For rigid-body motion, the strains will vanish. Under these conditions, integrate the straindisplacement relations (7.6.1) to show
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For rigid-body motion, the strains will vanish. Under these conditions, integrate the strain–displacement relations (7.6.1) to show that the most general form of a rigid-body motion displacement field in polar coordinates is given by:
Equation 7.6 .1
where a, b, c are constants. Also show that this result is consistent with the Cartesian form given by relation (2.2.9).
Equation 2.2 .9
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Elasticity Theory Applications And Numerics
ISBN: 9780128159873
4th Edition
Authors: Martin H. Sadd Ph.D.
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