Project: Particle entrapment in an EHD contact of a ball rolling-sliding on a flat surface.

Client: SKF Engineering & Research Centre B. V. (The Netherlands)  

Researcher: George K. Nikas (Imperial College London, Mechanical Engineering Department).


Project duration: 3 months (1996).

Technical report: A technical report was written by Dr Nikas and distributed to the supervisors of the project. The 79-page report contains 56 figures and 103 detailed equations.

Computer software developed: program SKF. Solid particle entrainment and entrapment analysis in elastohydrodynamic contacts. Compiled in FORTRAN 95. Code length: 798 lines. Latest version: 1.4.1.


    This project was about the theoretical modelling of the entrainment and entrapment of small, solid, spherical particles in a sliding-rolling elastohydrodynamic point contact of a ball on a plane. The model consists of two parts.

  1. The first part deals with the solution of the three-dimensional Navier-Stokes equations for a viscous, incompressible fluid to find how a particle behaves in the flow as the ball moves and rotates with constant speeds on the plane. As a result, the probability of a particle to end on the ball (collide with the ball) or to bypass it are estimated. The latter is achieved by solving the equation of motion of a particle in the fluid flow.

  2. The second part deals with what happens when a particle collides with the ball. An entrapment criterion is used to find if the particle will be temporarily rejected or if it will be trapped between the ball and the flat surface.

    Particles which are rejected many times may accumulate in the inlet zone of the contact and cause fluid starvation and scuffing. On the other hand, particles that are entrapped could damage the contact surfaces by abrasion or indentation.

    An example of the simulation is presented in the next figure, which shows 30 possible trajectories of a 20 micron spherical solid particle left in front of a ball rolling-sliding on a flat surface. The film thickness far away from the ball is 100 microns. The particle is left on the flat and is affected by the fluid flow created by the moving ball. Depending on its initial position, the particle may collide with the ball, become entrapped, be rejected by the ball, or completely bypass it. The "Particle contact semi-circle" is the line defining the imaginary boundary where a particle will come in first (undeformed) contact with both the ball and the flat (that is, the particle cannot enter that semi-circular area without being deformed first).

30 possible trajectories of a 20 micron particle left on the upper half area of the graph. Copyright George K. Nikas

30 possible trajectories of a 20 micron particle left on the upper half area of the graph.


    This is a very detailed study but, with the aid of the developed computer program, the risks of damage can be assessed quickly for any operating conditions (contact speed, film thickness, particle size, etc).

Publications of the author related to this work (most recent first)

Homepage of Dr Nikas