A motile bacterium of radius senses a chemoattractant of diffusion coefficient…

PHYSICS · Multi-part · Fermi University Physics · Biophysics & Medical Physics · Physical foundations of the living cell · Physical foundations of the living cell

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

Problem

A motile bacterium of radius a=0.50 μma = 0.50\,\mathrm{\mu m} senses a chemoattractant of diffusion coefficient D=5.0×10−10 m2 s−1D = 5.0\times10^{-10}\,\mathrm{m^2\,s^{-1}} present at bulk concentration c∞=1.0 μMc_\infty = 1.0\,\mathrm{\mu M}, using receptor patches of radius s=2.0 nms=2.0\,\mathrm{nm} scattered uniformly over its surface. The rate at which ligand molecules are captured by NN patches is I=4πDac∞ NsNs+πaI = 4\pi Dac_\infty\,\frac{Ns}{Ns+\pi a} (quoted). ((a)) Design the number of receptor patches NN the bacterium needs to capture at least 90%90\% of the diffusion-limited maximum rate Imax⁡=4πDac∞I_{\max}=4\pi Dac_\infty (the rate a fully absorbing sphere would achieve). ((b)) What fraction of its surface area do these patches cover, using Ns2/4a2Ns^2/4a^2 (quoted) as the coverage? ((c)) Evaluate Imax⁡I_{\max} and the actual capture rate II achieved with the NN from part (a), in molecules per second.

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