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Co-rotational time flux

To summarise, we have from equations (4.22), (4.23), (4.25) and (4.26) that the quantities v, Vv, W and h do not satisfy the principle of material frame-indifference, while from equations (4.18), (4.24) and (4.27) we see that the director n, the rate of strain tensor A and the co-rotational time flux N are frame-indifferent and therefore objective. For later ease of reference, we record that... [Pg.138]

Therefore, by the definitions of the relative angular velocity u and the co-rotational time flux N in equations (4.2) and (4.8), respectively, equation (4.76) leads to an equivalent formulation of the left-hand side of inequality (4.61) given by... [Pg.145]


See other pages where Co-rotational time flux is mentioned: [Pg.135]    [Pg.151]    [Pg.168]    [Pg.171]    [Pg.189]    [Pg.199]    [Pg.210]    [Pg.293]    [Pg.135]    [Pg.151]    [Pg.168]    [Pg.171]    [Pg.189]    [Pg.199]    [Pg.210]    [Pg.293]    [Pg.6158]    [Pg.176]    [Pg.176]    [Pg.585]    [Pg.356]   
See also in sourсe #XX -- [ Pg.135 , Pg.151 , Pg.293 ]




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Co-rotational

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