Tobacco mosaic virus (TMV) forms rigid rods of length and diameter

PHYSICS · Multi-part · Fermi University Physics · Condensed Matter, Materials & Soft Matter · Soft condensed matter · Soft condensed matter

Soft Matter at the Thermal Scale, Ch Nematic order and the isotropic-nematic transition

Problem

Tobacco mosaic virus (TMV) forms rigid rods of length L=300 nmL = 300\,\mathrm{nm} and diameter D=18 nmD = 18\,\mathrm{nm}. A thermotropic nematic made of similarly rod-shaped molecules has Landau-de Gennes coefficients (in the magnitude normalisation used for the invariants of QijQ_{ij}) a=0.15 MJ m−3 K−1a = 0.15\,\mathrm{MJ\,m^{-3}\,K^{-1}}, B=1.5 MJ m−3B = 1.5\,\mathrm{MJ\,m^{-3}} and C=4.0 MJ m−3C = 4.0\,\mathrm{MJ\,m^{-3}}. ((a)) Using the numerically exact solution of Onsager's equation, ϕI=3.29 D/L\phi_{\rm I} = 3.29\,D/L and ϕN=4.19 D/L\phi_{\rm N} = 4.19\,D/L, compute the coexistence concentrations at which the TMV suspension separates into isotropic and nematic phases. ((b)) Using TNI−T∗=2B2/9aCT_{\rm NI} - T^* = 2B^2/9aC and Sn(TNI)=2B/3CS_{\rm n}(T_{\rm NI}) = 2B/3C, compute the supercooling range and the order-parameter jump of the thermotropic nematic.

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