For a narrowly aligned nematic liquid crystal, the scalar nematic order parameter is . Hence the small-angle width of nematic orientation isThis is a root-mean-square angular width about the unoriented nematic director. The single value of does not determine a complete distribution or its full width at half maximum. For an isotropic two-component Gaussian tilt, each transverse component would have standard deviation .
For a spherical micelle of sodium dodecyl sulfate with molecules and a sharp tail-filled core of radius , volume and head-group area give and . Dividing gives the spherical micelle geometryThere is a consistency limit: exceeds the supplied maximum tail length . Equivalently the amphiphile packing parameter is , outside the strict spherical-core bound. Thus the requested spherical assumption gives these estimates, but the three molecular dimensions cannot all be exact within that ideal sharp-core geometry. Effective head area, core structure or aggregate shape must adjust; silently replacing by would no longer satisfy both packing equations.
For the polybutadiene chain in 1,4-dioxane, define from the negative end charge toward the positive one. The electric dipole energy is , so the force conjugate to end separation is , even though the two endpoint forces are opposite. Balancing it against the entropic spring force givesNumerically,The zero-field rms of just the component is , a different comparison. The mean extension is still much smaller than the contour length , consistent with the Gaussian ideal chain force law. This is an end-charged ideal polymer in an electric field; the direct endpoint Coulomb interaction is omitted as stipulated.
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