PHYSICS · Multi-part · Fermi University Physics · Biophysics & Medical Physics · Molecular machines, transport and bioenergetics · Molecular machines, transport and bioenergetics
Forces, Machines and Signals, Ch Measuring one molecule: traps, tweezers and single-molecule fluorescence
Problem
Kinesin-1 advances along a microtubule in 8.0nm steps. To time individual steps reliably, an optical-trap assay records the bead's position with a detection bandwidth of B=2.0kHz. The bead sits in water of viscosity η=1.0×10−3Pas at T=298K (kBT=4.11pNnm), held by a trap of stiffness κ=0.10pNnm−1. Treat the bead as a sphere in an unbounded fluid (ζ=6πηa) and the trap as harmonic. The one-sided position spectrum in the trap is the Lorentzian Sx(f)=kBT/[π2ζ(fc2+f2)] with fc=κ/2πζ, and the mean-square position noise in a bandwidth 0 to B is ⟨δx2⟩=∫0BSx(f)df=πκ2kBTarctan(B/fc), which reduces to the flat-spectrum result ⟨δx2⟩≈4kBTζB/κ2 only when B≪fc.
((a)) For the bead ordinarily used in this assay, of diameter 1.0μm, find fc and decide whether B counts as small compared with fc. Using whichever expression for ⟨δx2⟩ is appropriate, compute the rms noise δx=⟨δx2⟩ at B=2.0kHz, and state whether the 8.0nm step can be told apart from this noise with confidence.
((b)) A colleague proposes replacing the bead with one of diameter 0.20μm, keeping κ and B the same. Recompute fc, check whether B≪fc now holds, find the new δx, and state whether this change resolves the difficulty found in part (a).