A dilute suspension of a small ribonucleoprotein particle is spun in a centrifuge at…

PHYSICS · Multi-part · Fermi University Physics · Thermal, Statistical & Complex Systems · Biophysics & Medical Physics · Physical foundations of the living cell

Forces, Machines and Signals, Ch Diffusion: friction, capture and the crowded cytoplasm

Problem

A dilute suspension of a small ribonucleoprotein particle is spun in a centrifuge at constant angular velocity ω\omega. In the rotating frame each particle of buoyant mass mb=m(1−vˉρ)m_b = m(1-\bar v\rho) (the mass corrected for the buoyancy of the displaced fluid) feels an outward force F(r)=mbω2rF(r) = m_b\omega^2 r at radius rr from the axis, playing the part that mbgm_b g plays for a particle settling under gravity. ((a)) Write the outward drift flux Jdrift(r)=c(r)F(r)/ζJ_{\rm drift}(r) = c(r)F(r)/\zeta and the inward diffusive flux Jdiff(r)=−D dc/drJ_{\rm diff}(r) = -D\,dc/dr for the spinning suspension. Setting Jdrift+Jdiff=0J_{\rm drift}+J_{\rm diff}=0 once the profile has become steady, show that the resulting c(r)c(r) matches the Boltzmann distribution c(r)∝exp⁡[mbω2r2/(2kBT)]c(r)\propto \exp[m_b\omega^2 r^2/(2k_BT)] only if Dζ=kBTD\zeta = k_BT, independent of ω\omega, rr and the particle's shape. ((b)) A run at ω=5.0×102 rad s−1\omega = 5.0\times10^{2}\,\mathrm{rad\,s^{-1}} and T=293 KT=293\,\mathrm{K} reaches a steady profile with c(r2)=22 c(r1)c(r_2) = 22\,c(r_1) for r1=6.80 cmr_1 = 6.80\,\mathrm{cm} and r2=7.00 cmr_2 = 7.00\,\mathrm{cm}. Use the Boltzmann profile of part (a) to find the buoyant mass mbm_b of one particle. ((c)) Electron microscopy gives the particle a radius a=6.0 nma=6.0\,\mathrm{nm}. Taking the drag coefficient in water (η=1.0×10−3 Pa s\eta = 1.0\times10^{-3}\,\mathrm{Pa\,s} at 293 K293\,\mathrm{K}) as ζ=6πηa\zeta = 6\pi\eta a (quoted, for a sphere), use Dζ=kBTD\zeta = k_BT from part (a) to find the particle's diffusion coefficient DD. ((d)) The same particle now diffuses towards a fixed absorbing site of radius A=50 nmA = 50\,\mathrm{nm} (large enough that the particle can be treated as a point particle). Find the diffusion-limited rate constant for capture, k=4πDAk = 4\pi DA, in m3 s−1\mathrm{m^3\,s^{-1}} per particle and convert it to M−1 s−1\mathrm{M^{-1}\,s^{-1}}.

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