Question: Please solve question 2-9 scripts identifying the chemical species have been dropped for simplicity.) This result, which is valid instantaneously and locally, is equivalent to

Please solve question 2-9

 Please solve question 2-9 scripts identifying the chemical species have been

dropped for simplicity.) This result, which is valid instantaneously and locally, is

scripts identifying the chemical species have been dropped for simplicity.) This result, which is valid instantaneously and locally, is equivalent to Eq. (5.2-2) of Edwards et al. (1991). How does it compare with what is obtained by applying Eq. (2.2-15) to a chemical species? 2-8. Stochastic Model for Diffusion with a First-Order Reaction The objective is to generalize Eq. (2.8-8) to include a homogeneous reaction. Assuming that the reaction follows first-order kinetics and is irreversible, it is characterized on a molecular level by the probability that the molecule survives a given jump. In other words, 1 is the probability that it reacts during a jump. (a) Derive the differential equation governing p(r,t) for the reactive case. How is the first-order, homogeneous rate constant (kV, with units of s1) related to and ? (b) For the result of part (a) to be valid, what restriction must be placed on ? 2-9. Effective Diffusivity for Relative Motion of Two Particles Consider two particles or molecules, A and B, each of which undergoes Brownian motion. It is desired to predict how their relative position will vary with time. Their instantaneous positions relative to a fixed origin are given by the vectors rA and rB and their relative position is r=rBrA. The probability that the relative position is within dr of r is p(r,t)dr. Achieving a particular relative position r requires that B be at rA+r. Accordingly, p(r,t)=pA(rA,t)pB(rA+r,t)drA. To allow for the possibility that A might be anywhere, the integration is over all space. For simplicity, assume that the particles were at the origin at t=0, so that both single-particle probabilities follow Eq. (2.8-15). (a) Let the position vectors be represented as L(t) is rAr=Xex+Yey+Zez=xex+yey+zez Express pA(rA,t) and pB(rA+r,t) in terms of the Cartesian components (x,y,z) and (X,Y,Z). (b) Show that p(r,t)=8[(DA+DB)t]3/21exp[4(DA+DB)tr2] This is the same as Eq. (2.8-15), except that the single-particle diffusivity is replaced by the sum of the diffusivities. In other words, the effective diffusivity for relative motion of A and B is DA+DB. The following integral is helpful in obtaining this result: exp(p2x2qx)dx=pexp(4p2q2)(p>0)

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