Contact mechanics Contact mechanics is the study of the deformation of solids that touch each other at one or more points.Johnson, K. L, 1985, Contact mechanics, Cambridge University Press.Popov, Valentin L., 2010, ''Contact Mechanics and Friction. Physical P ...

is the study of the deformation of

solids Solid is one of the four fundamental states of matter (the others being liquid, gas, and plasma). The molecules in a solid are closely packed together and contain the least amount of kinetic energy. A solid is characterized by structural ...

that touch each other at one or more points. This can be divided into compressive and adhesive forces in the direction perpendicular to the interface, and

friction Friction is the force resisting the relative motion of solid surfaces, fluid layers, and material elements sliding against each other. There are several types of friction: *Dry friction is a force that opposes the relative lateral motion of ...

al forces in the tangential direction. Frictional contact mechanics is the study of the deformation of bodies in the presence of frictional effects, whereas '' frictionless contact mechanics'' assumes the absence of such effects. Frictional contact mechanics is concerned with a large range of different scales. * At the macroscopic scale, it is applied for the investigation of the motion of contacting bodies (see

Contact dynamics Contact dynamics deals with the motion of multibody systems subjected to unilateral contacts and friction. Such systems are omnipresent in many multibody dynamics applications. Consider for example * Contacts between wheels and ground in vehicle ...

). For instance the bouncing of a rubber ball on a surface depends on the frictional interaction at the contact interface. Here the total force versus indentation and lateral displacement are of main concern. * At the intermediate scale, one is interested in the local stresses, strains and deformations of the contacting bodies in and near the contact area. For instance to derive or validate contact models at the macroscopic scale, or to investigate

wear Wear is the damaging, gradual removal or deformation of material at solid surfaces. Causes of wear can be mechanical (e.g., erosion) or chemical (e.g., corrosion). The study of wear and related processes is referred to as tribology. Wear in ...

and

damage Damage is any change in a thing, often a physical object, that degrades it away from its initial state. It can broadly be defined as "changes introduced into a system that adversely affect its current or future performance".Farrar, C.R., Sohn, H., ...

of the contacting bodies' surfaces. Application areas of this scale are tire-pavement interaction, railway wheel-rail interaction, roller bearing analysis, etc. * Finally, at the microscopic and nano-scales, contact mechanics is used to increase our understanding of tribological systems (e.g., investigate the origin of

) and for the engineering of advanced devices like

atomic force microscope Atomic force microscopy (AFM) or scanning force microscopy (SFM) is a very-high-resolution type of scanning probe microscopy (SPM), with demonstrated resolution on the order of fractions of a nanometer, more than 1000 times better than the op ...

s and

MEMS Microelectromechanical systems (MEMS), also written as micro-electro-mechanical systems (or microelectronic and microelectromechanical systems) and the related micromechatronics and microsystems constitute the technology of microscopic devices, ...

devices. This page is mainly concerned with the second scale: getting basic insight in the stresses and deformations in and near the contact patch, without paying too much attention to the detailed mechanisms by which they come about.

History

Several famous scientists, engineers and mathematicians contributed to our understanding of friction. They include

Leonardo da Vinci Leonardo di ser Piero da Vinci (15 April 14522 May 1519) was an Italian polymath of the High Renaissance who was active as a painter, draughtsman, engineer, scientist, theorist, sculptor, and architect. While his fame initially rested on ...

Guillaume Amontons Guillaume Amontons (31 August 1663 – 11 October 1705) was a French scientific instrument inventor and physicist. He was one of the pioneers in studying the problem of friction, which is the resistance to motion when bodies make contact. He is ...

John Theophilus Desaguliers John Theophilus Desaguliers FRS (12 March 1683 – 29 February 1744) was a British natural philosopher, clergyman, engineer and freemason who was elected to the Royal Society in 1714 as experimental assistant to Isaac Newton. He had studied at ...

Leonhard Euler Leonhard Euler ( , ; 15 April 170718 September 1783) was a Swiss mathematician, physicist, astronomer, geographer, logician and engineer who founded the studies of graph theory and topology and made pioneering and influential discoveries ...

, and

Charles-Augustin de Coulomb Charles-Augustin de Coulomb (; ; 14 June 1736 – 23 August 1806) was a French officer, engineer, and physicist. He is best known as the eponymous discoverer of what is now called Coulomb's law, the description of the electrostatic force of attra ...

. Later, Nikolai Pavlovich Petrov,

Osborne Reynolds Osborne Reynolds (23 August 1842 – 21 February 1912) was an Irish-born innovator in the understanding of fluid dynamics. Separately, his studies of heat transfer between solids and fluids brought improvements in boiler and condenser design. ...

and

Richard Stribeck Richard Stribeck (7. July 1861 in Stuttgart , † 29. March 1950) was a German engineer, after whom the Stribeck Curve is named. Life Stribeck studied mechanical engineering in 1880 at the Technical University of Stuttgart in 1885 and worked as a ...

supplemented this understanding with theories of

lubrication Lubrication is the process or technique of using a lubricant to reduce friction and wear and tear in a contact between two surfaces. The study of lubrication is a discipline in the field of tribology. Lubrication mechanisms such as fluid-lubric ...

. Deformation of solid materials was investigated in the 17th and 18th centuries by

Robert Hooke Robert Hooke FRS (; 18 July 16353 March 1703) was an English polymath active as a scientist, natural philosopher and architect, who is credited to be one of two scientists to discover microorganisms in 1665 using a compound microscope that ...

Joseph Louis Lagrange Joseph-Louis Lagrange (born Giuseppe Luigi Lagrangiad’Alembert and Timoshenko. With respect to contact mechanics the classical contribution by

Heinrich Hertz Heinrich Rudolf Hertz ( ; ; 22 February 1857 – 1 January 1894) was a German physicist who first conclusively proved the existence of the electromagnetic waves predicted by James Clerk Maxwell's equations of electromagnetism. The uni ...

stands out. Further the fundamental solutions by Boussinesq and Cerruti are of primary importance for the investigation of frictional contact problems in the (linearly) elastic regime. Illustration of creepage for a railway wheel

Illustration of creepage for a railway wheel

Classical results for a true frictional contact problem concern the papers by F.W. Carter (1926) and H. Fromm (1927). They independently presented the creep versus creep force relation for a cylinder on a plane or for two cylinders in steady rolling contact using Coulomb’s dry friction law (see below). These are applied to railway locomotive traction, and for understanding the

hunting oscillation Hunting oscillation is a self-oscillation, usually unwanted, about an equilibrium. The expression came into use in the 19th century and describes how a system "hunts" for equilibrium. The expression is used to describe phenomena in such diverse ...

of railway vehicles. With respect to sliding, the classical solutions are due to C. Cattaneo (1938) and R.D. Mindlin (1949), who considered the tangential shifting of a sphere on a plane (see below). In the 1950s, interest in the rolling contact of railway wheels grew. In 1958, Kenneth L. Johnson presented an approximate approach for the 3D frictional problem with Hertzian geometry, with either lateral or spin creepage. Among others he found that spin creepage, which is symmetric about the center of the contact patch, leads to a net lateral force in rolling conditions. This is due to the fore-aft differences in the distribution of tractions in the contact patch. In 1967, Joost Jacques Kalker published his milestone PhD thesis on the linear theory for rolling contact. This theory is exact for the situation of an infinite friction coefficient in which case the slip area vanishes, and is approximative for non-vanishing creepages. It does assume Coulomb's friction law, which more or less requires (scrupulously) clean surfaces. This theory is for massive bodies such as the railway wheel-rail contact. With respect to road-tire interaction, an important contribution concerns the so-called magic tire formula by

Hans Pacejka Hans Bastiaan Pacejka (12 September 1934 – 17 September 2017) was an expert in vehicle system dynamics and particularly in tire dynamics, fields in which his works are now standard references. He was Professor emeritus at Delft University of Tec ...

. In the 1970s, many numerical models were devised. Particularly variational approaches, such as those relying on Duvaut and Lion’s existence and uniqueness theories. Over time, these grew into finite element approaches for contact problems with general material models and geometries, and into half-space based approaches for so-called smooth-edged contact problems for linearly elastic materials. Models of the first category were presented by LaursenLaursen, T.A., 2002, ''Computational Contact and Impact Mechanics, Fundamentals of Modeling Interfacial Phenomena in Nonlinear Finite Element Analysis'', Springer, Berlin and by Wriggers.Wriggers, P., 2006, ''Computational Contact Mechanics, 2nd ed.'', Springer, Heidelberg An example of the latter category is Kalker’s CONTACT model. A drawback of the well-founded variational approaches is their large computation times. Therefore, many different approximate approaches were devised as well. Several well-known approximate theories for the rolling contact problem are Kalker’s FASTSIM approach, the Shen-Hedrick-Elkins formula, and Polach’s approach. More information on the history of the wheel/rail contact problem is provided in Knothe's paper. Further Johnson collected in his book a tremendous amount of information on contact mechanics and related subjects. With respect to rolling contact mechanics an overview of various theories is presented by Kalker as well. Finally the proceedings of a CISM course are of interest, which provide an introduction to more advanced aspects of rolling contact theory.

Problem formulation

Central in the analysis of frictional contact problems is the understanding that the stresses at the surface of each body are spatially varying. Consequently, the strains and deformations of the bodies are varying with position too. And the motion of particles of the contacting bodies can be different at different locations: in part of the contact patch particles of the opposing bodies may adhere (stick) to each other, whereas in other parts of the contact patch relative movement occurs. This local relative sliding is called micro- slip. This subdivision of the contact area into stick (adhesion) and slip areas manifests itself a.o. in fretting wear. Note that

occurs only where

power Power most often refers to: * Power (physics), meaning "rate of doing work" ** Engine power, the power put out by an engine ** Electric power * Power (social and political), the ability to influence people or events ** Abusive power Power may a ...

is dissipated, which requires stress and local relative displacement (slip) between the two surfaces. The size and shape of the contact patch itself and of its adhesion and slip areas are generally unknown in advance. If these were known, then the elastic fields in the two bodies could be solved independently from each other and the problem would not be a contact problem anymore. Three different components can be distinguished in a contact problem. # First of all, there is the deformation of the separate bodies in reaction to loads applied on their surfaces. This is the subject of general

continuum mechanics Continuum mechanics is a branch of mechanics that deals with the mechanical behavior of materials modeled as a continuous mass rather than as discrete particles. The French mathematician Augustin-Louis Cauchy was the first to formulate such mo ...

. It depends largely on the geometry of the bodies and on their ( constitutive) material behavior (e.g.

elastic Elastic is a word often used to describe or identify certain types of elastomer, elastic used in garments or stretchable fabrics. Elastic may also refer to: Alternative name * Rubber band, ring-shaped band of rubber used to hold objects togethe ...

vs.

plastic Plastics are a wide range of synthetic or semi-synthetic materials that use polymers as a main ingredient. Their plasticity makes it possible for plastics to be moulded, extruded or pressed into solid objects of various shapes. This adapta ...

response, homogeneous vs. layered structure etc.). # Secondly, there is the overall motion of the bodies relative to each other. For instance the bodies can be at rest (statics) or approaching each other quickly (

impact Impact may refer to: * Impact (mechanics), a high force or shock (mechanics) over a short time period * Impact, Texas, a town in Taylor County, Texas, US Science and technology * Impact crater, a meteor crater caused by an impact event * Imp ...

), and can be shifted (sliding) or rotated (

rolling Rolling is a type of motion that combines rotation (commonly, of an axially symmetric object) and translation of that object with respect to a surface (either one or the other moves), such that, if ideal conditions exist, the two are in contact ...

) over each other. These overall motions are generally studied in

classical mechanics Classical mechanics is a physical theory describing the motion of macroscopic objects, from projectiles to parts of machinery, and astronomical objects, such as spacecraft, planets, stars, and galaxies. For objects governed by classi ...

, see for instance multibody dynamics. # Finally there are the processes at the contact interface: compression and

adhesion Adhesion is the tendency of dissimilar particles or surfaces to cling to one another ( cohesion refers to the tendency of similar or identical particles/surfaces to cling to one another). The forces that cause adhesion and cohesion can ...

in the direction perpendicular to the interface, and

and micro-slip in the tangential directions. The last aspect is the primary concern of contact mechanics. It is described in terms of so-called ''contact conditions''. For the direction perpendicular to the interface, the normal contact problem, adhesion effects are usually small (at larger spatial scales) and the following conditions are typically employed: # The gap

e_n

between the two surfaces must be zero (contact) or strictly positive (separation,

e_n>0

); # The normal stress

p_n

acting on each body is zero (separation) or compressive (

p_n > 0

in contact). Mathematically:

e_n \ge 0, p_n \ge 0, e_n\cdot p_n = 0\,\!

. Here

e_n, p_n

are functions that vary with the position along the bodies' surfaces. In the tangential directions the following conditions are often used: # The local (tangential) shear stress

\vec = (p_x, p_y)^\mathsf\,\!

(assuming the normal direction parallel to the

z

-axis) cannot exceed a certain position-dependent maximum, the so-called traction bound

g

; # Where the magnitude of tangential traction falls below the traction bound

\, \vec\,, the opposing surfaces adhere together and micro-slip vanishes, \vec = (s_x, s_y)^\mathsf = \vec\,\!;
# Micro-slip occurs where the tangential tractions are at the traction bound; the direction of the tangential traction is then opposite to the direction of micro-slip \vec = -g\vec/\, \vec\, \,\! .

The precise form of the traction bound is the so-called local friction law. For this Coulomb's (global) friction law is often applied locally: \, \vec\, \le g = \mu p_n\,\!, with \mu the friction coefficient. More detailed formulae are also possible, for instance with \mu depending on temperature T, local sliding velocity \, \vec\,, etc.

Solutions for static cases

Rope on a bollard, the capstan equation

Consider a rope where equal forces (e.g.,

F_\text = 400\,\mathrm

) are exerted on both sides. By this the rope is stretched a bit and an internal tension

T

is induced (

T = 400\,\mathrm

on every position along the rope). The rope is wrapped around a fixed item such as a

bollard A bollard is a sturdy, short, vertical post. The term originally referred to a post on a ship or quay used principally for mooring boats. It now also refers to posts installed to control road traffic and posts designed to prevent automotive ...

; it is bent and makes contact to the item's surface over a contact angle (e.g.,

180^\circ

). Normal pressure comes into being between the rope and bollard, but no friction occurs yet. Next the force on one side of the bollard is increased to a higher value (e.g.,

F_\text = 600\,\mathrm

). This does cause frictional shear stresses in the contact area. In the final situation the bollard exercises a friction force on the rope such that a static situation occurs. The tension distribution in the rope in this final situation is described by the

capstan equation The capstan equation or belt friction equation, also known as Euler-Eytelwein's formula (after Leonhard Euler and Johann Albert Eytelwein), relates the hold-force to the load-force if a flexible line is wound around a cylinder (a bollard, a ...

, with solution: :

\\ \phi_\text &= \frac \log\left(\frac\right) & \end

The tension increases from

T_\text

on the slack side (

\phi = \phi_\text

) to

T_\text

on the high side

\phi = \phi_\text

. When viewed from the high side, the tension drops exponentially, until it reaches the lower load at

\phi = \phi_\text

. From there on it is constant at this value. The transition point

\phi_\text

is determined by the ratio of the two loads and the friction coefficient. Here the tensions

T

are in Newtons and the angles

\phi

in radians. The tension

T

in the rope in the final situation is increased with respect to the initial state. Therefore, the rope is elongated a bit. This means that not all surface particles of the rope can have held their initial position on the bollard surface. During the loading process, the rope slipped a little bit along the bollard surface in the ''slip area''

\phi \in phi_\text, \phi_\text /math>. This slip is precisely large enough to get to the elongation that occurs in the final state. Note that there is no slipping going on in the final state; the term ''slip area'' refers to the slippage that occurred during the loading process. Note further that the location of the slip area depends on the initial state and the loading process. If the initial tension is 600\,\mathrm and the tension is reduced to 400\,\mathrm at the slack side, then the slip area occurs at the slack side of the contact area. For initial tensions between 400 and 600\,\mathrm, there can be slip areas on both sides with a stick area in between.

Generalization for a rope lying on an arbitrary orthotropic surface

If a rope is laying in equilibrium under tangential forces on a rough orthotropic surface then three following conditions (all of them) are satisfied: This generalization has been obtained by Konyukhov A.,

Sphere on a plane, the (3D) Cattaneo problem

Consider a sphere that is pressed onto a plane (half space) and then shifted over the plane's surface. If the sphere and plane are idealised as rigid bodies, then contact would occur in just a single point, and the sphere would not move until the tangential force that is applied reaches the maximum friction force. Then it starts sliding over the surface until the applied force is reduced again. In reality, with elastic effects taken into consideration, the situation is much different. If an elastic sphere is pressed onto an elastic plane of the same material then both bodies deform, a circular contact area comes into being, and a (Hertzian) normal pressure distribution arises. The center of the sphere is moved down by a distance

\delta_n

called the ''approach'', which is equivalent to the maximum penetration of the undeformed surfaces. For a sphere of radius

R

and elastic constants

E, \nu

this Hertzian solution reads: :

\begin
  p_n(x, y) &= p_0 \sqrt & 
    r &= \sqrt \le a & 
    a &= \sqrt \\
  p_0 &= \frac E^* \sqrt &   
    F_n &= \frac E^* \sqrt \delta_n^\frac & 
    E^* &= \frac
\end

Now consider that a tangential force

F_x

is applied that is lower than the Coulomb friction bound

\mu F_n

. The center of the sphere will then be moved sideways by a small distance

\delta_x

that is called the ''shift''. A static equilibrium is obtained in which elastic deformations occur as well as frictional shear stresses in the contact interface. In this case, if the tangential force is reduced then the elastic deformations and shear stresses reduce as well. The sphere largely shifts back to its original position, except for frictional losses that arise due to local slip in the contact patch. This contact problem was solved approximately by Cattaneo using an analytical approach. The stress distribution in the equilibrium state consists of two parts: :

\begin
  p_x(x, y) &= \mu p_0 \left(\sqrt - \frac\sqrt \right) &
    0 \le  &r \le c \\
  p_x(x, y) &= \mu p_n(x, y) & 
    c \le  &r \le a \\
  p_x(x, y) &= 0 &
    a \le  &r
\end

In the central, sticking region

0 \le r \le c

, the surface particles of the plane displace over

u_x = \delta_x/2

to the right whereas the surface particles of the sphere displace over

u_x = -\delta_x/2

to the left. Even though the sphere as a whole moves over

\delta_x

relative to the plane, these surface particles did not move relative to each other. In the outer annulus

c \le r \le r

, the surface particles did move relative to each other. Their local shift is obtained as :

s_x(x, y) = \delta_x + u_x^\text(x, y) - u_x^\text(x, y)

This shift

s_x(x, y)

is precisely as large such that a static equilibrium is obtained with shear stresses at the traction bound in this so-called slip area. So, during the tangential loading of the sphere, ''partial sliding'' occurs. The contact area is thus divided into a slip area where the surfaces move relative to each other and a stick area where they do not. In the equilibrium state no more sliding is going on.

Solutions for dynamic sliding problems

The solution of a contact problem consists of the state at the interface (where the contact is, division of the contact area into stick and slip zones, and the normal and shear stress distributions) plus the elastic field in the bodies' interiors. This solution depends on the history of the contact. This can be seen by extension of the Cattaneo problem described above. * In the Cattaneo problem, the sphere is first pressed onto the plane and then shifted tangentially. This yields partial slip as described above. * If the sphere is first shifted tangentially and then pressed onto the plane, then there is no tangential displacement difference between the opposing surfaces and consequently there is no tangential stress in the contact interface. * If the approach in normal direction and tangential shift are increased simultaneously ("oblique compression") then a situation can be achieved with tangential stress but without local slip. This demonstrates that the state in the contact interface is not only dependent on the relative positions of the two bodies, but also on their motion history. Another example of this occurs if the sphere is shifted back to its original position. Initially there was no tangential stress in the contact interface. After the initial shift micro-slip has occurred. This micro-slip is not entirely undone by shifting back. So in the final situation tangential stresses remain in the interface, in what looks like an identical configuration as the original one. Influence of friction on dynamic contacts (impacts) is considered in detail in.

Solution of rolling contact problems

Rolling contact problems are dynamic problems in which the contacting bodies are continuously moving with respect to each other. A difference to dynamic sliding contact problems is that there is more variety in the state of different surface particles. Whereas the contact patch in a sliding problem continuously consists of more or less the same particles, in a rolling contact problem particles enter and leave the contact patch incessantly. Moreover, in a sliding problem the surface particles in the contact patch are all subjected to more or less the same tangential shift everywhere, whereas in a rolling problem the surface particles are stressed in rather different ways. They are free of stress when entering the contact patch, then stick to a particle of the opposing surface, are strained by the overall motion difference between the two bodies, until the local traction bound is exceeded and local slip sets in. This process is in different stages for different parts of the contact area. If the overall motion of the bodies is constant, then an overall steady state may be attained. Here the state of each surface particle is varying in time, but the overall distribution can be constant. This is formalised by using a coordinate system that is moving along with the contact patch.

Cylinder rolling on a plane, the (2D) Carter-Fromm solution

Consider a cylinder that is rolling over a plane (half-space) under steady conditions, with a time-independent longitudinal creepage

\xi

. (Relatively) far away from the ends of the cylinders a situation of plane strain occurs and the problem is 2-dimensional. If the cylinder and plane consist of the same materials then the normal contact problem is unaffected by the shear stress. The contact area is a strip

x \in a, a /math>, and the pressure is described by the (2D) Hertz solution.

: \begin
  p_n(x) &= \frac \sqrt & 
    , x,  &\le a & 
    a^2 &= \frac \\
  p_0 &= \frac &&&
    E^* &= \frac &
\end The distribution of the shear stress is described by the Carter-Fromm solution. It consists of an adhesion area at the leading edge of the contact area and a slip area at the trailing edge. The length of the adhesion area is denoted 2a' . Further the adhesion coordinate is introduced by x' = x + a - a' . In case of a positive force F_x > 0 (negative creepage \xi < 0) it is:

: \begin
  p_x(x) &= 0 &
    , &x,  \ge a \\
  p_x(x) &= \frac \left( \sqrt - \sqrt \right) &
    a - 2a' \le  &x \le a \\
  p_x(x) &= \mu p_n(x) & 
    &x \le a - 2a'
\end The size of the adhesion area depends on the creepage, the wheel radius and the friction coefficient.

: \begin
     a' &= a \sqrt, &
                \mbox , F_x,  \le \mu F_n \\
    \xi &= -\operatorname(F_x) \, \frac, &
                \mbox , \xi,  \le \frac \\
    F_x &= -\operatorname(\xi) \,\mu F_n \left( 1 - \left( 1 + \frac\right)^2 \right)
\end For larger creepages a' = 0 such that full sliding occurs.

Half-space based approaches

When considering contact problems at the intermediate spatial scales, the small-scale material inhomogeneities and surface roughness are ignored. The bodies are considered as consisting of smooth surfaces and homogeneous materials. A continuum approach is taken where the stresses, strains and displacements are described by (piecewise) continuous functions. The half-space approach is an elegant solution strategy for so-called "smooth-edged" or "concentrated" contact problems. # If a massive elastic body is loaded on a small section of its surface, then the elastic stresses attenuate proportional to

1/distance^2

and the elastic displacements by

1/distance

when one moves away from this surface area. # If a body has no sharp corners in or near the contact region, then its response to a surface load may be approximated well by the response of an elastic half-space (e.g. all points

(x, y, z)^\mathsf \in \R^3\,\!

with

z>0\,\!

). # The elastic half-space problem is solved analytically, see the Boussinesq-Cerruti solution. # Due to the linearity of this approach, multiple partial solutions may be super-imposed. Using the fundamental solution for the half-space, the full 3D contact problem is reduced to a 2D problem for the bodies' bounding surfaces. A further simplification occurs if the two bodies are “geometrically and elastically alike”. In general, stress inside a body in one direction induces displacements in perpendicular directions too. Consequently, there is an interaction between the normal stress and tangential displacements in the contact problem, and an interaction between the tangential stress and normal displacements. But if the normal stress in the contact interface induces the same tangential displacements in both contacting bodies, then there is no relative tangential displacement of the two surfaces. In that case, the normal and tangential contact problems are decoupled. If this is the case then the two bodies are called ''quasi-identical''. This happens for instance if the bodies are mirror-symmetric with respect to the contact plane and have the same elastic constants. Classical solutions based on the half-space approach are: # Hertz solved the contact problem in the absence of friction, for a simple geometry (curved surfaces with constant radii of curvature). # Carter considered the rolling contact between a cylinder and a plane, as described above. A complete analytical solution is provided for the tangential traction. # Cattaneo considered the compression and shifting of two spheres, as described above. Note that this analytical solution is approximate. In reality small tangential tractions

p_y

occur which are ignored.

References

External links

Biography of Prof.dr.ir. J.J. Kalker (Delft University of Technology).

Kalker's Hertzian/non-Hertzian CONTACT software. {{Topics in continuum mechanics Mechanical engineering Solid mechanics