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One and two-fiber orientation kinetic theories of fiber suspensions

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Fig. 1. Two-fiber kinetic theory in 2D with n = B 0 = 0. There are no fiber–fiber correlations in the orientation and the stresses are the same as in the one-fiber kinetic theory.
Fig. 2. Two-fiber kinetic theory in 2D with (i) n – 0; B 0 ¼ 0, (ii) n – 0;B 0 – 0, (iii) n ¼ 0; B 0 – 0.
Fig. 3. Correlation function in the two-fiber kinetic theory in 2D with (i) n – 0; B 0 ¼ 0, (ii) n – 0; B 0 – 0, (iii) n ¼ 0; B 0 – 0.
illustration of the general formalism, Phys. Rev. E 56 (1997) 6633–6650.

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