A planar nematic cell of thickness and splay constant sits exactly at its…

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

Soft Matter at the Thermal Scale, Ch Frank elasticity, defects and smectic layers

Problem

A planar nematic cell of thickness d=8 μmd = 8\,\mu\mathrm{m} and splay constant K1=6.4 pNK_1 = 6.4\,\mathrm{pN} sits exactly at its Freedericksz threshold, where the director begins to tilt with a distortion wavevector q=π/dq = \pi/d. ((a)) At threshold the tilt amplitude is still vanishingly small, so estimate instead the elastic stiffness of this mode, the Frank energy density per radian squared of tilt, f≈12K1q2f \approx \tfrac12K_1q^2. ((b)) A rubber network (recall the entropic spring result G=nskBTG = n_sk_BT) has ns=1.0×1025 m−3n_s = 1.0\times10^{25}\,\mathrm{m^{-3}} effective strands per unit volume at T=298 KT = 298\,\mathrm{K}. Find its shear modulus GG. ((c)) Give the ratio of the Frank stiffness from part (a) to the rubber modulus from part (b), and say in one sentence what this ratio tells you about how easily a field can distort a nematic compared with how easily a rubber network can be sheared.

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