By A. O. Barut (auth.), Bruno Gruber, Francesco Iachello (eds.)
ISBN-10: 1461280826
ISBN-13: 9781461280828
ISBN-10: 1461307872
ISBN-13: 9781461307877
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22) aCt) = di get) = di X(t)g(t) yields get) = X(t)g(t) . l . 13), by missing the observation that the normal forces are up to the density p of a geometric nature. 27) divi yOF(g(tl,X(tl) = 0, where TF(g(t),X(t)l E Coo(M,IR). 26 1 p(X(t))(VU)X(t)X(t) + X(t» = gradiTF(g(tl,X(t» + yO(g(t),X(tl). l(i) invariant, then X(t) has to be divergence free for all tE (-A,A). 29) Tid Diff M = { X E rTM In this case a(t) 01 divi X = °}. l , being a constant function. 53 5. The IRD - invariance of internal constitutive laws Let us assume now that the motion of the deformable medium M is subjected to an internal constitution law F, which admits an integral representation.
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Symmetries in Science III by A. O. Barut (auth.), Bruno Gruber, Francesco Iachello (eds.)
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