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D.H. Lammlein PhD Dissertation - Vanderbilt University

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(1.11)<br />

where r p is the probe (pin) radius, h is the probe height, is the average shear stress<br />

over the probe surface, µ is the coefficient of friction, F is the translational force during<br />

welding, and λ is the thread helix angle. The remaining terms are defined as follows:<br />

Russell et al. [12] estimate the contribution of the probe to the total heat<br />

generation near the interface to be approximately 2% using equation (1.7) and assuming<br />

the contact shear stress to be 5% of its room temperature value (taking into account<br />

material softening with temperature and strain). Simar et al. [8] estimate 12% for this<br />

same value. These analytically calculated probe contributions are tool geometry,<br />

material, and parameter dependent, as are the empirical values.<br />

Debate exists over the predominant nature of the tool interface contact<br />

condition, particularly for the shoulder, and how best to model it. Schmidt et al. [24]<br />

assume full shoulder contact with a constant frictional coefficient over the shoulder<br />

surface. Under these conditions, slip occurs where the frictional shearing does not<br />

exceed the shear yield strength of the material, and stick occurs elsewhere. Colgrove et<br />

al. [22] use a stick condition with an artificially small contact radius and achieve good<br />

agreement with experiment. The authors however concede this approach to be physically<br />

unrealistic. Its use is justified as a simplification. The authors state that a slip condition<br />

13

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