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The Finite Element Method for the Analysis of Non-Linear and ...

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Definitions used in Contact <strong>Analysis</strong><br />

Let t f IJ : vector <strong>of</strong> contact surface traction on body I due to contact with<br />

body J <strong>the</strong>n t f IJ = − t f JI . Hence, <strong>the</strong> virtual work due to <strong>the</strong> contact<br />

traction can be written:<br />

∫<br />

δu I<br />

S IJ i fi IJ dS IJ +<br />

∫<br />

δu J<br />

S IJ i fi JI dS JI =<br />

∫<br />

δu IJ<br />

S IJ i fi<br />

IJ dS IJ<br />

where<br />

where<br />

δu IJ<br />

i = δu I i − δu J i<br />

We call <strong>the</strong> pair <strong>of</strong> surfaces S IJ , S IJ a contact surface pair.<br />

S IJ is named <strong>the</strong> ”contactor surface” <strong>and</strong><br />

S JI is named <strong>the</strong> ”target surface”<br />

Hence, <strong>the</strong> right h<strong>and</strong> side <strong>of</strong> <strong>the</strong> previous eqn represents <strong>the</strong> virtual work<br />

<strong>of</strong> <strong>the</strong> contact tractions over <strong>the</strong> relative virtual displacements δu I i , δuJ i<br />

Institute <strong>of</strong> Structural Engineering <strong>Method</strong> <strong>of</strong> <strong>Finite</strong> <strong>Element</strong>s II 36

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