TABLE VI.

Tobacco mosaic characteristics from general rigid bead–rod theory.

Macromolecule	$\frac{I_1}{m{L}^2}$, $\frac{I_2}{m{L}^2}$	$\frac{I_3}{m{L}^2}$	a	b	ν	$\frac{2b}{a\nu }$	$\frac{{\eta }_0-{\eta }_s}{nkT\lambda }$	$\frac{\lambda }{{\lambda }_0}$	λ0Dr	$\frac{{\mathrm{\Psi }}_{\mathrm{0,1}}}{\lambda \left({\eta }_0-{\eta }_s\right)}$
	143	0	$\frac{286}{15}$	$\frac{3}{5}$	$\frac{6}{143}$	$\frac{3}{2}$	1	286	$\frac{1}{1716}$	$\frac{6}{5}$