Page 507 - Introduction to Continuum Mechanics
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Non-Newtonian Fluids 491
(c)From the result of part (b), we have
Thus, from Eqs. (8.9.2)
[A3J, [A4J etc. can be obtained by computing the higher derivatives of the components of
C t and evaluating them at r = t.
8.10 Rivlin-Ericksen Tensor in Terms of Velocity Gradients - The Recursive
Formulas
In this section, we show that
