Chapter 12: Problem 7
Proteins and other macromolecules can be separated by size using centrifugation. The idea is to spin a sample containing proteins of different size in solution. The spinning produces a centrifugal force per unit mass \(g_{c},\) which leads to diffusion with a drift velocity that depends on the protein size. We assume that a protein in the sample can be approximated as a ball of radius \(R\) (a) Following the discussion in the chapter, fill in the steps leading up to the formula for the drift velocity of the protein as a function of its radius (Equation 12.45 ), \(v_{\text {drift }}=\frac{2\left(\rho_{\text {protein }}-\rho_{\text {solvent }}\right) g_{c} R^{2}}{9_{\eta}}\) where \(\rho_{\text {protein }}\) and \(\rho_{\text {solvent }}\) are the densities of the protein and the solvent and \(\eta\) is the solvent viscosity. (b) Estimate the drift velocity for hemoglobin in water in an ultracentrifuge with \(g_{c} \approx 10^{5} g\), where \(g=10 \mathrm{m} / \mathrm{s}^{2}\) is the acceleration of freely falling objects in Earth's gravitational field. Assume a typical protein density of \(1.2 \mathrm{g} / \mathrm{cm}^{3}\) (c) We would like to separate two similar proteins, having the same density, \(\rho^{\prime}=1.35 \mathrm{g} / \mathrm{cm}^{3} .\) They have diameters of \(4 \mathrm{nm}\) and \(5 \mathrm{nm}\), respectively. The two protein species start out mixed together in a thin layer at the top of a \(1 \mathrm{cm}\) long centrifuge tube. How large should the centrifuge acceleration \(q_{c}\) be so that the two proteins are separated before they drift to the end of the tube?
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