A bacterial chemoreceptor cluster is modelled as a protein with identical…

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

Forces, Machines and Signals, Ch Cooperativity: zippers, melting and allosteric binding

Problem

A bacterial chemoreceptor cluster is modelled as a protein with n=3n=3 identical ligand-binding sites that never interact with one another directly. The protein exists in two conformations, active (A) and inactive (I). A bound ligand contributes a statistical weight x=c/KAx=c/K_A per site when the protein is in state A, and ϵx\epsilon x per site (with ϵ=KA/KI<1\epsilon=K_A/K_I<1) when it is in state I; the unliganded I state carries a weight LL relative to the unliganded A state, which is taken as the reference state of weight 11. ((a)) Build the states-and-weights table over the number of ligands bound (0,1,2,30,1,2,3) in each conformation, sum each row with the binomial theorem, and hence show that the partition function is Z(x)=(1+x)n+L(1+ϵx)nZ(x)=(1+x)^n+L(1+\epsilon x)^n with n=3n=3. Differentiate ln⁡Z\ln Z to obtain the fractional occupancy θ(x)\theta(x), and show that it collapses to the simple hyperbola θ=x/(1+x)\theta=x/(1+x) if either L=0L=0 or ϵ=1\epsilon=1. In one or two sentences explain why the three sites can still show a cooperative, S-shaped binding curve for general LL and ϵ≠1\epsilon\ne1 even though no site ever senses the occupancy of another. ((b)) A separate synthetic polypeptide of 400400 residues has Zimm-Bragg nucleation parameter σ=1.0×10−3\sigma=1.0\times10^{-3}. Starting from the cooperative length ℓ=σ−1/2\ell=\sigma^{-1/2} and the midpoint slope dθdln⁡s∣s=1=14σ\left.\dfrac{d\theta}{d\ln s}\right|_{s=1}=\dfrac{1}{4\sqrt\sigma}, derive a single relation between the slope and ℓ\ell, then evaluate ℓ\ell and the slope for this peptide. State whether the whole chain melts as one cooperative unit.

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