinchuk V.G. Analysis of the dislocation structure of the surface layer of metals by friction and the development of methods for increasing their wear resistance: author. diss. . Dokt. those. Sciences: 05.02.04 / IMMS. Gomel, 1994. - 37 p.

159. Victory B.E. Principles of computational mechanics of composites // Fur. compos. Mater. 1996. - T. 32, No. 6. - P. 729-746.

160. Victory B.E. Mechanics of composite materials. M.: Publishing House of Moen, University, 1984, - 336 p.

161. Weather L.I., Golubaev N.F. Approaches and criteria in assessing durability and wear resistance of materials // Problems of engineering and reliability of machines. 1996. - № 3. - P. 44-61.

162. Weather L.I., Chulkin S.G. Modeling the processes of wear of materials and parts of machines based on a structural and energy approach // Problems of mechanical engineering and reliability of machines. 1998. - № 5. - P. 94-103.

163. Poles A.A., Ruzanov F.I. Friction based on self-organization. M.: Science, 1992, - 135 p.

164. Popov G.Ya., Savchuk V.V. Contact task of the theory of elasticity in the presence of a circular area of \u200b\u200bcontact, taking into account the surface structure of contacting tel // Izv. Academy of Sciences of the USSR. MTT. 1971. - № 3. - P. 80-87.

165. Prague V., Hodj F. The theory of perfect plastic tel. M.: Science, 1951. - 398 p.

166. Prokopovich I.E. On solving a flat contact task of the theory of creep // Blind. Mat. And fur. 1956. - T. 20, no. 6. - P. 680-687.

167. Application of creep theories when processing metals pressure / Pozdeev A.A., Tarnovsky V.I., Eremeev V.I., Baakashvili B.C. M., Metallurgy, 1973. - 192 p.

168. Prosov I.A. Thermoelastic anisotropic records. MN: from BSU, 1978 - 200 p.

169. Rabinovich A.C. On solving contact problems for rough bodies // Izv. Academy of Sciences of the USSR. MTT. 1979. - № 1. - P. 52-57.

170. Rabotnov Yu.N. Selected Works. Problems of mechanics of the deformable solid body. M.: Science, 1991. - 196 p.

171. Rabotnov Yu.N. Mechanics of a deformed solid body. M.: Science, 1979, 712 p.

172. Rabotnov Yu.N. Elements of hereditary mechanics of solids. M.: Science, 1977. - 284 p.

173. Rabotnov Yu.N. Calculation of machine parts for creep // Izv. Academy of Sciences of the USSR, rel. 1948. - № 6. - P. 789-800.

174. Rabotnov Yu.N. The theory of creep // Mechanics in the USSR for 50 years, T. 3. -M.: Nauka, 1972. P. 119-154.

175. Calculations for strength in mechanical engineering. In 3 volumes. Volume II: Some tasks of applied theory of elasticity. Calculations outside of elasticity. Calusing / Ponomarev SD, Biderman B.jl, Likharev et al. Moscow: Mashgiz, 1958. 974 p.

176. Rzhanitsyn A.R. The theory of creep. M: Stroyzdat, 1968.-418C.

177. Rosenberg V.M. Creeping metals. M.: Metallurgy, 1967. - 276 p.

178. Romanis N.B. Trap V.P. Destruction of structurally non-uniform bodies. -Riga: Zinane, 1989. 224 p.

179. Ryzhov E.V. Contact hardness of machine parts. M.: Mechanical Engineering, 1966.- 195 p.

180. Ryzhov E.V. Scientific bases of technological management of the quality of the surface of parts under mechanical processing // friction and wear. 1997. -t.18, No. 3. - P. 293-301.

181. Rudzit Ya.A. Microgeometry and contact interaction of surfaces. Riga: Zinane, 1975. - 214 p.

182. Ruschsky Ya.y. On a contact task of a flat theory of viscoelasticity // Blind. fur. 1967. - T. 3, no. 12. - P. 55-63.

183. Savin G.N., Van Fo Fa G.A. Distribution of stresses in a plate of fibrous materials // Blind. fur. 1966. - T. 2, Issue. 5. - p. 5-11.

184. Savin G.N., Ruschsky Ya.y. On the applicability of the Volterra principle // Mechanics of deformable solids and structures. M.: Mechanical Engineering, 1975. - with. 431-436.

185. Savin G.N., Urazgildyaev K.U. The effect of creep and CTLA material on a stressful state near the holes in the plate // Blind. fur. 1970. - T. 6, no. 1, - p. 51-56.

186. Sargsyan B.c. Contact tasks for semi-positions and strips with elastic overlays. Yerevan: Publishing House of Yerevan University, 1983. - 260 s.

187. Sviridenok A.I. Trend of development of tribology in the countries of the former USSR (1990-1997) // friction and wear. 1998, T. 19, No. 1. - P. 5-16.

188. Sviridenok A.I., Chizhik S.A., Petrodovets M.I. Mechanics of discrete friction contact. MN: Woven I Tahshka, 1990. - 272 p.

189. Serfones V.N. The use of creep nuclei and relaxation in the form of an exhibitor amount when solving some problems of linear visco-elasticity by the operator method // Tr. Map. State those. un-ta. 1996. - T. 120, No. 1-4. - WITH.

190. Sirenko G.A. Antifriction carboplastics. Kiev: Technique, 1985.109.125.195С.

191. Spearman Yu.V. Diagnostics and management of service characteristics by tribosystems, taking into account hereditary phenomena: operational information materials / ind Mash BCSR. Minsk, 1985. - 70 p.

192. Skripnyak V.A., Retriderin A.B. Modeling the process of plastic deformation of metallic materials, taking into account the evolution of dislocation substructures // Izv. universities. Physics. 1996. - 39, No. 1. - P. 106-110.

193. Summer A.M., Bulavas F.Ya. Structural theory of reinforced plastics. Riga: Zinane, 1978. - 192 p.

194. Soldatenkov I.A. Solution of the contact problem for the composition of the band-half-plane in the presence of wear with a changing area of \u200b\u200bcontact // Izv. RAS, MTT. 1998. - №\u003e 2. - p. 78-88.

195. Sosnovsky Ji.A., Makhutov H.A., Shurinov V.A. The basic patterns of wear-tight damage. Gomel: Belijt, 1993. -53 s.

196. The resistance of the deformation and plasticity of steel at high temperatures / Tarnovsky I.Ya., Pozdeev A.A., Baakashvili B.C. And others. --TBRI: Sabchota Sakartvelo, 1970. 222 p.

197. Handbook of tributery / under total. ed. Hebda M., Chinadze A.B. In 3 tons. T.1. Theoretical basis. M.: Mechanical Engineering, 1989. - 400 s.

198. Starovoitov E.I., Moskvitin V.V. To the study of the stress-strain state of two-layer metal of polymer plates during cyclic loads // Izv. Academy of Sciences of the USSR. MTT. 1986. - № 1. - P. 116-121.

199. Starovoitov E.I. To bending a round three-layer metal-polymer plate // Theoretical and applied mechanics. 1986. - Vol. 13. - P. 5459.

200. Suslov A.G. Technological support of contact stiffness of the compounds. M.: Science, 1977, - 100 s.

201. Sukharev I.P. The strength of hinge assemblies M.: Mechanical engineering, 1977. - 168 p.

202. Tarikov G.P. To solve the spatial contact problem, taking into account the wear and heat dissipation using electrical modeling, friction and wear. -1992. -T. 13, No. 3. P. 438-442.

203. Tarnovsky Yu.M. Zhigun I.G., Polyakov V.A. Spatially reinforced composite materials. M.: Mechanical Engineering, 1987. -224c.

204. Theory and practice of using wear-resistant and protective-decorative coatings. Kiev: Kiev House of Scientific and Technical Propaganda, 1969. -36 p.

205. Teply M.I. Contact tasks for bodies with circular boundaries. Lviv: Summing up School, 1980. - 176 p.

206. Teply M.I. Determination of wear in a pair of friction shaft-sleeve // \u200b\u200bfriction and wear. -1983. T. 4, No. 2. - P. 249-257.

207. Teply M.I. On the calculation of stresses in cylindrical pairing // Problems of strength. 1979. - № 9. - P. 97-100.

208. Trapeznikov L.P. Thermodynamic potentials in the theory of creep theory of aging media // Izv. Academy of Sciences of the USSR. MTT. 1978. - № 1. - P. 103-112.

209. Tribological reliability of mechanical systems / Drozdov Yu.N., Mudryak V.I., Milet S.I., Drozdova E.Yu. // Problems of mechanical engineering and reliability of machines. - 1997. No. 2. - P. 35-39.

210. Umansky Ya.S., Skakov Yu.A. Metal physics. The atomic structure of metals and alloys. M.: Atomizdat, 1978. - 352 p.

211. Stability of multilayer tribotechnical coatings with small pre-critical deformations / GUZ A.N., Tkachenko E.A., Chekhov V.N., Studdotilov B.C. // Blind. fur. -1996, - t. 32, No. 10. P. 38-45.

212. Fedyukin V.K. Some current issues of determining the mechanical properties of materials. M.: Ipmash RAS. St. Petersburg, 1992. - 43 p.

213. Fedorov C.B. Development of the scientific foundations of the energy method of united by tribosystems: author. diss. . Dokt. those. Sciences 05.02.04 / Nats. those. University of Ukraine / Kiev, 1996. 36 p.

214. The physical nature of the creep of crystalline bodies / Incenbus V.M., Mogilevsky MA, Orlov A.N., Rosenberg V.M. // Magazine Gap. Mat. and those. Phys. 1965. - № 1. - P. 160-168.

215. Goodune L.P., Saltykov N.S. Thermoflasticity of two-component blends. Kiev: sciences. Dumka, 1984. - 112 p.

216. Good R.P., Chicula E.H. The effect of scattering the strength of the components on deformation of the grain composite with micro-conversion // Blind. fur. 1997. - T. 33, No. 8. - P. 39-45.

217. Husu A.P., Witonberg Yu.R., Palmov V.A. Surface roughness (theoretical and probabilistic approach). M.: Science, 1975. - 344 p.

218. Cesnek L.S. Mechanics and microphysics of abrasion of surfaces. M.: Mechanical Engineering, 1979. - 264 p.

219. Tsetskocho V.V. To justify the method of collocation of solving integral equations of the first kind with weak features in the case of open circuits // Incorrect tasks of mathematical physics and analysis. -Nosbirsk: Science, 1984. P. 189-198.

220. Zuckerman S.A. Powder and composite materials. M.: Science, 1976. - 128 p.

221. Cherepanov G.P. Mechanics of the destruction of composite materials. M: Science, 1983. - 296 p.

222. Chernets M.V. On the question of assessing the durability of cylindrical tribosystems of sliding with borders close to circular // friction and wear. 1996. - t. 17, No. 3. - P. 340-344.

223. Chernets M.V. About one method Roses the resource of cylchschdrichny systems Covenne // Presentation Nationally! "Academy of Sciences of Decorations. 1996, No. 1. - P. 4749.

224. Chigarev A.B., Kravchuk A.C. Contact interaction of cylindrical bodies of close radii // Materials, technologies, tools. 1998, No. 1. -C. 94-97.

225. Chigarev A.B., Kravchuk A.C. Contact task for hard disk and composite plate with cylindrical hole // Polymer composites 98: Sat. Tr. interddes scientific and technical Conf., Gomel, September 29-30, 1998 / AMMS Namb Gomel, 1998 - pp. 317-321.

226. Chigarev A.B., Kravchuk A.C. Calculation of the strength of the support of the slip, taking into account the rheology of the roughness of their surfaces // 53rd of the interface. scientific and technical conf. Prof., teacher., Scientific slave and aspir. BGPA: Sat. Tez. Dokl., Part 1. Minsk, 1999 / BGPA Minsk, 1999. - P. 123.

227. Chigarev A.B., Kravchuk A.C. Determination of voltages when calculating the strength of parts of machines bounded by cylindrical surfaces // Applied problems of mechanics of solid media: Sat. Articles. Voronezh: Publishing House of the VSU, 1999. - P. 335-341.

228. Chigarev A.B., Kravchuk A.C. Contact task for hard disk and plate with rough cylindrical hole // Modern problems of mechanics and applied mathematics: Sat. Tez. Dokl., Voronezh, April 1998 / Voronezh: VSU, 1998. p. 78.

229. Chigarev A.B., Chigarev Yu.V. A self-consistent method for calculating the effective coefficients of inhomogeneous media with the non-complicated distribution of physicomechanical properties // Reports of the USSR Academy of Sciences. 1990. -t. 313, №2. - P. 292-295.

230. Chigarev Yu.V. The effect of heterogeneity for stability and contact deformation of rheological environments: author. diss. . Fiz, -mat. Sciences: 01.02.04./ Bel Agrar. those. un-t. Minsk, 1993. - 32 p.

231. Chizhik S.A. Tribeomechanics of precision contact (scanning probe analysis and computer simulation): Author. diss. . Dokt. those. Sciences: 05.02.04. / ICMS Naja. Gomel, 1998. - 40 s.

232. Shemyakin E.I. On one effect of complex loading // Bulletin of Moscow State University. Ser. 1. Mathematics, mechanics. 1996. - № 5. - P. 33-38.

233. Shemyakin E.I., Nikiforovsky B.C. Dynamic destruction of solids. Novosibirsk: Science, 1979. - 271 p.

234. Sheremetyev M.P. Plates with bare edge. Lviv: from Lv-go un-ta, 1960. - 258 p.

235. Shermeror TD The theory of elasticity of micronenel bodies. M.: Science, 1977.-400 p.

236. Shrenkov G.P. Physics and chemistry of friction. MN: University, 1991. - 397 p.

237. Stanman I.Ya. Contact task of the theory of elasticity - M.-L.: Gostichizdat, 1949, - 270 p.

238. Shcherk M. Methodical foundations of systematization of experimental tribological research: ace. in the form of scientific Dokl. . Dokt. those. Sciences: 05.02.04 / IN-T TECHNOLOGATT OPERATION. Moscow, 1996. - 64 p.

239. Shcherk mm fun fun. Methodological foundations of experimental tribological studies // On the nature of friction of solids: Tez. Dokl. International Symposium, Gomel 8-10 June, 1999 / IMMS NANB. -Gomel, 1999. P. 56-57.

240. Aniteescu M. Time-Stepping Methods for Stiff Multi-Rigid-Body Dynamics WITH CONTACT AND FRICTION // Fourth Intern. Congress on Industrial and Applied Mathematics, 5-6 July, 1999, Edinburg, Scotland. P. 78.

241. Bacquias G. Deposition Des Metaux du Proupe Platime // Galvano-Organo. -1979. -N499. P. 795-800.

242. Batsoulas Nicolaos D. Prediction of Metallic Materials Creep Deformation Under Multiaxial Stress State // Steel Res. 1996. - V. 67, N 12. - P. 558-564.

243. Benninghoff H. Galvanische. Uberzuge Gegen Verschleiss // Indastrie-Anzeiger.- 1978. BD. 100, N 23. - S. 29-30.

244. BESTERCI M., IIADEK J. CREP IN DISPERSION STRENGTHENED MATERIALS ON AI BASIS. // POKR. PRASK. Met., Vupm. 1993. - N 3, P. 17-28.

245. Bidmead G.F., Denies G.R. The Potentialities ElectrodePosition and Associated Processes in Engineering Practice // Transactions of the Institute of Metal Finishing.- 1978.-Vol. 56, N3, -P. 97-106.

246. BOLTZMANN L. ZUR THEORIE DER ELASTISCHEN NACHWIRKUNG // Zitzungsber. ACAD. Wissensch. Math. -Naturwiss. Kl. 1874. - B. 70, H. 2. - S. 275-305.

247. Boltzmann L. Zur Theorie der Elastischen Nachwirkung // Ann. Der Phys. Und Chem. 1976, - BD. 7, H. 4. - S. 624-655.

248. Chen J.D., Liu J.h. Chern, JU C.P. Effect of Load On Tribological BEHAVIOR OF CARBON-CARBON COMPOSITES // J. Mater. SEI. 1996. -VOL. 31, N 5. - P. 1221-1229.

249. Chigarev A.V., Kravchuk A.S. CONTACT PROBLEM OF A RIGID DISK AND ISOTROPIC PLATE WITH CYLINDRICAL HOLE // Mechanika. 1997. - № 4 (11). - P. 17-19.

250. Chigarev A.V., Kravchuk A.S. RHEOLOGY OF REAL SURFACE IN PROBLEM FOR INTERIOR CONTACT OF ELASTIC CYLINDERS // Abstracts of Conference "Modelling" 98 ", Praha, Czech Republic, 1998. P. 87.

251. Chigarev A.V., Kravchuk A.S. Effect of Thin Metal Coating On Contact Rigidity // Intern. Conf. ON MULTIFIELD PROBLEMS, OCTOBER 6-8, 1999, STUTTGART, GERMANY. P. 78.

252. Chigarev A.V., Kravchuk A.S. Creep of a Rough Layer in A CONTACT PROBLEM FOR RIGID DISK AND ISOTROPIC PLATE WITH CYLINDRICAL HOLE. // Proc. Of 6th Intern. Symposium on Creep and Coupled Processes Bialaowieza, September 23-25, 1998, Poland. P. 135-142.

253. Chigarev A.V., Kravchuk A.S. Wear and roghness Creep in Contact Problem for Real Bodies. // Proc. Oftern. Conf. "MECHANIKA" 99 ", Kaunas, April 8-9, 1999, Lietuva. P. 29-33.

254. Chigarev A.V., Kravchuk A.S. INFLUENCE OF ROGHNESS RHEOLOGY ON CONTACT RIGIDITY // ICER "99: PROC. OF INTERN. CONF, Zielona Gora, 27-30 June, 1999. P. 417-421.

255. Chigarev A.V., Kravchuk A.S. Thin Homogeneous Growing Old Coating In Contact Problem for Cylinders // Proceedings of 6th International Symposium Insycont "02, Cracow, Poland, September 19th-20th, 2002. P. 136 - 142.

256. Childs T.h.c. The Persistence of Asperities in Indentation Experiments // Wear. -1973, V. 25. P. 3-16.

257. Eck C., Jarusek J. On The Solvability of ThermoviscicoElastic Contact Problems with Coulomb Friction // Intern. Conference on Multifield Problems, October 6-8, 1999, Stuttgart, Germany. P. 83.

258. Egan John. A New Look At Linear Visco Elasticity // Mater Letter. 1997. - V. 31, N3-6.-P. 351-357.

259. Ehlers W., Market B. Intrinsic ViscoLasticity of Porous Materials // Intern. Conference on Multifield Problems, October 6-8, 1999, Stuttgart, Germany. P. 53.

260. Faciu C., Suliciu I. A. Maxwellian Model for PseudoElastic Materials // SCR. Met. Et. Mater. 1994. - V. 31, N 10. - P. 1399-1404.

261. Greenwood J., Tripp J. The Elastic Contact of Rough Spheres // Transactions of the Asme, Ser. D (E). Journal of applied Mechanics. 1967. - Vol. 34, No. 3. - P. 153-159.

262. Hubell F.N. Chemically Deposited Composites A New Generation Of Electrolyses Coating // Transaction Of The Institute of Metal Finishing. - 1978. - Vol. 56, N 2. - P. 65-69.

263. Hubner H., Ostermann A.E. Galvanisch und Chemisch Abgeschiedene Funktionelle Schichten // Metallo-Berflache. 1979. - BD 33, N 11. - S. 456-463.

264. Jarusek J., Eck C. Dynamic Contact Problems WITH FRICTION FOR VISCOELASTIC BODIES EXISTENCE OF SOLUTIONS // INTERN. Conf. ON MULTIFIELD PROBLEMS, OCTOBER 68,1999 STUTTGART, GERMANY. - P. 87.

265. Kloos K., Wagner E., Broszeit E. Nickel Siliciumcarbid -DisperSionsschichten. TEILL. Tribolozische und Tibologich-Chemische EiGenschaften // Metalljberflache. - 1978. - BD. 32, N 8. - S. 321-328.

266. Kowalewski Zbigniew L. Effect of Plastic Prestrain Magnitude ON UNIAXIAL TENSION CREP OF COOPER AT ELEVATEMATURES // MECH. Teor. I Stosow. 1995. -VOL. 33, N3. - P. 507-517.

267. Kravchuk A.S. Mathematic Modelling of Spatial Contact Interaction of A System of Finite Cylindrical Bodies // Technische Mechanik. 1998. - BD 18, H 4. -S. 271-276.

268. Kravchuk A.S. Power Evaluation of the Influence of Roughness On The Value of Contact Stress for Interaction Of Rough Cylinders // Archives of Mechanics. 1998. -N6. - P. 1003-1014.

269. Kravchuk A.S. Contact of Cylinders with Plastic Coating // Mechanika. 1998. -№4 (15). - P. 14-18.

270. Kravchuk A.S. Determination of Contact Stress for Composite Sliding Bearings // Mechanical Engineering. 1999. - № 1. - P. 52-57.

271. Kravchuk A.S. Study of Contact Problem for Disk and Plate with Wearing Hole // Acta Technica CSAV. 1998. - 43. - P. 607-613.

272. Kravchuk A.S. Wear In Interior Contact of Elastic Composite Cylinders // Mechanika. 1999. - №3 (18). - P. 11-14.

273. Kravchuk A.S. Elastic Deformation Energy of A Rough Layer In A CONTACT PROBLEM FOR RIGID DISK AND ISOTROPY PLATE WITH CYLINDRIC HOLE // NORDTRIB "98: PROF.OF THE 8TH INTERN. CONF. On Tribology, Ebeltoft, Denmark, 7 10 June 1998. - P. 113-120.

274. Kravchuk A.S. Rheology of Real Surface in Problem for Rigid Disk and Plate with Hole // Book of Abstr. of conf. NMCM98, Miskolc, Hungary, 1998. P. 52-57.

275. Kravchuk A.S. Effect of Surface Rheology on Contact Displacement // Technische Mechanik. 1999. - Band 19, Heft N 3. - P. 239-245.

276. Kravchuk A.S. Evaluation of contact Rigidity in The Problem for Interaction of Rough Cylinders // Mechanika. 1999. - №4 (19). - P. 12-15.

277. Kravchuk A.S. CONTACT PROBLEM FOR ROUGH RIGID DISK AND PLATE WITH THIN COATING ON CYLINDRICAL HOLE // INT. J. Of Applied Mech. Eng. 2001. - Vol. 6, N 2, P. 489-499.

278. Kravchuk A.S. Time Depend Nonlocal Structural Theory of Contact Of Real Bodies // Fifth World Congress On Computational Mechanics, Vienna July 7-12, 2002.

279. Kunin i.A. Elastic Media with MicroStructure. V I. (One-Dimensional Models). -Springer Series in Solid State Sciences 26, Berlin etc. Springer-Verlag, 1982. 291 p

280. Kunin i.A. Elastic Media with MicroStructure. V II. (Three-Dimensional Models). Springer Series in Solid State Sciences 44, Berlin etc. Springer-Verlag, 1983. -291 p.

281. Lee E.h., Radok J.R.M., Woodward W.B. Stress Analysis for Linear ViscoLastic Materials // Trans. SOC. Rheol. 1959. - Vol. 3. - P. 41-59.

282. Markenscoff X. The Mechanics of Thin Ligaments // Fourth Intern. Congress on Industrial and Applied Mathematics, 5-6 July, 1999, Edinburg, Scotland. P. 137.

283. MIEHE C. Computational Homogenization Analysis of Materials with Microgstructures AT Large Strains // Intern. Conf. ON MULTIFIELD PROBLEMS, OCTOBER 68, 1999, STUTTGART, GERMANY.-P. 31.

284. Orlova A. Instabilities in Compressive Creep in Copper Single Crystals // Z. Metallk. 1995. - V. 86, N 10. - P. 719-725.

285. Orlova A. DISLOCATION SLIP CONDITIONS AND STRUCTES IN COPPER SINGLE CRYSTALS IN CREEP // Z. METALLK. 1995. - V. 86, N 10. - P. 726-731.

286. Paczelt L. Wybrane Problemy Zadan Kontaktowych DLA UKLADOW SPRYZYSTYCH // Mech. Kontactu Powierzehut. Wroclaw, 1988.- C. 7-48.

287. PROBERT S.D., UPPAL A.H. Deformation of Single and Multiple Asperities on Metal Surface // Wear. 1972. - V. 20. - P.381-400.

288. Peng Xianghen, Zeng Hiangguo. A Constitutive Model for Coupled Creep and Plasticity // Chin. J. Appl. Mech. 1997. - V. 14, N 3. - P. 110-114.

289. Pleskachevsky Yu. M., Mozharovsky V.V., Rouba Yu.f. Mathematical Models of Quasi-Static Interaction Between Fibrous Composite Bodies // Computational Methods in Contact Mechanics III, Madrid, 3-5 Jul. 1997. P. 363372.

290. Rajendrakumar P.K., Biswas S.K. Deformation Due To Contact Between A TWO-Dimensional Rough Surface and A Smooth Cylinder // Tribology Letters. 1997. - N 3. -P. 297-301.

291. Schotte J., Miehe C., Schroder J. Modeling The Elastoplastic Behavior of Copper Thin Films on Substrates // INTERN. Conf. ON MULTIFIELD PROBLEMS, OCTOBER 6-8, 1999, STUTTGART, GERMANY. P. 40.

292. Speckhard H. Functionelle Galvanotechnik Eine Einfuhrung. - Oberflache -Surface. - 1978. - BD 19, N 12. - S. 286-291.

293. Still F.A., Dennis J.K. Electrodeposited Wear Resistant Coatings for Hot Forging Dies // Metallurgy and Metal Forming, 1977, Vol. 44, N 1, p. 10-12.

294. Volterra Y. Lecons Sur Les Fonctions de Lisnes. Paris: Gauther - Villard, 1913. -230 p.

295. Volterra V. Sulle Equazioni Integro-Differenziali, Della Theoria Dell Elasticita // Atti Realle Academia Dei Lincei Rend. 1909. - v. 18, N 2. - P. 295-301.

296. Wagner E., Brosgeit E. Tribologische EiGenschaften Von NikeldisperSionsschichten. Grundiagen und Anwendungsbeispiele Aus der Praxis // Schmiertechnik + Tribology. 1979. - BD 26, N 1. - S. 17-20.

297. Wang Ren, Chen Xiaohong. The Progress of Research on Visco-Elastic Constitutive Relations of Polymers // Adv. Mech. 1995. - V 25, N3. - P. 289-302.

298. Xiao Yi, Wang Wen-Xue, Takao Yoshihiro. Two Dimensional Contact Stress Analysis of Composite Laminates WITH Pinned Joint // Bull. RES. Inst. Appl. Mech. -1997. -N81. - p. 1-13.

299. Yang Wei-Hsuin. The CONTACT PROBLEM FOR VISCOELASTIC BODIES // JOURN. Appl. Mechanics, Pap. N 85-APMW-36 (PREPRINT).

Please note the scientific texts presented above are posted for familiarization and obtained by recognizing the original texts of theses (OCR). In this connection, they may contain errors associated with the imperfection of recognition algorithms. In PDF the dissertation and the author's abstracts that we deliver such errors.

480 rub. | 150 UAH. | $ 7.5 ", Mouseoff, Fgcolor," #FFFFCC ", BGColor," # 393939 ");" Onmouseout \u003d "Return nd ();"\u003e Dissertation period - 480 rub., Delivery 10 minutes , around the clock, seven days a week and holidays

Kravchuk Alexander Stepanovich. The theory of contact interaction of deformable solid bodies with circular boundaries, taking into account the mechanical and microgeometric characteristics of surfaces: dis. ... Dr. Fiz.-Mat. Sciences: 01.02.04: Cheboksary, 2004 275 c. RGB OD, 71: 05-1 / 66

Introduction

1. Modern problems of contact interaction mechanics 17

1.1. Classic hypotheses applied when solving contacts for smooth tel 17

1.2. Effect of solid creep on their formation in contact area 18

1.3. Evaluation of the convergence of rough surfaces 20

1.4. Analysis of contact interaction of multilayer structures 27

1.5. Relationship of mechanics and friction and wear problems 30

1.6. Features of the application of modeling in tribology 31

Conclusions on the first chapter 35

2. Contact interaction of smooth cylindrical bodies 37

2.1. Solution of the contact problem for smooth isotropic disks and plates with cylindrical cavity 37

2.1.1. General formulas 38.

2.1.2. Conclusion of the regional condition for movements in the area of \u200b\u200bcontact 39

2.1.3. Integral equation and its decision 42

2.1.3.1. Study of the obtained equation 4 5

2.1.3.1.1. Bringing a singular integro differential equation to an integral equation with a core having a logarithmic feature 46

2.1.3.1.2. Rating of the norm of the linear operator 49

2.1.3.2. Approximate solution of equation 51

2.2. Calculation of a fixed connection of smooth cylindrical tel 58

2.3. Determination of movement in the moving connection of cylindrical tel 59

2.3.1. Solution of auxiliary problem for an elastic plane 62

2.3.2. Solving auxiliary task for elastic disk 63

2.3.3. Determination of the maximum normal radial movement 64

2.4. Comparison of theoretical and experimental data research of contact stresses with internal touch of cylinders of close radii 68

2.5. Modeling the spatial contact interaction of the system of coaxial cylinders of the final dimensions 72

2.5.1. Setting the problem 73.

2.5.2. Solution of auxiliary two-dimensional tasks 74

2.5.3. Solution of the original task 75

Conclusions and main results of the second chapter 7 8

3. Contact tasks for rough bodies and their solution by adjusting the curvature of the deformed surface 80

3.1. Spatial nonlocal theory. Geometrical assumptions 83.

3.2. Relative rapprochement of two parallel circles, determined by the deformation of roughness 86

3.3. Method of analytical assessment of the effect of roughness deformation 88

3.4. Definition of movements in the contact area 89

3.5. Determination of auxiliary coefficients 91

3.6. Determination of the sizes of the elliptic area of \u200b\u200bcontact 96

3.7. Equations for determining the contact area close to circular 100

3.8. Equations for determining the contact area close to line 102

3.9. Approximate determination of the coefficient A in the case of a contact area in the form of a circle or strip

3.10. Features of the averaging of pressures and deformations when solving a two-dimensional problem of internal contact of rough cylinders of close radii 1I5

3.10.1. The output of the integro-differential equation and its solution in the case of internal contact of the rough cylinders 10 "

3.10.2. Determination of ripping coefficients

Conclusions and main results of the third chapter

4. Solution of contact tasks of viscoelasticity for smooth bodies

4.1. Basic provisions

4.2. Analysis of the principles of conformity

4.2.1. Principle of Volterra

4.2.2. Permanent transverse expansion coefficient during creep deformation 123

4.3. Approximate solution of a two-dimensional contact problem of linear creep for smooth cylindrical bodies

4.3.1. Common case of viscoelastic operators

4.3.2. Solution for the monotonous increasing area of \u200b\u200bcontact 128

4.3.3. Solution for fixed connection 129

4.3.4. Simulation of contact interaction in case

uniformly aging isotropic plate 130

Conclusions and main results of the fourth chapter 135

5. Creeping surface 136

5.1. Features of contact interaction bodies with low yield strength 137

5.2. Construction of a model deformation model taking into account creep in the case of an elliptic area of \u200b\u200bcontact 139

5.2.1. Geometrical assumptions 140.

5.2.2. Model Creeping Surface 141

5.2.3. Determination of medium deformations of a rough layer and medium pressures 144

5.2.4. Determination of auxiliary coefficients 146

5.2.5. Determination of the size of the elliptic area of \u200b\u200bcontact 149

5.2.6. Determination of the size of the circular area of \u200b\u200bcontact 152

5.2.7. Determination of the width of the contact area in the form of a strip 154

5.3. Decision of a two-dimensional contact task for internal touch

rough cylinders, taking into account the creep of the surface 154

5.3.1. Setting the problem for cylindrical bodies. Integro-

differential equation 156.

5.3.2. Definition of reprimising coefficients 160

Conclusions and main results of the fifth chapter 167

6. Mechanics interaction of cylindrical bodies, taking into account the presence of coatings 168

6.1. Calculation of efficient modules in the theory of composites 169

6.2. Construction of a self-consistent method for calculating the effective coefficients of inhomogeneous media, taking into account the scatter of physicomechanical properties of 173

6.3. Solution of the contact task for disk and plane with elastic composite coating on the opening circuit 178

6.3. 1 Statement of the problem and the basic formulas 179

6.3.2. Conclusion of the regional condition for movements in the area of \u200b\u200bcontact 183

6.3.3. Integral equation and its decision 184

6.4. Solution of the problem in the case of orthotropic elastic coating with cylindrical anisotropy 190

6.5. Determination of the influence of viscoelastic aging coating on the change in contact parameters 191

6.6. Analysis of the features of contact interaction of multicomponent coating and disk roughness 194

6.7. Simulation of contact interaction taking into account thin metal coatings 196

6.7.1. Contact ball with plastic coating and rough semisimpace 197

6.7.1.1. The main hypotheses and model of interaction of solid bodies 197

6.7.1.2. Approximate solution of problem 200

6.7.1.3. Determination of the maximum contact convergence 204

6.7.2. Solution of the contact problem for a rough cylinder and a thin metal coating on the loop circuit 206

6.7.3. Determination of contact stiffness with internal contact of cylinders 214

Conclusions and main results of the sixth chapter 217

7. Solution of mixed boundary value problems, taking into account the wear of the surfaces of the dressed bodies 218

7.1. Features of the solution of the contact task, taking into account the wear of surfaces 219

7.2. Setting and solving the problem in the case of elastic deformation of roughness 223

7.3. Method of theoretical assessment of wear, taking into account the creep of the surface 229

7.4. Wear appraisal method based on the effect of coverage 233

7.5. Final comments on the formulation of flat tasks taking into account the wear 237

Conclusions and main results of the seventh chapter 241

Conclusion 242.

List of sources used

Introduction to work

The relevance of the topic of the thesis. Currently, the considerable efforts of engineers in our country and abroad are aimed at finding ways to determine the contact stresses of interacting bodies, since to transition from the calculation of the wear of materials to the problems of structural wear resistance, the contact tasks of the mechanics of the deformable solid body have a crucial role.

It should be noted that the most wide studies of contact interaction are made using analytical methods. In this case, the use of numerical methods is significantly expanding the possibilities of analyzing the stress state in the area of \u200b\u200bcontact, taking into account the properties of surfaces of rough bodies.

The need to take into account the structure of the surface is explained by the fact that the protrusions formed during technological processing have different height distribution and touch of microneria occurs only on separate sites forming the actual contact area. Therefore, when simulating the convergence of surfaces, it is necessary to use the parameters characterizing the real surface.

The bulky of the mathematical apparatus used in solving contact problems for rough bodies, the need to use powerful computing means is significantly contained by the use of existing theoretical developments in solving applied tasks. And, despite the progress achieved, while it is difficult to obtain satisfactory results, taking into account the peculiarities of the macro and microgeometry of the surfaces of the interacting bodies, when the surface element on which the characteristics of the roughness of solid bodies are installed, commensurate with the contact area.

All this requires the development of a single approach to solving contact problems, which is most fully taking into account both the geometry of interacting bodies, microgeometric and rheological characteristics of surfaces, characteristics of their wear resistance, and the possibility of obtaining an approximate solution to the problem with the least amount of independent parameters.

Contact problems for bodies with circular boundaries constitute the theoretical basis for calculating such elements of machines as bearings, hinged connections, connections with tension. Therefore, these tasks are usually selected as a model when conducting such studies.

Intensive work carried out in recent years in Belarusian National Technical UniveuiII SI E. Dwishk iIіkishenya

on the solution of this problem and constitute the floor at the Motddododododod ^ s.

Communication of work with brupter scientific programs, themes.

Studies were carried out in accordance with the following themes: "Develop a method for calculating contact stresses with an elastic contact interaction of cylindrical bodies, not described by the theory of Hertz" (Ministry of Education of the Republic of Belarus, 1997, No. 19981103); "The influence of micronics of contacting surfaces on the distribution of contact stresses in the interaction of cylindrical bodies having close in the magnitude of the radii" (Belarusian Republican Foundation Fund, 1996, No. GR 19981496); "Develop a method for predicting the wear of the suspension supports, taking into account the topographic and rheological characteristics of surfaces of interacting parts, as well as the presence of antifriction coatings" (Ministry of Education of the Republic of Belarus, 1998, No. 2009929); "Modeling the contact interaction of machine parts, taking into account the randomness of the rheological and geometric properties of the surface layer" (Ministry of Education of the Republic of Belarus, 1999 № GR2000G251)

The purpose and objectives of the study. Development of a single method of theoretical prediction of the effect of geometric, rheological characteristics of the roughness of the solid surfaces and the presence of coatings on the stress state in the contact area, as well as the establishment on this basis the patterns of changing the contact rigidity and wear resistance of conjugations on the example of the interaction of bodies with circular boundaries.

To achieve the goal required to solve the following problems:

Develop a method of approximate solution of problems of the theory of elasticity and viscoelasticity about Contact interaction of the cylinder and cylindrical cavity in the plate using a mupimal amount of independent parameters.

Develop a nonlocal model of contact interaction
Taking into account microgeometric, rheological characteristics
Surfaces, as well as the presence of plastic coatings.

Justify an approach that allows you to adjust the curvature
interacting surfaces due to the deformation of roughness.

Develop a method of approximate solution of contact problems for disk and isotropic, orthotropic with cylindrical anisotropy and viscoelastic aging coatings on the hole in the plate, taking into account their transverse deformability.

Build a model and determine the effect of microgeometric features of the surface of the solid body to contact interaction with Plastic coating on the counter.

Develop a method for solving problems taking into account the wear of cylindrical bodies, the quality of their surfaces, as well as the presence of antifriction coatings.

The object and subject of the study are non-classical mixed objectives of the theory of elasticity and viscoelasticity for bodies with circular boundaries, taking into account the nonlocality of the topographic and rheological characteristics of their surfaces and coatings, on the example of which in this paper developed a comprehensive method for analyzing the intense state in the area of \u200b\u200bcontact depending on the quality indicators their surfaces.

Hypothesis. When solving the boundary challenges, taking into account the quality of the surface of the bodies, a phenomenological approach is used, according to which the roughness deformation is considered as deformation of the intermediate layer.

Tasks with time-changing regional conditions are treated as quasistatic.

Methodology and methods of research conducted. When conducting research, the main equations of the mechanics of the deformable solid body, tribology, functional analysis were used. The method has been developed and substantiated to correct the curvature of loaded surfaces due to the deformations of micronovalities, which significantly simplifies the conducted analytical transformations and allows you to obtain analytical dependencies for the size of the contact area and contact voltages, taking into account the specified parameters without using the assumption about the smallness of the basic measurement of the roughness of the roughness of the roughness Contact area.

When developing a method of theoretical prediction of surface wear, observed macroscopic phenomena were considered as a result of the manifestation of statistically averaged relations.

The accuracy of the results obtained in the work is confirmed by comparisons of the resulting theoretical solutions and the results of experimental studies, as well as comparison with the results of some solutions found by other methods.

Scientific novelty and significance of the results obtained. For the first time, the example of the contact interaction of bodies with circular boundaries was summarizing, and a single method of comprehensive theoretical prediction of the influence of nonlocal geometric, rheological characteristics of rough surfaces of interacting bodies and the presence of coatings on the stress state, contact rigidity and wear resistance of conjugations were developed.

A comprehensive research complex allowed the theoretically substantiated method of solving the problems of solid mechanics, based on a consistent consideration of macroscopically observed phenomena, as the result of the manifestation of microscopic links statistically averaged at a significant portion of the contact surface.

As part of solving the problem:

A spatial nonlocal contact model has been proposed.
The interactions of solid bodies with isotropic surface roughness.

A method has been developed for determining the effect of the characteristics of the surface of solid bodies on the distribution of stresses.

An integro-differential equation obtained in contact problems for cylindrical bodies was investigated, which made it possible to determine the conditions for the existence and uniqueness of its solution, as well as the accuracy of the constructed approximations.

Practical (economic, social) significance of the results obtained. The results of theoretical studies are brought to acceptable techniques for practical use and can be directly applied during engineering calculations of bearings, sliding supports, gears. The use of the proposed solutions will reduce the time of creating new machine-building structures, as well as with great accuracy to predict their official characteristics.

Some results of the research performed were introduced on N P P P "Cycloprod", NGO "Altech".

The main provisions of the dissertation endowed with the defense:

Approximate decide the task of the deformed mechanics
solid body about the contact interaction of the smooth cylinder and
Cylindrical cavity in the plate, with sufficient accuracy
describing the studied phenomenon when using the minimum
The number of independent parameters.

The solution of nonlocal boundary value problems of the mechanics of the deformable solid, taking into account the geometric and rheological characteristics of their surfaces based on the method, allowing you to correct the curvature of interacting surfaces by deformation of roughness. The absence of assumptions about the smallness of the geometric sizes of the basic lengths of roughness measurement compared with the size of the contact area makes it possible to move to the development of multi-level models for deformation of the surface of solids.

Construction and substantiation of the method of calculating the movements of the boundaries of cylindrical bodies caused by deformation of the surface layers. The results obtained allow to develop a theoretical approach,

contact stiffener with By consideration of the joint influence of all features of the state of the surfaces of real bodies.

Modeling of viscoelastic disk interaction and cavity in
Plate of aging material, ease of implementation of results
which allows you to use them for a wide circle of applied
Tasks.

Approximate solution of contact problems for disk and isotropic, orthotropic with Cylindrical anisotropy, as well as viscoelastic aging coatings on the hole in the plate with By consideration of their transverse deformability. This makes it possible to estimate the effect of composite coatings. with Low modulus of elasticity on the loading of pairs.

Construction of a nonlocal model and determination of the effect of the characteristics of the roughness of the solid surface on the contact interaction with plastic coating on the counter.

Development of the method of solving boundary value problems with By consideration of the wear of cylindrical bodies, the quality of their surfaces, as well as the presence of antifriction coatings. On this basis, a methodology that focuses mathematical and physical methods has been proposed in the study of wear resistance, which makes it possible to make the main emphasis on the study of phenomena taking place instead of research at Contact area.

Personal contribution of the applicant. All results endowed with protection are obtained by the author personally.

Approbation of the dissertation results. The results of the research given in the thesis were presented at 22 international conferences and congresses, as well as conferences of the CIS countries and the Republican, among them: "Pontryaginian readings - 5" (Voronezh, 1994, Russia), "Mathematical models of physical processes and their properties" ( Taganrog, 1997, Russia), NordTrib "98 (EBELTOFT, 1998, Denmark), Numerical Mathematics and Computational Mechanics -" NMCM "98" (Miskolc, 1998, Hungary), "Modelling" 98 "(Praha, 1998, Czech Republic), 6th International Symposium on Creep and Coupled Processes (Bialowieza, 1998, Poland), "Computational Methods and Production: Reality, Problems, Perspectives" (Gomel, 1998, Belarus), "Polymer Composites 98" (Gomel, 1998, Belarus), " Mechanika "99" (Kaunas, 1999, Lithuania), P of the Belarusian Congress on theoretical and applied mechanics (Minsk, 1999, Belarus), Internat. Conf. On Engineering Rheology, Icer "99 (Zielona Gora, 1999, Poland)," TRANSPORT STRENGROUT TRANSPORT TRANSFERS "(St. Petersburg, 1999, Russia), International Conference on MultiField Problems (Stuttgart, 1999, Germany).

Structure and scope of the dissertation. The thesis consists of introduction, seven chapters, conclusions, the list of used sources and applications. The full amount of the thesis is 2 minutes, including the volume occupied by illustrations - 14 pages, tables - 1 page. The number of sources used includes 310 items.

The influence of solid creep on their forming in the area of \u200b\u200bcontact

The practical preparation of analytical dependencies for stresses and displacements in a closed form for real objects, even in the simplest cases, is associated with significant difficulties. As a result, when considering contact tasks, it is customary to resort to idealization. So, it is believed that if the dimensions of the bodies themselves are sufficiently large compared to the size of the contact area, the voltages in this zone are weakly dependent on the configuration of the bodies away from the contact area, as well as the method of their consolidation. At the same time, the voltage with a fairly good degree of reliability can be calculated by considering each body as an infinite elastic medium bounded by a flat surface, i.e. As an elastic half-space.

The surface of each body is assumed to topographically smooth on micro and macro levels. At the micro-level, this means the absence or invoking the micronetics of contacting surfaces, which would determine the incomplete fit of the contact surfaces. Therefore, the real area of \u200b\u200bcontact that is formed on the tops of the protrusions is significantly less theoretical. On the macro level, surface profiles are considered continuous in the contact zone along with the second derivatives.

These assumptions were first used by Herz when solving the contact task. The results obtained on the basis of its theory satisfactorily describe the deformed state of ideally elastic bodies in the absence of friction on the contact surface, but not applicable, in particular, to low-modulus materials. In addition, the conditions in which the theory of hertz is used is violated when considering the contact of the agreed surfaces. This is due to the fact that due to the application of the load, the size of the contact area is rapidly growing and can reach the values \u200b\u200bcomparable to the characteristic sizes of contacting bodies, so that the bodies cannot be considered as elastic half-space.

Of particular interest in solving contact tasks causes taking into account the forces of friction. At the same time, the last on the surface of the section of the two bodies of the agreed form, which are in normal contact;, plays a role only at relatively high friction coefficient values.

The development of the theory of contact interaction of solid bodies is associated with the refusal to the hypotheses listed above. It was carried out in the following main areas: the complication of the physical model of deformation of solids and (or) the refusal to the hypotheses of smoothness and the homogeneity of their surfaces.

Interest in creep sharply increased due to the development of technology. Among the first researchers, found the phenomenon of deformation of materials in time at a constant load, were Vika, Weber, Kollarush. Maxwell first presented the law of deformation in time in the form of a differential equation. A somewhat later Bolygman created a common apparatus for describing linear creep phenomena. This device, significantly developed subsequently Volterra, is currently a classic section of the theory of integral equations.

Until the middle of the last century, elements of the theory of deformation of materials in time have found small use in the practice of calculating engineering structures. However, with the development of energy installations, chemical-technological devices operating at higher temperatures and pressures, the phenomenon of creep is needed. Requests of mechanical engineering led to a huge scope of experimental and theoretical studies in the field of creep. Due to the need for accurate calculations, the phenomenon of creep began to take into account even in such materials as wood and soils,

The study of creep in contact with the contact of solid bodies is important for a number of causes of applied and principled nature. So, even with constant loads, the form of interacting bodies and their intense state, as a rule, it changes, which must be considered when designing machines.

A qualitative explanation of the processes occurring during creep can be given, based on the main representations of the theory of dislocations. So, in the structure of the crystal lattice, various local defects may occur. These defects are called dislocations. They move, interact with each other and cause various types of sliding in the metal. The result of the dislocation movement is shift to one interatomic distance. The intense state of the body facilitates the movement of dislocations, reducing potential barriers.

Temporary laws of creep depends on the structure of the material that changes over the creep. Experimentally obtained an exponential dependence of the speeds of the steady creep against voltages at relatively high voltages (-10 "and more from the modulus of elasticity). In a significant voltage interval, the experimental points on the logarithmic grid are usually grouped at some straight line. This means that in the considered voltage interval (- 10 "-10" from the modulus of elasticity) There is a power dependence of the velocities of strain deformations. It should be noted that at low stresses (10 "and less from the elastic module) this dependence is linear. A number of works are given various experimental data on the mechanical properties of various materials in a wide range of temperatures and deformation rates.

Integral equation and its decision

Note that if the elastic permanent disks and plates are equal, then Wow \u003d O and this equation becomes an integral equation of the first kind. Features of the theory of analytic functions allow in this case using additional conditions, to obtain a single solution. These are the so-called formulas for the treatment of singular integral equations, allowing to obtain a solution to the task explicitly. The peculiarity is that in the theory of boundary value problems, three cases are usually considered (when V is part of the border of the border): the solution has a feature at both ends of the integration region; The solution has a feature at one of the ends of the integration area, and on the second it turns into zero; The solution is drawn to zero at both ends. Depending on the choice of one or another embodiment, a general type of solution is built, which in the first case includes a general solution of a homogeneous equation. Setting the behavior of the solution on infinity and angular points of the contact area, based on physically reasonable assumptions, a single solution is built that satisfies the specified restrictions.

Thus, the uniqueness of the solution of this task is understood in the sense of the restrictions received. It should be noted that when solving contact problems of the theory of elasticity, the most common restrictions are the requirements of circulation to zero solutions at the ends of the contact area and the assumption of the disappearance of stresses and rotations on infinity. In the case when the area of \u200b\u200bintegration is the entire border of the region (body), the uniqueness of the solution is guaranteed by Cauchy formulas. In this case, the easiest and most common method of solving applied tasks in this case is the view of the Cauchy integral in the form of a series.

It should be noted that in the above general information from the theory of singular integral equations, the properties of the contours of the studied regions are not specified, because In this case, it is known that the arc of the circle (the curve along which integration is performed) satisfies the Lyapunov condition. Generalization of the theory of two-dimensional boundary value problems In case of more general assumptions on the smoothness of the boundaries of areas can be found in the monograph of the AI. Danilyuk.

The greatest interest is the total case of the equation, when 7i 0. The absence of methods for constructing an accurate solution in this case leads to the need to apply numerical analysis methods and approximation theory. In fact, as it has already been noted, the numerical methods for solving integral equations are usually based on approximation of solving the equation by the functionality of a certain species. The amount of accumulated results in this area allows you to highlight the main criteria for which these methods are usually compared when using them in applied tasks. First of all, the simplicity of the physical analogy of the proposed approach (usually it is in one form or another method of superposition of a system of certain solutions); the amount of necessary preparatory analytical calculations used to obtain the corresponding system of linear equations; the required size of the system of linear equations to achieve the required accuracy of the solution; The use of a numerical method for solving a system of linear equations that makes the feature of its structure and, accordingly, allowing the numerical result with the highest speed. It should be noted that the last criterion plays an essential role only in the case of large-order linear equations. All this determines the effectiveness of the approach used. At the same time, it should be stated that by now there are only separate studies on comparative analysis and possible simplifications in solving practical problems with the help of various approximations.

It should be noted that the integro-differential equation can be given to the form: V arc of the circumference of a single radius concluded between two points with the angular coordinates -ss0 and a0, a0 є (0, l / 2); U1 is a real coefficient determined by the elastic characteristics of interacting bodies (2.6); F (T) is a known function defined by the applied loads (2.6). In addition, we recall that the STG (T) appeals to zero at the ends of the integration segment.

Relative rapprochement of two parallel circles determined by the deformation of roughness

The task of the internal compression of circular cylinders of close radii was considered first considered by I.Y. Stanman. When solving the problem supplied by it, it is customary that the external load acting on the internal and external cylinders on their surfaces is carried out in the form of a normal pressure, diametrically opposite contact pressure. When the equation is derived, the solution is used to compress the cylinder with two opposite forces and the solution of a similar problem for the appearance of the circular opening in an elastic medium. It was obtained an explicit expression for moving the cylinder loop points and holes through the integral operator from the voltage function. This expression was used by a number of authors to assess the contact stiffness.

Using the heuristic approximation for the distribution of contact stresses for the scheme I.Ya. Stanman, A.B. Milov received simplified dependence for maximum contact movements. However, it was found that the resulting theoretical assessment differs significantly from experimental data. Thus, the movement determined from the experiment turned out to be less theoretical 3 times. This fact is explained by the author of the essential influence of the features of the spatial loading scheme and proposes the transition coefficient from a three-dimensional task to flat.

A similar approach used M.I. Warm, setting the approximate solution somewhat different. It should be noted that in this work, in addition, a linear second-order linear differential equation was obtained to determine the contact movements in the case of the circuit shown in Figure 2.1. The specified equation follows directly from the method of obtaining an integro differential equation to determine normal radial stresses. In this case, the complexity of the right part determines the bulky of the resulting expression for movements. In addition, in this case there are unknown values \u200b\u200bof the coefficients in solving the corresponding homogeneous equation. At the same time, it is noted that without establishing the values \u200b\u200bof permanent, one can determine the amount of radial movements of the diametrically opposite points of the holes and shaft.

Thus, despite the relevance of the task of determining the contact stiffness, the analysis of literary sources did not allow to identify the method of its solution, which makes it possible to reasonably establish the magnitudes of the largest normal contact movements due to the deformation of the surface layers without taking into account the deformations of the interacting bodies as a whole, which is due to the lack of formalized definition of the concept "Contact Stiffness ".

When solving the task, we will proceed from the following definitions: movements under the action of the main vector of forces (excluding the features of contact interaction) will be called closer (removal) of the center of the disk (holes) and its surface that does not lead to a change in the shape of its border. Those. This is the rigidity of the body as a whole. Then the contact stiffness is the maximum movement of the center of the disk (holes) without taking into account the movement of the elastic body under the action of the main vector of forces. This system of concepts allows you to divide the movement; obtained from the solution of the problem of the theory of elasticity, and shows that the assessment of the contact rigidity of cylindrical bodies obtained by A.B. Milovish from Solution Il. Stanman, Verne only for this loading scheme.

Consider the task set in paragraph 2.1. (Figure 2.1) with boundary condition (2.3). Given the properties of analytical functions, from (2.2) we have that:

It is important to emphasize that the first terms (2.30) and (2.32) are determined by the solution of the problem of concentrated strength in the infinite region. This explains the presence of a logarithmic feature. The second terms (2.30), (2.32) are determined by the lack of tangent stresses on the disk circuit and the opening;, as well as the condition for the analytical behavior of the corresponding components of the complex potential in zero and at infinity. On the other hand, superposition (2.26) and (2.29) ((2.27) and (2.31)) gives the zero main vector of forces acting on the contour of the hole (or disk). All this allows you to express through the third term of the radial movement in an arbitrary fixed direction C, in the plate and in the disk. To do this, we find the difference between the FPD (g), (z) and FP 2 (2), 4v2 (z):

Approximate solution of a two-dimensional contact problem of linear creep for smooth cylindrical bodies

The idea of \u200b\u200bthe need to take into account the microstructure of the surface of compressible bodies belongs to I.Ya. Stanman. It was introduced a model of a combined base, according to which in an elastic body, in addition to displacements caused by the action of normal pressure and determined by the solution of the corresponding tasks of the theory of elasticity, additional normal movements arise, due to the purely local deformations, depending on the microstructure of contacting surfaces. I.Y. I.Sterman suggested that additional movement is proportional to normal pressure, and the proportionality coefficient is for this material by constant. As part of this approach, they were first obtained by an equation of a flat contact problem for an elastic rough body, i.e. Body having a layer of high adhesiveness.

In a number of work, it is assumed that additional normal movements due to the deformation of the microprifurizers of contacting bodies are proportional to the macro-strand into some extent. This is based on an equalization of the averaged values \u200b\u200bof movements and stresses within the base length of the surface roughness measurement. However, despite the fairly well developed apparatus of solving problems of a similar class, a number of methodical difficulties are not overcome. So, the hypothesis of the power supply of the stresses and movements of the surface layer, taking into account the real characteristics of microgeometry, is true at small baseline lengths, i.e. The high purity of the surface, and, therefore, with the justice of the hypothesis about the topographic smoothness on micro and macro levels. It should also be noted a significant complication of the equation when using a similar approach and the impossibility of describing with its help of the effect of waviness.

Despite the fairly well-developed device for solving contact problems, taking into account the layer of increased advantage, a number of issues of a methodical nature remained, impede its application in the engineering practice of calculations. As already noted, the surface roughness has a probabilistic height distribution. The commensity of the size of the surface element on which the characteristics of roughness are determined, with the size of the contact area, it is the main difficulty in solving the task and determines the incorrect of applying by some authors of the direct connection between the diameters and the strain of roughness in the form: where S is the surface point.

It should also be noted the solution of the task using the assumption about the transformation of the type of pressure distribution into parabolic, if the deformations of the elastic half-space in comparison with the deformations of the rough layer can be neglected. This approach leads to a significant complication of the integral equation and allows you to receive only numerical results. In addition, the authors have been used by the already mentioned hypothesis (3.1).

It is necessary to mention the attempt to develop an engineering method of accounting for the effect of roughness in the internal touch of cylindrical bodies based on the assumption that elastic radial movements in the contact area caused by the deformation of micro-irregularities are constant and proportional to the average contact voltage T to some extent to. However, Despite its obvious simplicity, the disadvantage of this approach is that with this method of accounting for roughness, its influence gradually increases with an increase in the load, which is not observed in practice (Figure 3 l,).

We carry out all types of student work

Applied theory of contact interaction of elastic bodies and the creation on it is based on the processes of formation of supports of friction-rolling with rational geometry

ThesisHelp in writingFind out the cost my Work

However, the current theory of elastic contact does not sufficiently search for a rational geometric shape of contacting surfaces in a fairly wide range of conditions of work of rolling friction. Experimental search in this area is limited by the complexity of the measuring equipment and experimental equipment used, as well as high labor intensity and durability ...

  • Received conventions
  • CHAPTER 1. Critical analysis of the status of the question, goals and objectives of the work
    • 1. 1. Systemic analysis of the current state and trends in the field of improving the elastic contact of the bodies of complex
      • 1. 1. 1. The current state of the theory of local elastic contact of the bodies of complex shape and optimization of geometric contact parameters
      • 1. 1. 2. The main directions of improving the technology of grinding the working surfaces of the rolling form
      • 1. 1. 3. Modern technology of forming wind superfining surfaces
    • 1. 2. Research tasks
  • Chapter 2. Elastic contact mechanism
  • Complex geometric shape
    • 2. 1. The mechanism of the deformed state of the elastic contact of the bodies of the complex
    • 2. 2. The mechanism of the intense state of the contact area of \u200b\u200bthe elastic bodies of complex shape
    • 2. 3. Analysis of the effect of the geometric shape of contacting bodies on the parameters of their elastic contact
  • findings
  • Chapter 3. Forming a rational geometric shape of parts on grinding operations
    • 3. 1. Forming the geometric shape of rotation parts by grinding by inclined to the axis parts around
    • 3. 2. Algorithm and program for calculating the geometric shape of parts on grinding operations by inclined circle and stress-deformation state of the region of its contact with elastic body in the form of a bowl
    • 3. 3. Analysis of the effect of grinding process parameters by inclined circle on the reference ability of the ground surface
    • 3. 4. Studies of technological capabilities of grinding process by inclined to the axis of the workpiece with grinding circle and the operational properties of bearings made with its use
  • findings
  • Chapter 4. Basics of the formation of parts profile on superfining operations
    • 4. 1. Mathematical model of the mechanism of the process of formation of parts during superfinishing
    • 4. 2. Algorithm and program for calculating the geometric parameters of the treated surface
    • 4. 3. Analysis of the influence of technological factors on the parameters of the process of formation of the surface during superfinishing
  • findings
  • Chapter 5. Results of studying the effectiveness of the process of forming superfine
    • 5. 1. Methods of experimental studies and processing experimental data
    • 5. 2. Regression analysis of the indicators of the process of forming superfinishing depending on the characteristics of the instrument
    • 5. 3. Regression analysis of the indicators of the process of forming superfinishing depending on the processing mode
    • 5. 4. General mathematical model of the process of forming superfine
    • 5. 5. Performance of roller bearings with a rational geometric shape of working surfaces
  • findings
  • Chapter 6. Practical application of research results
    • 6. 1. Improving constructs of supports of friction-rolling
    • 6. 2. Method of grinding rings bearings
    • 6. 3. Method for monitoring the profile track rolling rings of bearings
    • 6. 4. Methods of superfining parts of the type of rings of a complex profile
    • 6. 5. Method for picking bearings with rational geometric shape of working surfaces
  • findings

The cost of unique work

Applied theory of contact interaction of elastic bodies and the creation on its basis the processes of formation of friction-rolling support with rational geometry ( abstract, term, diploma, control)

It is known that the problem of the development of the economy in our country depends largely on the lifting industry based on the use of progressive technology. This provision primarily refers to bearing production, since the activity of other sectors of the national economy depends on the quality of bearings and the effectiveness of their production. Increasing the operational characteristics of rolling friction supports will increase the reliability and resource of machines and mechanisms, the competitiveness of equipment on the world market, which means it is a problem of paramount importance.

A very important direction in improving the quality of rolling friction supports is the technological ensuring the rational geometric shape of their working surfaces: bodies and rolling tracks. In the works of V. M. Alexandrova, O. Yu. Davidenko, A.B. Queen, A.I. Lurie, A.B. Orlova, I.Ya. Staple mana and others. It is convinmed that giving the working surfaces of elastically contacting parts of the mechanisms and machines of a rational geometric shape can significantly improve the parameters of elastic contact and significantly increase the operational properties of friction nodes.

However, the current theory of elastic contact does not sufficiently search for a rational geometric shape of contacting surfaces in a fairly wide range of conditions of work of rolling friction. The experimental search in this area is limited by the complexity of the measuring equipment and experimental equipment used, as well as the high difficulty and duration of research. Therefore, currently there is no universal technique for choosing a rational geometric shape of the contacting surfaces of machine parts and instruments.

A serious problem on the path of practical use of nodes of friction of rolling machines with rational geometry of contact is the lack of effective ways of their manufacture. Modern methods of grinding and adjusting the surfaces of machine parts are designed mainly on the manufacture of surfaces of parts relative to a simple geometric shape, the profiles of which are defined with circular or straight lines. Methods of forming superfining, developed by the Saratov Scientific School, are very effective, but their practical application is designed only for the treatment of external surfaces of the type of rolling track of the internal rollers of roller bearings, which limits their technological capabilities. All this does not allow, for example, to effectively manage the form of a form of contact voltages of a number of rolling friction structures, and therefore, significantly influence their operational properties.

Thus, ensuring a systematic approach to improving the geometric shape of the working surfaces of rolling friction assemblies and its technological support should be considered as one of the most important directions for further improvement of the operational properties of mechanisms and machines. On the one hand, the study of the effect of the geometric shape of the contacting elastic bodies of the complex form on the parameters of their elastic contact allows you to create a universal methodology for improving the design of rolling friction supports. On the other hand, the development of the basics of technological support of the specified form of details ensures effective production of supports of rolling friction mechanism and machines with increased operational properties.

Therefore, the development of the theoretical and technological foundations of improving the parameters of the elastic contact of the details of the rolling friction supports and the creation on this basis of highly efficient technologies and equipment for the production of rolling bearings is a scientific problem that is important for the development of domestic engineering.

The aim of the work is to develop an applied theory of local contact interaction of elastic bodies and the creation of the processes of forming friction-rolling supports with rational geometry, aimed at improving the performance of bearing nodes of various mechanisms and machines.

Methods of research. The work was made on the basis of the fundamental provisions of the theory of elasticity, modern methods of mathematical modeling of the deformed and intense state of locally contacting elastic bodies, modern provisions of mechanical engineering technology, the theory of abrasive processing, theory of probabilities, mathematical statistics, mathematical methods of integral and differential calculation, numerical calculation methods.

Experimental studies were carried out using modern techniques and equipment using experimental planning methods, experimental data processing, and regression analysis, as well as using modern computer software packages.

Accuracy. Theoretical provisions of work are confirmed by the results of experimental studies made in both laboratory and production conditions. The reliability of theoretical provisions and experimental data is confirmed by the introduction of the results of work in production.

Scientific novelty. The paper developed an applied theory of local contact interaction of elastic bodies and created on its basis the processes of formation of friction-rolling supports with rational geometry, opening the possibility of a significant increase in the operational properties of bearing supports and other mechanisms and machines.

The main provisions of the dissertation endowed with the defense:

1. Applied theory of local contact of the elastic bodies of the complex geometric shape, which takes into account the impermanence of the eccentricity of the contact ellipse and the various forms of the initial gap profiles in the main sections described by power dependencies with arbitrary indicators.

2. The results of studies of the intense state in the field of elastic local contact and an analysis of the influence of a complex geometric shape of elastic bodies on the parameters of their local contact.

3. The mechanism of formation of rolling friction supports with a rational geometric shape on the surface grinding operations by inclined to the axis of the workpiece with grinding circle, the results of the analysis of the effect of grinding parameters by the inclined circle on the supporting ability of the grinding surface, the results of the study of the technological capabilities of the grinding process by inclined to the axis of the workpiece grinding circle and operational properties of bearings made with its use.

4. The mechanism of the process of formation of parts during superfining, taking into account the complex kinematics of the process, uneven degree of insolence of the tool, its wear and formation during the processing process, the results of the analysis of the effect of various factors on the process of removal of metal at various points of the profile of the workpiece and forming its surface

5. Regression multifactoric analysis of the technological capabilities of the process of forming superfining parts of bearings on the superfine machines of the latest modifications and operational properties of bearings made using this process.

6. Methods of targeted design of the rational design of the working surfaces of parts of the complex geometric shape of the type of rolling bearings parts, a comprehensive method of manufacturing rolling support parts, which includes preliminary, final processing and control of geometric parameters of work surfaces, the design of new technological equipment created on the basis of new technologies and intended for Production of rolling support parts with rational geometric shape of working surfaces.

The basis for this work includes materials of numerous studies of domestic and foreign authors. The experience and support of a number of specialists of the Saratov Bearing Plant, the Saratov Research and Production Enterprise of non-standard products of Mechanical Engineering, Saratov State Technical University and other organizations contributed to the discussion of this work.

The author considers his duty to express special thanks to valuable advice and multilateral assistance provided in the fulfillment of this work, a deserved figure of science of the Russian Federation, Dr. Technical Sciences, Professor, Academician of Raen Yu. V. Chebotarev and Dr. Technical Sciences, Professor A.M. Cleaner.

The limited amount of work did not allow to give exhaustive answers to a number of affected issues. Some of these issues are more fully reviewed in the published works of the author, as well as in joint work with graduate students and applicants ("https: // Site", 11).

334 Conclusions:

1. The method of targeted design of the rational design of the working surfaces of parts of a complex geometric shape of the type of rolling bearings and as an example, a new design of the ball bearing with a rational geometric shape of rolling tracks was proposed.

2. A comprehensive technology for the manufacture of rolling support parts, which includes the preliminary, final processing, control of the geometric parameters of working surfaces and picking bearings.

3. The designs of the new technological equipment created on the basis of new technologies and intended for the manufacture of parts of rolling supports with a rational geometric shape of work surfaces are proposed.

Conclusion

1. As a result of the research, a system for finding a rational geometric shape of locally contacting elastic bodies and technological bases of their formation, which opens up the prospects for improving the working capacity of a wide class of other mechanisms and machines.

2. A mathematical model has been developed that reveals the mechanism of local contact of the elastic bodies of the complex geometric shape and takes into account the impermanence of the eccentricity of the contact ellipse and various forms of the initial gap profiles in the main sections described by power dependencies with arbitrary indicators. The proposed model summarizes the previously obtained solutions and significantly expands the scope of the practical application of the exact solution of contact tasks.

3. A mathematical model of the intense state of the region of elastic local contact of the body of complex form, showing that the proposed solution of the contact problem gives a fundamentally new result, which opens up a new direction to optimize the contact parameters of the elastic bodies, the nature of the distribution of contact stresses and ensures efficient increase in the performance of the mechanisms of friction and machines.

4. A numerical solution of the local contact of the bodies of the complex form, the algorithm and the program for calculating the deformed and intense state of the contact area, allowing to purposefully design the rational structures of the working surfaces of parts.

5. An analysis of the effect of the geometric form of elastic bodies was performed on the parameters of their local contact, showing that due to changes in the form of bodies, it is possible to simultaneously control the form of the contact stresses, their magnitude and size of the contact site, which allows to provide a high supporting ability of contacting surfaces, and consequently, To a large extent, increase the performance properties of contact surfaces.

6. The technological basis for the manufacture of rolling friction supports with a rational geometric shape on technological operations of grinding and forming superfinishing is developed. These are the most frequently used technological operations in the exact machine-making machine, which ensures the wide practical implementation of the proposed technologies.

7. Developed technology grinding ball supports oblique to the axis of the workpiece with a grinding circle and a mathematical model of shaping of a grinded surface. It is shown that the formed form of the ground surface, in contrast to the traditional form, the arc of the circle has four geometric parameters, which significantly expands the ability to control the reference capacity of the surface being processed.

8. A complex of programs is proposed that ensure the calculation of the geometric parameters of the surfaces of parts obtained by grinding the inclined circle, intense and deformation state of the elastic body in rolling supports with different grinding parameters. An analysis of the effect of grinding parameters by the inclined circle on the supporting ability of the grinded surface is carried out. It is shown that changing the geometric parameters of the grinding process by the inclined circle, especially the angle of inclination, one can significantly redistribute contact voltages and at the same time vary the dimensions of the contact site, which significantly increases the carrying capacity of the contact surface and helps reduce friction on contact. Checking the adequacy of the proposed mathematical model gave positive results.

9. Studies of technological capabilities of grinding process by inclined to the axis of the workpiece with grinding circle and the operational properties of bearings made with its use are carried out. It is shown that the grinding process by the inclined circle contributes to an increase in processing performance compared to conventional grinding, as well as improved the quality of the treated surface. Compared to standard bearings, the durability of bearings made by grinding the inclined circle increases by 2-2.5 times, the waviness decreases by 11 dB, the friction torque decreases by 36%, and the speed spell increases more than twice.

10. A mathematical model of the mechanism of the process of forming parts during superfinishing is developed. In contrast to previous studies in this area, the proposed model provides the ability to determine the removal of the metal at any point of the profile, reflects the process of forming a tool profile during the processing process, a complex mechanism for its insolence and wear.

11. A set of programs that ensure the calculation of the geometric parameters treated with superfinishing of the surface, depending on the main technological factors. An analysis of the influence of various factors on the process of removal of metal at various points of the billet profile and the formation of its surface is performed. As a result of the analysis, it was established that the declaration of the working surface of the tool is determined by the decisive effect on the formation of the billet profile in the superfining process. The adequacy of the proposed model has been performed, which gave positive results.

12. A regression multifactoric analysis of the technological capabilities of the process of forming superfining bearing parts on the superfine machines of the latest modifications and operational properties of bearings made using this process are performed. A mathematical model of the superfining process is constructed, which determines the connection of the main performance indicators and the quality of the processing process from technological factors and which can be used to optimize the process.

13. A method of targeted designing a rational design of working surfaces of parts of a complex geometric shape of the type of rolling bearings and as an example, a new design of the ball bearing with a rational geometric shape of rolling tracks was proposed. A comprehensive technology for the manufacture of rolling support parts, which includes the preliminary, final processing, control of the geometric parameters of the working surfaces and the acquisition of bearings is developed.

14. Designs of new technological equipment created on the basis of new technologies and intended for the manufacture of rolling support parts with a rational geometric shape of working surfaces.

The cost of unique work

List of references

  1. Alexandrov V.M., Pozharsky D. A. Non-classic spatial tasks of mechanics of contact interactions of elastic bodies. M.: Factorial, 1998. - 288c.
  2. Alexandrov V.M., Romanis B. L. Contact tasks in mechanical engineering. M.: Mechanical Engineering, 1986. - 174c.
  3. Alexandrov V.M., Kovalenko E. V. Problems of mechanics of solid media with mixed boundary conditions. M.: Science, 1986. - 334 with
  4. Alexandrov V.M. Some contact tasks for the elastic layer// PMM. 1963. T.27. Vol. 4. P. 758-764.
  5. Alexandrov V.M. Asymptotic methods in the mechanics of contact interactions// Mechanics of contact interactions. -M.: Fizmatlit, 2001. C.10-19.
  6. Amenzade Yu.A. Theory of elasticity. M.: Higher School, 1971.
  7. A.C. № 2 000 916 of the Russian Federation. The method of processing the shaped surfaces of rotation / Korolev A.A., Korolev A.B.// Bi 1993. № 37-38.
  8. A.C. No. 916 268 (USSR), Mich B24 at 35/00. Head for superfine treatment of surfaces of rotation with curvilinear forming /A.V. Korolev, A. Ya. Chihiev // Bul. image 1980. № 7.
  9. A.C. No. 199 593 (USSR), MKI V24N 1/100, 19/06. The method of abrasive processing of the surfaces of rotation / A. V. Korolev // Bul. image 1985. -№ 47.
  10. A.C. 1 141 237 (USSR), MIM 16C 19/06. Rolling bearing / A. V. Korolev // Bul. image 1985. № 7.
  11. A.C. № 1 337 238 (USSR), MKI B24 at 35/00. Purity method / A.B. Korolev, O. Yu. Davidenko, A.G. Marinin // Bul. image 1987. No. 17.
  12. A.C. № 292 755 (USSR), MKI B24 in 19/06. Superfining method with an additional movement of Bruck / S. Radko, A.B. Korolev, A.I.
  13. Sprishevsky // Bul. image 1972.№ 8.
  14. A.C. No. 381 256 (USSR), MKI V24N 1/00, 19/06. The method of final processing of parts / S. G. Radko, A. V. Korolev, M. S. Rod, and others. // Bul. image 1975. No. 10.
  15. A.C. 800 450 (USSR), Mni 16C 33/34. Roller for rolling bearings / E.E.Novikov// Bul. image 1981.№ 4.
  16. A.C. № 598 736 (USSR). The method of finishing the details of the rings of rolling bearings / O. V. Taratynov // Bul. image 1978.№ 11.
  17. A.C. 475 255 (USSR), Mni at 24 V 1 / JU, 35/00. The method of finishing processing of cylindrical surfaces bounded by Burta.B. Grish-Kevich, A.B. Stupin // Bul. image 1982. No. 5.
  18. A.C. 837 773 (USSR), MKI B24 in 1/00, 19/06. The method of superstitising of treadmills of rolling bearings /A.A.Petrov, A. N. Ruzanov // Bul. image 1981.№ 22.
  19. A.C. 880 702 (USSR). Mni B24 in 33/02. Honing head / hard. Cabbage, V. G. Yevtukhov, A.B. Grishkevich // Bul. image 1981. No. 8.
  20. A.C. № 500 964. USSR. Device for electrochemical processing / G. M. Pontiling, M. M. Sarapulkin, Yu. P. Cherepanov, F. P. Kharkov. 1976.
  21. A.C. № 778 982. USSR. A device for regulating an interelectrode gap with dimensional electrochemical processing. / A. D. Kulikov, N. D. Silovanov, F. G. Zaremba, V. A. Bondarenko. 1980.
  22. A.C. № 656 790. USSR. A device for controlling cyclic electrochemical processing / ji. M, Lapiders, Yu. M. Chernyshev. 1979.
  23. A.C. № 250 636. USSR. The method of controlling the process of electrochemical treatment / V. S. Gepstein, V. Yu. Kurochkin, K. G. Nikishin. 1971.
  24. A.C. № 598 725. USSR. The device for the size of electrochemical treatment / Yu. N. Penkov, V. A. Lyskovsky, L. M. Samorukov. 1978.
  25. A.C. № 944 853. USSR. The method of measuring electrochemical treatment / A. E. Martyshkin, 1982.
  26. A.C. № 776 835. USSR. The method of electrochemical treatment / R. G. Nikmatulin. 1980.
  27. A.C. № 211 256. USSR. Cathode device for electrochemical processing / V. I. Egorov, P.E. Imphessman, M. I. Perepetkin et al. 1968.
  28. A.C. № 84 236. USSR. The method of electrifalmal inner grinding / GP. Kersha, A.B. Gushchin. E. V. Ivanitsky, A.B. Remainsman. 1981.
  29. A.C. No. 1 452 214. USSR. The method of electrochemical polishing of spherical tel / A. V. Marchenko, A. P. Morozov. 1987.
  30. A.C. № 859 489. USSR. The method of electrochemical polishing of spherical bodies and a device for its implementation / A. M. Filippenko, V. D. Kadcheev, Yu. S. Kharitonov, A. A. Tspsenkov. 1981.
  31. A.C. USSR № 219,799 CL. 42, 22/03 / Method of measuring the radius of the profile // Grigoriev Yu. L., Nehambin E.L.
  32. A.C. № 876 345. USSR. The method of electrochemical dimensional processing / E. V. Denisov, A. I. Mashyanov, A. E. Denisov. 1981.
  33. A.C. № 814 637. USSR. The method of electrochemical processing / E. K. Lipatov. 1980.
  34. Bathenkov C.B., Sabersky A.C., Cherepakova G. S. The study of the intense state of the elements of the cylindrical roller bearings at the skewers of the rings using photolasticity and holography methods//R.Inz/vnipp. M., 1981. - № 4 (110). P.87-94.
  35. Baselman RD, Tsapkin B. V., Perel L. Ya. Rolling bearings. Directory. M.: Mechanical Engineering, 1967 - 685 s.
  36. Belyaev N.M. Local stresses in compressing elastic bodies// Engineering facilities and construction mechanics. JL: Path, 1924. P. 27-108.
  37. Berezhinsky V.M. Effect of skewing rings of a bombed conical roller bearings on the nature of the contact of the end of the roller with supporting sides//R.Inz/vnipp. M., 1981.-№ 2. C.28-30.
  38. Bilik Sh. M. Macrogeometry details of machines. M.: Mechanical Engineering, 1973.-C.336.
  39. Bochkareva I.I. Study of the process of formation of the convex surface of cylindrical rollers with a non-center supersaturation with longitudinal feed: Dis .. Cand. tehn Sciences: 05.02.08. Saratov, 1974.
  40. Brodsky A.C. On the shape of a grinding and leading circle with a non-center grinding of the convex surface of the rollers with longitudinal feed// Tr. IN-TA / VNIPP. M., 1985. No. 4 (44). - S.78-92.
  41. Brozgol I.M. Influence of finishing the working surfaces of the rings on the level of vibration of bearings// Proceedings of the Institute / VNIPP, - M., 1962.№ 4.C 42-48.
  42. Waitus Yu.M., Maksimova Ji.a., Livshits Z. B., etc. Investigation of the distribution of durability of spherical double-rolled roller bearings when tested for fatigue// Trudy In-Ta / VNIPP. M., 1975. -№ 4 (86). - p.16-19.
  43. Vdovenko V. G. Some issues of efficiency of technological projects of electrochemical processing of parts// Electrochemical dimensional processing of machine parts. Tula: TPI, 1986.
  44. Beniaminov K.N., Vasilevsky C.B. Influence of the finishing operation on the durability of rolling bearings// Title / VNIPP. M., 1989. No. 1. C.3-6.
  45. Visaras R.V., Borisov V. G., and others. On the issue of overhanging rollers in rolling guides/ Izv. universities. Mechanical engineering. 1978. - № 10. p.27-29
  46. . M.: Science, 1974.- 455С.
  47. Vorovich I.I., Aleksandrov V. M., Babesha V. A. Non-classic mixed tasks of the theory of elasticity. M.: Science, 1974. 455 p.
  48. Exhibition. "FRG machines in Moscow" / Sost. N. G. Edelman // Bearing Industry: Scientific and Technology. Ref. Sat M.: NIIAVTOPROM, 1981. MOT. - P. 32-42.
  49. Galanov B.A. The method of bone equations of the type of gammerstein for contact problems of the theory of elasticity in the case of unknown areas of contact// PMM. 1985. T.49. Vol. 5. -C.827-835.
  50. Galakhov MA, Flanman Ya. Sh. Optimal shape of a bombed roller// Vestn. Mechanical engineering. 1986. - № 7. - p.36-37.
  51. Galin Ji.A. Contact tasks of the theory of elasticity. M.: Gostichizdat, 1953, - 264c.
  52. GASTEN V. A. Improving the accuracy of the installation of an interelectrode clearance during cyclic dimensional electrochemical processing: Author. dis. Cand. Tehn Science Tula, 1982
  53. Gebel I.D. and etc. Ultrasonic Superfinishe. L.: LDNTP, 1978.218 p.
  54. Golovachev V. A., Petrov B. I., Filimin V. G., Shmitanev V. A. Electrochemical dimensional processing of components of complex shape. M.: Mechanical Engineering, 1969.
  55. Gordeev A.B. Flexible abrasive tool used in mechanical engineering: Overview Inform. / Branch of TsNII-TEIAVTOSELHOZMASHA.- Tolimatti, 1990. 58c.
  56. Grishkevich A.B., Cabbage V. A., Topors O.A. The method of finishing processing of steel tempered parts// Bulletin of Mechanical Engineering. 1973. № 9 -S.55-57.
  57. Grishkevich A.B., Tsymbal I. P. Design operations of machining. Kharkov: Vice School, 1985. - 141 p.
  58. Davidenko O.Yu., Guskov A.B. Method of bacage finishes with increased versatility and technological flexibility// State and Prospects for the development of GPS Mechanical Processing in the conditions of Hosrat and self-financing: Interunion. Scientific Sat Izhevsk, 1989. -s. thirty.
  59. Davidenko O.Yu., Savin C.B. Multipurpose Superfining Rolling Road Roller Roller Wheel// Finishing machine parts: Interunion. Sat Saratov, 1985. - S.51-54.
  60. {!LANG-b771d46a3c353ed0fe59a5c3dca9056b!}
  61. {!LANG-f7e9bef18e23d63d7e5e65008bb69975!} {!LANG-d9882bc67e848ed1ee2d1f721eba5cf4!}{!LANG-a338fbc8d8a88ad3386fd7234b577a1c!}
  62. {!LANG-2c62edafbb431b902a4c7ff58943ccdb!}
  63. {!LANG-1774f05c179bb8fd3056009eec4afa5a!} {!LANG-230db3198b5fd3698518d0622e20ab5c!}{!LANG-b768db33a2986e155bf5dd26adb2eb3f!}
  64. {!LANG-e83cf299fa2ecc44c92bb907ba3f8ac0!} {!LANG-8656030ef0808d67b3d2dc538051ec52!}{!LANG-e7c508139a1c90f6b7b5bd67e0f96fc6!}
  65. {!LANG-6ce1bf93b75f9f668fb5840fcaed70f5!}
  66. {!LANG-13b20d2446e85f25648bebf34779c3ac!} {!LANG-107581c3b363884c194441b451559e48!}{!LANG-9a335ec0735544b90aa4bf7be3950687!}
  67. {!LANG-0b77d7a300a206d570fec6b608658515!} {!LANG-a6c7aac90c38cd20ceb3a7798ed58589!}{!LANG-fcd6742b9870074432476fc1cf51445a!}
  68. {!LANG-cbb685498ee9f527e0d16fbfe63b16e0!} {!LANG-44bb6fb540b9ab9f63699f507745091e!}{!LANG-e2ed3bb4cd9f1e229f058e0b0822beaa!}
  69. {!LANG-0cf0cd0b3b96786b882d5e465164aadd!} {!LANG-2c5475b7695a114b58241303018e9bb9!}{!LANG-79ed10eb88a11d8fe9e822dc96f51add!}
  70. {!LANG-002ade69002db2ebf5b57e388a37f032!} {!LANG-791e7190a2fb23312258fda102d0ca9e!}{!LANG-fff1d5f0b6460302b5205698042d6cff!}
  71. {!LANG-7167a2c391e27a8220e657d9687dea1e!} {!LANG-d94771f40fa4fb2f39690b214f66f560!}{!LANG-2891f9137678a3f991f6ebd94415ab25!}
  72. {!LANG-ade56423b97c2862cc888e28e6422206!} {!LANG-1a6e4456370eb9ec1727668c84f2a972!}{!LANG-37c668a8af085876e9f00db3f2b3d0a3!}
  73. {!LANG-724d9616815012d92ec0c2ad15f9d41f!} {!LANG-1d191acd096c539728f6d6951f9e8cbd!}{!LANG-822dc12016c8b100eda5120e115d1f52!}
  74. {!LANG-1f90941fd469d552862a24e40858f5b8!} {!LANG-6218ecec4c58851ec1078b09cec20edc!}{!LANG-41392677481cb78bc535c67c0823e4d8!}
  75. {!LANG-dfd887d0dbf7a52f3726dacf62de33e7!} {!LANG-9c4cc0ab0e10310ad05b5dd474d9135d!}{!LANG-8ffed20162ab5d5566a5a4c77fa0befe!}
  76. {!LANG-13db942ae9ba594fd5d4f2c042d6ecf6!}
  77. {!LANG-38b5a4c06909084aaa49f780806d0236!} {!LANG-0e8859302b38c8b2130fa9794c72d040!}{!LANG-2609705777e0c99e3bbc7f433c84f657!}
  78. {!LANG-be00408adfa9fc61797f80ac51665789!} {!LANG-8c10cd9553aad5361b8e8a1f733620af!}{!LANG-bd155af52be25edfaefe4606c385bd88!}
  79. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-b9f12acdcaece12bdd2a27dc3bc0779c!}{!LANG-ca575b2ca317d21bf2633fc38e2bf6e8!}
  80. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-e21374fab0994a9299605a1cae858bf2!}{!LANG-e1cff234b82a4477f2e7d9240af3effd!}
  81. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-82df46769d2be12e9529ddf17e51c9a1!}{!LANG-17e0ce3b1d3cba1aa7a1eb9b3c716cf1!}
  82. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-0a448939d83be0f172d4ec975f6204b0!}{!LANG-7fd5c4c45fa13c372ace3b185f487d8e!}
  83. {!LANG-db5c60fc502eb13769864b16ca26d6f2!}
  84. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-7a5d1cb460345249a12ca8074fccc152!}{!LANG-a28d48828caf962889a850fbe4d68f75!}
  85. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-e7235bdc2fbe9dd09e0cd17bf2fc150d!}{!LANG-cd8e0f4c6238ff911187262788551b10!}
  86. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-c738f4788540388848a8c68ef39a85e5!}{!LANG-dd0c37f6627b8d627afead178721b91b!}
  87. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-27704650c3c4f7b96f221af127c012db!}{!LANG-a4f13886d4c81f92ad57ec2835f404e0!}
  88. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-c4acfa5f05788f62126c46d36afb6b28!}{!LANG-2c92eeb5e75e02cdea968e6eda9e4427!}
  89. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-2a10eaa0845e3d7e917dcfe7217d253f!}{!LANG-e8a0dc77a2e81654e01d405113b26ccd!}
  90. {!LANG-48e4b2111327a0d629a7eaf417033de1!} {!LANG-5370e98fa4f3f4e7213da0f5e46f8af2!}
  91. {!LANG-21f061f11192858f79559166f5fb6032!} {!LANG-cc070b88cb5e3bb33f3cd962e3480d03!}{!LANG-d4c394ed2088f9320d099db97cde0b56!}
  92. {!LANG-1d83266cbe38ce59d432e803503649ca!} {!LANG-fa6899cd4534703d3e3376c82bbb5186!}{!LANG-4835be449706f1f3c64951ada49a4067!}
  93. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-044701efd7404dede265d673a98bf634!}
  94. {!LANG-1d83266cbe38ce59d432e803503649ca!} {!LANG-aca8b15f3c850b5b2e63136e047439ce!}{!LANG-32bc0b0598bd6dd6d69fbde33a12c09d!}
  95. {!LANG-21f061f11192858f79559166f5fb6032!} {!LANG-d24d44c0671e2259cbf51d2eaa562aaa!}{!LANG-32bc0b0598bd6dd6d69fbde33a12c09d!}
  96. {!LANG-f365049bf7c0006befa61d040e8d8e66!} {!LANG-7618195db6da9d92e4df90cb71074ae4!}{!LANG-4c4ed6443895f8bd16776cd98f3f36eb!}
  97. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-6570d8b7607acc83a3f4347d815ae2ab!}{!LANG-ac113f7935a8c01609ce06ed687aafb0!}
  98. {!LANG-d07a042942b61cd79a3ed2c94fc3cf78!}
  99. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-0deaaed45bd20b14bc6798344577d92a!}{!LANG-92edcac4cc3c96aaae1ac61097c2b9b8!}
  100. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-fc8502dbf449e6a5504fc18478fd99ff!}{!LANG-e657fcc98284ee834f0fb93957b91143!}
  101. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-27585dd3f1f36a781ab826fa2b6aae6f!}{!LANG-b844796acc4e840fb5ac67d049d860cb!}
  102. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-c8b6bf93d3c31bb8d2b6b459e0347609!}{!LANG-7c3fe7f169a135eee3177e31c2e18e60!}
  103. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-d339533470d04879359aa98cb04bd705!}
  104. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-cbf608f1c1982b4bd52c6c43f28e6203!}{!LANG-29a0e6a70f10812d9f65bf6dbb4a5fd7!}
  105. {!LANG-d079b634cad2561d1c7de12dbc9543d4!} {!LANG-53ab61c657aa3707553f8b829a9be322!}{!LANG-1605cd3345ca226f8bf69c509bcbc051!}
  106. {!LANG-c1a0d4ce171b37d191540c24eb2628d3!} {!LANG-94a44fab1f197d8f0f79ede6749e82df!}{!LANG-def8c32641efe4b892297d96df7b2b1c!}
  107. {!LANG-f6195a62621d61ddcc3c4be6351b0fff!} {!LANG-8da7b16b5fdbec8eca4eaf495ca49150!}{!LANG-588b3b8c726d9775368c8f036a890104!}
  108. {!LANG-0ed8ac28615b4ec88c4ff71fd0c3e56f!} {!LANG-9a8731b9c6d907fad5c75eef8f015a71!}{!LANG-71e3cb275ca4f063f4312ac2c1acfaf7!}
  109. {!LANG-49f34ccc925f924bbc41663db0f4a408!} {!LANG-70a8bd602b953a89bb4b2dfc8f54267c!}{!LANG-c0794bdca82d7035022852367a719d02!}
  110. {!LANG-49906cfaaf79eac9b542ae05d3ef94e6!} {!LANG-cf587d1f011dbab5924fe4b1a22e386a!}{!LANG-46de7235b60874e89949147b4ad6b287!}
  111. {!LANG-43384470612613f8602ade8da38994dc!} {!LANG-133c58f803e883f74a6ec63aef845f91!}{!LANG-a7429945d05cd292655a1865c5a5cb8f!}
  112. {!LANG-ad881640fa888b1a05d2ec50f46846ef!} {!LANG-74f2ecc265fbaa7b2be0445591ac6920!}{!LANG-9da9d86f30ce7ef058ff63d274f98979!}
  113. {!LANG-49906cfaaf79eac9b542ae05d3ef94e6!} {!LANG-f130374c3f232eeb2294cd48eb8be1db!}{!LANG-3639ac02c42f249ff4ca4c32df624c28!}
  114. {!LANG-49906cfaaf79eac9b542ae05d3ef94e6!} {!LANG-ba50564a0b1bfb82b1e8fdbe25ed5c3f!}{!LANG-eb7a8267bfd4e9269f55e7c475e6e45c!}
  115. {!LANG-cc1560e9d4098ec25a4b09bebae98efb!}
  116. {!LANG-8e958fe13d87bb8c81a64453bb6f454b!} {!LANG-6c4ae2f3b5404c9a7731536e807c06ab!}{!LANG-b7fc59ea328dc280b82d5c3f406c9cd9!}
  117. {!LANG-1a58d035353bd2029ebc2dbe88815654!} {!LANG-5cd600c5642d918a5e39538839190fb9!}{!LANG-426dbf9b508630d580e83bd6a2528783!}
  118. {!LANG-f1045e6783d25b95dc094d61f0fcad72!} {!LANG-a768262b8aa15013b38ddc3f67bb8055!}{!LANG-c927fad2f0af868f66cf198a5b7a12e3!}
  119. {!LANG-967f83a75a2c0e26d17c5a1b461662eb!} {!LANG-364bf23c1bb2f4a679bd862d45d186e9!}{!LANG-e940c9003a7b36b8908a2221f5692b83!}
  120. {!LANG-3f237f6dc0ec8466f01e80eb5dec5fd0!} {!LANG-a5cb5268e67e8b7907fd4fe413486dc6!}{!LANG-84610afeb851c879b907ae3692a06a06!}
  121. {!LANG-3259948ded54d0c9df4268debdf7a356!} {!LANG-73b30dfd6e7b3c75f4a093f7e1cf5765!}{!LANG-067ec31d2384cc2c71e7c3e429bb0ccb!}
  122. {!LANG-b364d7b7c49ba225e0107a21285c59c4!} {!LANG-93c69345eb2c392f91f2ebb879b655b7!}{!LANG-b65ab1466083aca1557d0b05af58d5f8!}
  123. {!LANG-896288f5f652d03386644b8943a39054!} {!LANG-ca606a01c9bf36c13e01c749bda132b3!}{!LANG-4c58b264a159b89255650511c3d2458b!}
  124. {!LANG-7a0bea0ff5fb6d64b0cc4a5ed7ebc9aa!} {!LANG-0c84b44d2e1fd8cfad00ac5b3f03e4bb!}{!LANG-1ed68b8ca0de78a7a63dd328699630ce!}
  125. {!LANG-15386dd25c95e8d4e9c9c72f61d96c8b!} {!LANG-30849369acc0c31c89e803606d3b868a!}{!LANG-851d32953ef02801f257e3c70c4faa14!}
  126. {!LANG-f25634ca3d5e672d2b8771b2f1810392!}{!LANG-5663aa5d52c29ffa9649af643ce9bb88!}
  127. {!LANG-233c959a34a0a4eb40700b8500b9cc7c!} {!LANG-08b9f4ac0c4a6ef698de0c734373eca8!}{!LANG-3661df7c9d45bdb943b4a816130f6a09!}
  128. {!LANG-cee95149da55ff16f985834d6fa05271!} {!LANG-9a4baeb34bb428bebe963826e0b92229!}{!LANG-dabe67a93d807ceaf35094b004d86964!}
  129. {!LANG-cee95149da55ff16f985834d6fa05271!} {!LANG-c20cc052e6dc3326524f83e507ee6aa4!}{!LANG-93b632a6081a08b016c039454e08632e!}
  130. {!LANG-d5bc3334db10b20dca48fab0ce554ee0!} {!LANG-4c29aca8b01e7281b117a8a5ccfe027f!}{!LANG-666b0f6a5f68ea8b6e97496e61bd49bb!}
  131. {!LANG-f68630c29dded94980d890df2a8870e5!} {!LANG-e1be63fe2bac130b3d3c35a4d79627b2!}{!LANG-10ab6e3f4b6d18325e14bc4ea0b94d2a!}
  132. {!LANG-851460ad4abbe0a58f22b6f60b62bd1b!} {!LANG-6d6983578636d32b2993983433bfd6dc!}{!LANG-d2612ea158029536d6e67502c3885c05!}
  133. {!LANG-e434d3128626a9cffaf9f61c563b0ece!} Theory of elasticity{!LANG-73c6f4afa662f9fe28c8e4caee8ee26b!}
  134. {!LANG-4072e018af1c628adeee3fae18797d7b!} {!LANG-5547d5465c51914d48400fd3474683d2!}{!LANG-3a8e87d148af6397d39f72afd4a30477!}
  135. {!LANG-621165b1e47f4d9fcf060cfeb6787fb2!} {!LANG-4b6f0f343428da3b16c1cc2307b13678!}{!LANG-2b0881ab51aa22f35cbe0ce3009c9bc8!}
  136. {!LANG-621165b1e47f4d9fcf060cfeb6787fb2!} {!LANG-2961291ac26a8ce49c57ec935a7b071e!}{!LANG-b4ffbd78ed53f329e6495cfd38302f6c!}
  137. {!LANG-2b28b0fe1923659a30f2ea304f24f3b3!} {!LANG-6251fa82cbe62c297860d077f1e58f56!}{!LANG-c715b2e885fc06ade9a0d60be3b32629!}
  138. {!LANG-2b28b0fe1923659a30f2ea304f24f3b3!} {!LANG-da53f044fc18200d72b059931223800a!}{!LANG-731fc6bae69dfa4e400acb0d6b1f6585!}
  139. {!LANG-5730b36121952b597cf98c3d58843c07!} {!LANG-fd6330076ec4af2b683ea992ab4e0c73!}{!LANG-bc8e303a39b7e790460b4742bc6984db!}
  140. {!LANG-afbe955261e458b64a06bea4ce0a9792!}
  141. {!LANG-2096b763135107217ef08fc5d74b095d!}
  142. {!LANG-5a4c32fcf0f0aad4557c5bbd9c37f19d!} {!LANG-76541b83c9c1a427f97a4b680e67ff0b!}{!LANG-978241dfbc84771cf6aaf642073d76d4!}
  143. {!LANG-d4779a29803e9c090b83c053004a3f67!} {!LANG-bd03176c5acbb69b7adc19ab52ea4315!}{!LANG-2db62ba3b7070f24d129208d20c1f0f7!}
  144. {!LANG-96ad6d15563d2ada400c29018b5fed4c!} {!LANG-79d1833d5ce1d63ff20eff61185f48ec!}{!LANG-204cd36f29fdfd8a89033dc4b65ac7a5!}
  145. {!LANG-2902d3e044c5abee0e821a5229ceeed6!} {!LANG-19b88bc9a9c8f5c1ca19f9ac75ca63a6!}{!LANG-fd4b9b1d1c16d53b7abc3a44644cc5b3!}
  146. {!LANG-376f1a9abb124a8420ff19d6b1025bd0!} {!LANG-e3740f98738e20b06d490d15f9dfc81c!}{!LANG-ac289ab32cae8ac4b415fd9c5655d587!}
  147. {!LANG-afb19a1cb4d27d29a8ff7d42be796bae!} {!LANG-31ed5adf1171e8f0ac9c9199a3f5c6c9!}{!LANG-b66c0fb25306feba0b0a16feb39aa631!}
  148. {!LANG-8f6233d1c0941ff10f11026f6bfe9a2e!} {!LANG-f5b909e9759c0ab197e0f60702117b1f!}{!LANG-de20c18658fd936629a8aa77dc923eae!}
  149. {!LANG-42500b1af8703e917041f5217f04908d!} {!LANG-d238739d735dc78586805c183cc3cd5a!}{!LANG-b5433081ee1f96a4d2536316daa763f1!}
  150. {!LANG-0bd0aa2c2ee71d699859b4f116e2fa9f!} {!LANG-85030f2462e56e1d7cb2b07389e1715e!}{!LANG-dc496b10dbb7c2fa3cd1c5dc518eaa85!}
  151. {!LANG-0ab755fdb78d74c4e7f635fd04fceded!} {!LANG-693c7adf82b36d111c0a2799b974a2ba!}{!LANG-67a57d641bb2a4f0509f39cbec933dcc!}
  152. {!LANG-7d3a4ec8d2b907b5e4977ed05e46e9ce!} {!LANG-6f6998f26aee4a95e8fc1efef0160d3e!}{!LANG-a4810477adb2da09b3deed0bb174b933!}
  153. {!LANG-7d3a4ec8d2b907b5e4977ed05e46e9ce!} {!LANG-508b8fb363157d0e0a0bc06b0f6ff7dc!}{!LANG-1dc6878e2a22a43ad2b233420bb979b6!}
  154. {!LANG-5b28dac50af865acaadb85d2db8a80ea!} {!LANG-b3cf8882c9c4aa59ab25384d5b5da7d7!}{!LANG-9c1c99b494684c34ce8a59f616b42996!}
  155. {!LANG-760b52b9d6c258df99eafa93f25b5d01!} {!LANG-0578fbc87b284800e0c91c1196ec1ee0!}{!LANG-ae96a4d226a1ba4466bd9a6e95fa5858!}
  156. {!LANG-808f12a6b983a6f4437bc3cbb0ee9804!} {!LANG-d18777e783536fed1e36240248ffd7da!}{!LANG-8a945d56fd29a971c42dccc4fab0ddee!}
  157. {!LANG-5a25696d6f3cd7c6f18d4ddc0554743a!} {!LANG-989157254de855bdf5f2b116885ac7d2!}{!LANG-b2dae6bf9ab6cb3f32a739b61f9fe364!}
  158. {!LANG-ecf3d48a1a2a43be1e1e7ab1107d48f6!}
  159. {!LANG-74d4584573049a115fdde6cfefe84e71!}
  160. {!LANG-d177c302d7242f2c7a531e05c177e98b!}
  161. {!LANG-fcfb37bbe6b8e34f1a7ee7fa0389420d!}
  162. {!LANG-484c6983f787566f97cfd4290f62f567!}
  163. {!LANG-18ee521450cb81d14f142e369d91342f!}
  164. {!LANG-83bd3af55aa3f972f20925bffcf1c023!}
  165. {!LANG-63d6d1049ea64d46b9dee8a5bc8686d9!}
  166. {!LANG-6b3df8d2812278ce20f97164dc707f94!}
  167. {!LANG-264a1a1d114f6dbfa47a51cc119308c2!}
  168. {!LANG-c12fad6472a849c473410c410af2e7ad!}
  169. {!LANG-d41c88d74dade1b3a4380262ba221b93!}
  170. {!LANG-cd46872b3355fec29134c7c4915a447d!}
  171. {!LANG-81c3dc252370c6d3f9bdd7edf0fcc86e!}
  172. {!LANG-9d2089436b44cb81db64409c14e76b62!}
  173. {!LANG-cf14f042198a35287f872cde9a147927!}
  174. {!LANG-97a06acec22364d7f8f63ef2cde35a27!}
  175. {!LANG-269a3cbf6b341a442adf6c44bd512bff!}
  176. {!LANG-f5a5d9356809459732d6f1b37e023c5b!}
  177. {!LANG-7d1436c18cf82901de9adc2114c3e289!}
  178. {!LANG-4b00646f12d9fe07df7d6bf53fc26776!}
  179. {!LANG-fbf427feeb8faa0f6b9862a6dea1bbd0!}
  180. {!LANG-bd0f0e269ec53133a296d5be06b882f9!}
  181. {!LANG-477c22acbccbb498a440a92b7106be14!}
  182. {!LANG-311910e0d4058a115cba04eacfeafa5b!}
  183. {!LANG-b430bfdd172bdb024f4c58234792b3a6!} {!LANG-ccce29bbe1557fd552832632b66dab61!}{!LANG-0d5edeb3f1118c76c1047295f2e88fc1!}
  184. {!LANG-364df396ac080bef149b27254d7b7810!} {!LANG-76a1d4d5daea6b9489866dc4d6d3468b!}{!LANG-debdf2bc5d2b9459ba43431436c155f3!}
  185. {!LANG-cf4e84ec648c270a1b2fa2ff6363a38b!} {!LANG-33e80b7546a0d2101481e82dd93f5a52!}{!LANG-20fbdbd843d2540c3392d828656a1def!}
  186. {!LANG-ff47d9c0340726589fc8dd21b44a40f9!} {!LANG-06ae909a6c6dea67aa8239307e51e0ba!}{!LANG-84df2681aa9acc8423fbdb8da0ad0a53!}
  187. {!LANG-fc0dbcceb1fc2f190dd9345dfd3c524c!} {!LANG-28a7857f0ec72bef8cea7ef01f88c4e5!}{!LANG-12697b0f69e72e6e144df590fc67b985!}
  188. {!LANG-6e51f8c837d60215705ff330fc502c98!} {!LANG-c7e48c435a5eb4afa5f73f42cd2f7680!}{!LANG-75a25e796f8ed69c59215b02b8231ad4!}
  189. {!LANG-ee06f3cd04a3063e40e18eaab580fc61!}
  190. {!LANG-7f88801166347e3da1bbfb2362c70463!} {!LANG-0d3c62a2308c8c1382f5ec57c90ddb47!}{!LANG-4d806f6cf118bb127540aabeca1291f3!}
  191. {!LANG-144ea2cb765aa017c4db4ce262443bee!}
  192. {!LANG-249994901dcc74a37832bd2e97e3551e!} {!LANG-2c22c0f7bb0af9740a437fbabf5735b3!}{!LANG-43c774c3df2827451ee8651fe910835b!}
  193. {!LANG-8fa42bd2c52a4c98baaf680043938045!} {!LANG-46c9f65fd76626e4dd4380f7c56e106b!}{!LANG-4c4af3cbeedb7b895946135e957d9871!}
  194. {!LANG-404de695e26e9d1c42c1cb83a444b51c!} {!LANG-9b09b6e14d4720e8cc857addb237b7b0!}{!LANG-f9be2cf3792b41ebe0da834cec8132dd!}
  195. {!LANG-404de695e26e9d1c42c1cb83a444b51c!} {!LANG-f49dc436627b4748e23003f23d51860a!}{!LANG-7eabd279e627b40f94fda1e35b776ab4!}
  196. {!LANG-404de695e26e9d1c42c1cb83a444b51c!} {!LANG-2d2ad328bf4890ec9b34c67d6b2fe529!}{!LANG-3caccbd442d48ea939d70df11925ef91!}
  197. {!LANG-df736e2e590902a23b6a3dbecc392122!} {!LANG-0bbffddb6f75f6a424d264528ae21223!}{!LANG-ee8f564308d617cbad88f02297052a25!}
  198. {!LANG-d07e705cbfffe937a2fee91e4c769c3a!} {!LANG-f28179704603a57509fa05ab1f19a32b!}{!LANG-22554cf853f3eb477de64f7d107872ac!}
  199. {!LANG-3f70c3e248c8b37cede1e38e5af2e2e6!} {!LANG-a01c13709ba326214707de48ed8733f2!}{!LANG-99fe480f07ee38177f5ac9958674abf8!}
  200. {!LANG-5db994ff24c205235edd5e13d54f7634!}
  201. {!LANG-89c91375c8c04560e71827897f0c0717!} {!LANG-cd741dbee23c4ea280fbc0018131b9b4!}{!LANG-f9c8efe403a9be30bd74b03ea6411291!}
  202. {!LANG-e80dc5512c047905e29a78c7f794c1af!} {!LANG-3624418ee7019d18fdb898b3ad9fa2d9!}{!LANG-cdf766665df45e8a2ab8a1bbad6bf35c!}
  203. {!LANG-c842bc9d73d6604239cc7ad4557913eb!}
  204. {!LANG-281bfe15c0998e3e4c2ad5dd6249f58c!} {!LANG-3cffca8c7c5635938b65fd6ca28a53a0!}{!LANG-ac90811cc64251856afce0680c194e44!}
  205. {!LANG-e297a6675f196b0675a7350e0e6faa7d!} {!LANG-3a59c5ec92a4c21d969e5d8f548cde7c!}{!LANG-e21571a05028934ef26a5c53497b2719!}
  206. {!LANG-61b29c548a167a270055a4dd57157574!} {!LANG-0bd3f8424df17d103b39e2f2599f3398!}{!LANG-5441fdf063c5dea1c0f8bd31977d32b9!}
  207. {!LANG-09d7318b9ec79558d58b07a899e2b70a!} {!LANG-78e3846e2b3378d5f11d65d313cbcb63!}{!LANG-d9540734cda6b32e8ec87f64f46c6efc!}
  208. {!LANG-93626932c314281c676d53caa87049c4!}
  209. {!LANG-f930a0dea26bb2ee13100e20be126bed!} Rolling bearings{!LANG-57a5ddfa1af4910948873124820194e5!}
  210. {!LANG-0906f76775afa3e1030a9b33d52f671a!} {!LANG-a784c07b755638a53c33a2511fdaaa85!}{!LANG-554a9699abe94122bfc5e7863ecc0b16!}
  211. {!LANG-858ddd38fcfe4266fefc9de43946021f!} Theory of elasticity{!LANG-10f394c1f5295dff90f097ad82d35cdc!}
  212. {!LANG-2d6273f9e076654835d1519934ba743b!} {!LANG-02ea80a5375dea9766c59b8dff88fbfb!}{!LANG-de7c8b32c8f24b3cca783d3e8358a6d4!}
  213. {!LANG-85f71de6f58382f1b1658d9205e26df4!} {!LANG-44e60333004c378a8711bd8e682c9d0b!}{!LANG-82c4512ce47e6a8384f05091bdc1aa19!}
  214. {!LANG-585c3288fe39e077ad1b2d6e5ba74947!} {!LANG-e4738a73dba00d953ad5e31bfbb04851!}{!LANG-c9d384055f45db31c700e21cc4a33a48!}
  215. {!LANG-a9693d5e3156b744f90b556b6b7605b2!} {!LANG-07aa1f16b09cbe294002e111fd759f0b!}{!LANG-ea5570bcc2a31307a8765a1ef3dfa539!}
  216. {!LANG-0ac20884ec8f95c44aa519c5827fc2c7!} {!LANG-0cbf2dbfd5e9431a93c4b79239b8039b!}{!LANG-f97df334f77fe407ab43a21ec449dcd0!}
  217. {!LANG-11ae952e6663379fceb953b3394b4ff4!} {!LANG-e3abad9e4ce39f3f2845824b980100df!}{!LANG-e6b3a6264bc6ccaeae46196d1c10acf5!}
  218. {!LANG-d1705539dfe6f40d3afb8f818e9fc9d3!} {!LANG-1cdd41f48463c5c84455cadb7fd6e227!}{!LANG-b4fc905b21fb399cb568984ee6c719a1!}
  219. {!LANG-c847dba68b2c96939c676538ac6dec5c!} {!LANG-d2575c4d167bb7a97ac60c32aaace2a9!}{!LANG-aba8232980e943c7c93722f13b7baac8!}
  220. {!LANG-d1705539dfe6f40d3afb8f818e9fc9d3!} {!LANG-f694c0dec385b71d9527fa66fb1c3d8d!}{!LANG-eaeb372ce3394ccd752688400ec34177!}
  221. {!LANG-28e7771a8eda2f236c5d0fbf0011c94f!} {!LANG-7bfff4d8d6bab0761e1d00cbe45bf118!}{!LANG-df1c91cceb5035cedac4ce3554832147!}
  222. {!LANG-2ec7aa53b84c170fcd71649251ae42c9!} {!LANG-d9331773d58fb78bec7ad5a766f2adf1!}{!LANG-8479f8e2b2af0c04465ff8f89b1f2461!}
  223. {!LANG-4461559305d6c216e1c950d7783b2ea5!} {!LANG-4fbc428b10a3a20fc78ee6386ab23681!}{!LANG-e5ff184f619eb4924171b784b3356d82!}
  224. {!LANG-11b36c28f1a33e7ece603ac7922f6095!} {!LANG-f024aac582567a86dfb0f210f29f1468!}{!LANG-a082c124e75b6ff1557d8b452884f702!}
  225. {!LANG-4ad998a221ff8b264cf0520793d29f23!} {!LANG-fc9813fca4ef0c0e663a43e98c1e0361!}{!LANG-4365aaa52983fbdec6d25e366a8aada1!}
  226. {!LANG-c97896b939ffcf34a6618f436c18d3eb!} {!LANG-4953a5627f14207e9378b4658d4344c5!}{!LANG-f4f6747c8a42194cb8380505107eab04!}
  227. {!LANG-65a1d30d661c17dafdab2dc2cf37d9e7!}
  228. {!LANG-0e8d45acb5e1cecc89e82ef656a2b3ad!}
  229. {!LANG-e94ca631fedbd092126f3c4ac46e0ad4!}
  230. {!LANG-4f022b909571bf9633f6adf0a627fc9c!}
  231. {!LANG-eb865600adf290061914bb2ef4fa99a0!}

{!LANG-3333e6b1e9331384b91ff9c440fa1f35!}

{!LANG-c39a297b6426c8a2ab9ebaee59a436dd!}

{!LANG-575e1679cfd788b010688fa20dc027ed!}

{!LANG-7169a3cf8efc26413829070072f12e63!}

Introduction

{!LANG-02cc72fe65a5692c8a71907d70d8d078!}

{!LANG-ed2860824795b6589f9ffb64181d0555!}

{!LANG-027e8bbcef8639e7df848a9109bae14f!}

{!LANG-509d179d935d3cb70902a225cbb11660!}

{!LANG-16d4c8774e35afee7aec9c1050dd940d!}

{!LANG-620284c74ff00448bbd5f5d523119a32!}

{!LANG-85c0e1f9b4fcc70993f5a267b0a5527b!}

{!LANG-28d49babcbccbf754e21c4defaa7e74a!}

{!LANG-58ce8e692710dbf05a4ca1ca027b5644!}

{!LANG-755382d994f2e77f14cf78f42b859df5!}

{!LANG-553ca440930342d4801c040144b58e38!}

{!LANG-659d620bead85c9cf91226e89f4ce946!}

{!LANG-64b85eeb3ce7875199e39979f7653dba!}

{!LANG-e4e71f8f6a7843731844596e3c8acfec!}

{!LANG-87b30893d2bee7b205241f41cab66503!}

{!LANG-e01f057d2766622ca30ba55f1a62f190!}

{!LANG-43b4cdc2a9237454ce874de36647908b!}

{!LANG-14af96df09d04c59474af0aa3864edc9!}

{!LANG-be6cebe86ae7f8f8923a0e5285648a26!}

{!LANG-d4491bb7e9a625baa30398b44962f652!}

{!LANG-c5d4161433ccdceff080f42afa902a30!}

{!LANG-7c278c8bf7382b42fb34b279a75d4069!}

{!LANG-5945e963e635c56c20acdedcc3f8205a!}

{!LANG-bd7b52291ef1b18ab2ffe4d387dcb3b3!}

{!LANG-502f943833735d46d3366055ae8a5f4c!}

{!LANG-f7d19b036f5ec032460a002c82bcc494!}

{!LANG-bd10c1035255054b254930aa69e1e115!}

{!LANG-46a54d1656f0a7cd3291f0c24141fb88!}

{!LANG-418bba97612e1109cd84acb32c1d1543!}

{!LANG-9ba7cdfb8e6780473538748aa51b19d4!}

{!LANG-ebe48672cb4f214cd8d9168fe2f716c2!}

{!LANG-46e71d047df2675840a8e33b23b80fd5!}

{!LANG-6595ee4fb56e8a6d49406c14484bf060!}

{!LANG-c035b5c27af5cb1608ba3f48d97e1cc6!}<2/3 поверхность при контакте деформируется только упруго. Величина ш была введена Гринвудом и Вильямсоном и носит название индекса пластичности.

{!LANG-d6e0fc9515531707aa77b00926b3cdad!}

{!LANG-49673824e3d3826a53aacd1a7ff4958f!}

{!LANG-ecc7be054767c82678526f1b222f7228!}

{!LANG-75406d124cd645c4dc39d9a9b6355c2a!}

{!LANG-544a40ddee47eefa60f184398ba62fdb!}

{!LANG-18970e6f99ca8e5483399b21936e7354!}

{!LANG-cb3d89c6e7311b5e850a892128b05687!}

{!LANG-7df7424a3cdad3f02e3e6dc68ca46515!}

{!LANG-a75d8aa0e3ce988d2f980159f3e163fa!}

{!LANG-5b0ca25d007bb9ae711e76abd047d147!}

{!LANG-2e98ee74387d4904b2f3d47e3de930b3!}

{!LANG-50a0cc32f8168827a1aa51c2fc90eb79!}

{!LANG-0fdef4cbe2d5fd4f20294387fadc11e7!}

{!LANG-cb43c0e048fbf67e9726452f097806e3!}

{!LANG-977c8dacb9e33caccc73d7c4c284daff!}

{!LANG-0378a49f03b22f9febe10606a2909ad3!}

{!LANG-52e9edb4bd35d8ced746c9c5a2860da6!}

{!LANG-06b4ca66b737c85edcecb2c96e74d678!}

{!LANG-1565d7b0dae657fe2cd6c3a859dd32d6!}

{!LANG-22169a77ec379f442a4f25f7db988c15!}

{!LANG-92cf8d2698df14d7daacbe12dbdb05dc!}

{!LANG-0ee29743971e58ab817ce9c46f9690ba!}

{!LANG-df2d0094357ae0d1ee6d0796ca839332!}

{!LANG-4c87171f3fa606547f04f72fa2bf0196!}

{!LANG-904c749a4c4b0e35353500d979dabaa2!}< D < 2) является величиной постоянной, можно сделать вывод о том, что радиус контурной площади контакта зависит только от площади отдельной максимально деформированной неровности.

{!LANG-003aa9a21a6136667bd37dfd77e37cea!}

{!LANG-dac742421037759a68db6cab93379d32!}

{!LANG-0e27ad4d0850a14c3f470703d753394d!}

{!LANG-89b8e5ab09ee0837b7a199287a9e1e04!}

{!LANG-93f5be199b4c3f6ff33550e2d228217e!}

{!LANG-09a89237d0631ed9de5162387ddd15cb!}

{!LANG-3ef3eb226367468449560bcb35e3ba96!}

{!LANG-83ee0762955a8cec3885787491870a13!}

{!LANG-afe60bb14c37ee4913b0ffe4f781d40f!}

{!LANG-a8ddaefa329d75fe19d7daa0d4bd7278!}

{!LANG-53470576564813e3ec716280817fc0df!}

{!LANG-c2e2618f9b3f15e0c1527eaa4c2c3967!}

{!LANG-e8e9584bac634f701361cc012ef3633a!}

{!LANG-d2d466add070b018451dafd3dd690c08!}

{!LANG-c9d0a9ad94b3b86daf435bf201d6b20e!}

{!LANG-14cb4b78e925bb579b80a9f8a25bd6e5!}

{!LANG-e455d6634a31645a313b8fd1a86805d6!}

{!LANG-96c50a08cf334a9a2725863a9bf64039!}

{!LANG-49c6faad5caf3cb75330002fbdca4a57!}

{!LANG-8785ea050e47bc9019abab6135843e77!}

{!LANG-b3d2148beecdac61f856748121589616!}

{!LANG-a8536d071b4be63803e788dea2fa65a0!}

{!LANG-c7f854fea6c21689d3d703e13c2cd264!}

{!LANG-cee57f025e1ea0d024a93a6b8df15e9a!}

{!LANG-5954baeb629fad48df7b877b2dc2d741!}

{!LANG-02bdade65ac072d4eb469289e3fe1ef0!}

{!LANG-b5d3ad1e4505abf0d70c9d18eea8145a!}

{!LANG-8bd19cf39703ff2b1072d4efa5786e0a!}

{!LANG-024c709fb6b9d434a747a11194047ce7!}

{!LANG-8bd19cf39703ff2b1072d4efa5786e0a!}

{!LANG-024c709fb6b9d434a747a11194047ce7!}

{!LANG-f3127fefebd62d8e4aa0c38537c61501!}

{!LANG-d52e59872960c2f9e52c6a0d185885e6!}

{!LANG-906dd548c6199053c195fea2857dbbf1!}

{!LANG-66d0375cd6e22d447f52c36e216cdd23!}

{!LANG-c06a8299f108d6920747786ff20981fe!}

{!LANG-179ad890f26425bad2dcafef875f2a53!}

{!LANG-b0c5b4e3ff9448a0d3c936eb31bef01c!}

{!LANG-dd3bd048a01cabe0f304c77b668584c6!}

{!LANG-d63c20d1c4f172003ed3d9f3e42c1c10!}

{!LANG-3874d8d69b75c424b628503628255c29!}

{!LANG-372ddc28a02c8894fe7fe71967691cf9!}

{!LANG-9447e9f881e929afca1e407a75607db5!}

List of references

{!LANG-9b3d9401a8fc8ac67c6aaeee2ab12254!}

{!LANG-2067ec889c63ca34b04e95bb6aef328d!}

{!LANG-32782eb14234f4a30d7abab0fa3c1fa9!}

{!LANG-b1f093ca1c194809ee5e1bc50ad71e86!}

{!LANG-72716188edb3de39534549e6f4240b53!}

{!LANG-4f110b9f1a58200b83615a3b2e6b33e7!}

{!LANG-7f3659813e97e04aae477e1260905833!}

{!LANG-387bd29d86cc300115ef30ba67bac60d!}

{!LANG-992b99f6364e220c2cf93725cba1df8e!}

{!LANG-79abc143f0e3e2a11c8c60c8fc411b2f!}

{!LANG-e4589413a8a7be043b56925a5fed83b1!}

{!LANG-2315defc5e8fbf7be03badaab0f522f9!}

    {!LANG-75f9395979bf48b939a3898c22d68775!}

    {!LANG-f61076c11e05411ef750f3613c0331f5!}

    {!LANG-cae248f999b5ff0c4c18ee40fa9877c0!}

    {!LANG-ebea6362d78d7ff1dec12be24b4e3d5d!}

    {!LANG-84ed84132e07203224cbdd825c3f5163!}

    {!LANG-65ed3e5e9ac6547269946c6b16a4ce6b!}

    {!LANG-3716ce2c7e0692981396409d2cec30e7!}

    {!LANG-aeefd390a20d220a9c8aa7b56b03f2ed!}

    {!LANG-23cc18c701e89b9d773a5c3261f1b9b6!}

    {!LANG-0ab1c57ade59b64b2ccf96fec4326364!}

    {!LANG-06364a927c74d6b9baab4f3c3e19933f!}

    {!LANG-a88d3dff287eac44b23ec3adf81f6fb6!}

    {!LANG-cb39f5a3dda56ad96aa415b53eacb3b0!}

    {!LANG-7f3dc8bf40ba4c22f2d33095510e4ad5!}

    {!LANG-219da9a0a25d8c115c966f022a9c6bb7!}

    {!LANG-e7ad7f6d935bda7a16b580faaee78931!}

    {!LANG-37dd799d24fdcc682e64089605ceafd6!}

    {!LANG-38476d10a7306bec3f3e14c8ba6362ea!}