A micropipette aspiration experiment on a giant unilamellar vesicle at is carried out…

PHYSICS · Multi-part · Fermi University Physics · Biophysics & Medical Physics · Macromolecules, membranes and cell architecture · Macromolecules, membranes and cell architecture

Forces, Machines and Signals, Ch The fluid membrane: bending, flicker and shape

Problem

A micropipette aspiration experiment on a giant unilamellar vesicle at 298 K298\,\mathrm{K} is carried out entirely in the low-tension, entropic-tension regime, where the area strain obeys α=kBT8πκln⁡(σσ0).\alpha = \frac{k_BT}{8\pi\kappa}\ln\left(\frac{\sigma}{\sigma_0}\right). Two points on the aspiration curve are recorded: at σ1=1.0 μN m−1\sigma_1 = 1.0\,\mu\mathrm{N\,m^{-1}}, α1=0.80%\alpha_1 = 0.80\%; at σ2=10.0 μN m−1\sigma_2 = 10.0\,\mu\mathrm{N\,m^{-1}}, α2=2.00%\alpha_2 = 2.00\%. ((a)) Use the two data points to extract the bending modulus κ\kappa of this membrane, in joules and in units of kBTk_BT. ((b)) A separate optical-tweezers pulling experiment on a single actin filament, a semiflexible polymer treated with the worm-like chain, finds a persistence length ξp=15 μm\xi_p = 15\,\mu\mathrm{m}. Using ξp=κf/kBT\xi_p = \kappa_f / k_BT, where κf\kappa_f is the filament's bending stiffness, find κf\kappa_f in SI units. ((c)) Explain why κf\kappa_f from part (b) cannot be compared numerically to κ\kappa from part (a), even though both are called a bending modulus and both use the symbol κ\kappa. Name the dimensional difference and the geometric reason for it, bending a one-dimensional rod versus bending a two-dimensional sheet. ((d)) The pipette applies a real mechanical tension σ\sigma. Explain, using the idea of an entropic force, why the low-tension area response probed in part (a) is nevertheless called entropic, and why it depends on κ\kappa but not on KAK_A.

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