1549380323-Statistical Mechanics Theory and Molecular Simulation

(jair2018) #1

364 Free energy calculations


e. Develop a Monte Carlo approach for sampling the distribution function

P(q) =

1


Z


e−βφ(q)

from part d.

f. Derive molecular dynamics equations of motion, including full expressions
for the force onqusing the chain rule on the derivatives (dU/dx)(dx/dq)
and (dU/ ̃ dx)(dx/dq), and develop a numerical procedure for obtaining
these forces.

Hint: Consider expanding exp[−βU ̃(x)] in a set of orthogonal polyno-
mials such as Legendre polynomialsPl(α(x)) withα(x)∈[− 1 ,1]. What
should the functionα(x) be?

8.14. It has been suggested (Peterset al., 2007) that the committor probability
pB(r) for a single reaction coordinateq(r) can be approximated by a function
πB(q(r)) that depends onronly throughq(r).
a. What are the advantages and disadvantages of such an approximation?

b. Suppose thatπB(q(r)) can be accurately fit to the following functional
form
πB(q(r)) =
1 + tanh(q(r))
2

.


Isq(r) a good reaction coordinate? Why or why not?
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