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. In the rotating frame each particle of buoyant mass mb=m(1−vˉρ) (the mass corrected for the buoyancy of the displaced fluid) feels an outward force F(r)=mbω2r at radius r from the axis, playing the part that mbg plays for a particle settling under gravity.
((a)) Write the outward drift flux Jdrift(r)=c(r)F(r)/ζ and the inward diffusive flux Jdiff(r)=−Ddc/dr for the spinning suspension. Setting Jdrift+Jdiff=0 once the profile has become steady, show that the resulting c(r) matches the Boltzmann distribution c(r)∝exp[mbω2r2/(2kBT)] only if Dζ=kBT, independent of ω, r and the particle's shape.
((b)) A run at ω=5.0×102rads−1 and T=293K reaches a steady profile with c(r2)=22c(r1) for r1=6.80cm and r2=7.00cm. Use the Boltzmann profile of part (a) to find the buoyant mass mb of one particle.
((c)) Electron microscopy gives the particle a radius a=6.0nm. Taking the drag coefficient in water (η=1.0×10−3Pas at 293K) as ζ=6πηa (quoted, for a sphere), use Dζ=kBT from part (a) to find the particle's diffusion coefficient D.
((d)) The same particle now diffuses towards a fixed absorbing site of radius A=50nm (large enough that the particle can be treated as a point particle). Find the diffusion-limited rate constant for capture, k=4πDA, in m3s−1 per particle and convert it to M−1s−1.