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Consequence of the EntroPY Principle for a Non-Isotropie Body of Fourier Type. 65) I. Müller 62 '{J may depend on T, T, g and the density p. We say "" that such bodies are of Fourier type, because the heat flux obeys holds and where a and "' Fourier' s law of heat conduction. 66) or holds much along the sarne lines as in an isotropic body. Once we know. 67) ~ aT = The integrability conditions for 11 implied by (2.

The experimentally verifiable results agree for all three theories and, indeed, they concern thermostatics and agree with that theory. v out the other, because thennodynarnic experimentation in non-equilibrium is difficult. 2. Thennodynarnics to Thennostatics 2. 2. 1 . v Thennostatic Processes. Thennostatics neglects acceleration and satisfies the rnomentum balance by considering only uniform fields of density, deformation gradient and temperature. 1) and thE equations of balance (1 . • F e. ds • is the heating.

Müller 62 '{J may depend on T, T, g and the density p. We say "" that such bodies are of Fourier type, because the heat flux obeys holds and where a and "' Fourier' s law of heat conduction. 66) or holds much along the sarne lines as in an isotropic body. Once we know. 67) ~ aT = The integrability conditions for 11 implied by (2.

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