Title: Contact Mechanics
1Contact Mechanics
- Maria Persson Gulda
- Kathleen DiSanto
2Outline
- What is Contact Mechanics?
- The two different kind of contacts.
- Boussinesq and Cerruti Potential Functions
- The specific case of an Applied Normal Force
- Hertz Equations- Derivation, Assumptions
- Rigid Sphere Contacting a Deformable Plate
- Deformable Sphere Contacting a Rigid Plate
3What is Contact Mechanics?
- The theory of contact mechanics is concerned
with the stresses and deformation which arise
when the surfaces of two solid bodies are brought
into contact. - Professor Johnsson
4Two kinds of contact
- Conforming contacts
- The two surfaces fit exactly or closely together
without deformation - Non-conforming contact
- The surfaces, or one of the two surfaces, deforms
when there is a contact area in between them.
5Derivation Boussinesq and Cerruti Potential
Functions
- Here are the potential functions
- Each satisfy Laplaces equation
6Special Case Applied Pressure Only
- The potential functions are reduced as follows
- Displacement equations
- By Hookes Law, the stresses are
7Concentrated Normal Force on an Elastic Half Space
- The displacements are
- The stresses in polar coordinates
8Concentrated Force Cont.
- Now looking only at the surface, z0
- The displacements in polar coordinates become
- For a general pressure distribution, the
displacement for any surface point in S, by
Greens function method, becomes
9Hertz Pressure
- The Pressure distribution is
- Equation for determining surface displacement
-
- The Hertz displacement equation
where a is the radius of the contact area
10Hertz Theory of Elastic Contact
- Assumptions
- The radii of curvature of the contacting bodies
are large compared with the radius of the circle
of contact. - The dimensions of each body are large compared to
the radius of the circle of contact. - The contacting bodies are in frictionless
contact. - The surfaces in contact are continuous and
nonconforming.
11Examples
- Focus on two examples
- Rigid spherical indenter pushing to deformable
flat surface. - Deformable sphere contacting rigid plate.
(2)
(1)
12Equations to be Used
- where R is the radius of the rigid sphere and
- RS is the radius of the deformable plate
(2) where d is the vertical distance the point
where the load is applied moves and a
is the contact area radius determined by
the equation
(3) h is the original distance between a point
on the rigid sphere and the deformable
plate before load application.
(4) These are the equations of
displacement derived previously
(5) This states that the translation of the
point of load application equals the
surface displacement of the plate and
sphere plus the original distance
between the surfaces.
13Rigid Sphere Contacting Deformable Flat Surface
with Abaqus
Theoretical Contact Radius 11.995 mm Abaqus
Contact Radius 11.6 mm Error 3
14Deformable Sphere Contacting Rigid Plate with
Abaqus
Theoretical Contact Radius 9.288 mm Abaqus
Contact Radius 8.5 mm Error 6
15Conclusion
- Contact problems in general are very complicated
to model numerically and theoretically - Other factors
- Friction - rough surfaces
- Blunt edges, sharp corners
- Sliding and rolling contact
- Dynamic impact
16A Special Thank You To
- Dr. Ashkan Vaziri
- Professor James Rice
17References
- Johnson, K. L. Contact Mechanics, Cambridge
Cambridge University Press 1985 - Fisher-Cripps, A. C. The Hertzian contact
surface. J. Materials Science. 199934129-137 - Kogut, L., Etsion, I. Elastic-Plastic Contact
Analysis of a Sphere and a Rigid Flat. J. of
Applied Mechanics. 200269657-662 - Johnson, K. L., Greenwood, J. A. An Adhesion Map
for the contact of elastic Spheres. J. of Colloid
and Interface Science. 1997192326-333 - Barber, J. R.,Clavarella, M. Contact mechanics.
Inter. J. of Solids and Structures. 20003729-43
18Any Questions?