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G25.2651: Statistical Mechanics

Problem set #3

Due: March 3, 2003

1.
Calculate the volume fluctuations tex2html_wrap_inline106 given by

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in the isothermal-isobaric ensemble. Express your answer in terms of the isothermal compressibility tex2html_wrap_inline108 given by

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Show that tex2html_wrap_inline110 and hence vanish in the thermodynamic limit.

2.
onsider an ideal gas of N particles at temperature T inside a cylinder with radius a and a vertical extent L. The cylinder rotates along its axis (taken as the z-axis) with angular velocity tex2html_wrap_inline122 . In addition, a uniform gravitational field g acts vertically in the negative z direction. In this case, the Hamiltonian for a single particle is given by

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where tex2html_wrap_inline128 is the z component of the cross product.

a.
Calculate the canonical partition function.
b.
Suppose that the cylinder is equipped with a movable piston that allows only the length, L, to change in such a way as to maintain a constant pressure. What is the partition function in this case?

Hint: It may help you to know that the binomial expansion is

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c.
Imagine, once again, the case of fixed cylinder volume. Using cylindrical coordinates tex2html_wrap_inline134 , imagine dividing the cylinder into rings of radius r with radial thickness tex2html_wrap_inline138 and height tex2html_wrap_inline140 . Within a ring, we can assume that r and z are constant. Also within each ring, we can work in the grand canonical ensemble. Show generally (i.e., even in the presence of interactions between the particles), that the grand canonical partition function satisfies:

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where tex2html_wrap_inline146 is the grand canonical partition function for tex2html_wrap_inline148 and g=0. tex2html_wrap_inline152 is the volume of the ring. What is tex2html_wrap_inline154 ?

3.
A simple model for polymers is the so called Gaussian random coil model, which is illustrated in the figure below:

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In this model, the endpoint particles at positions tex2html_wrap_inline156 and tex2html_wrap_inline158 are fixed in space, while the remaining N particles are free to move. Assume all particles have the same mass m. The N particles interact with each other via a nearest-neighbor harmonic potential of the form:

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where tex2html_wrap_inline122 is the frequency of the harmonic coupling between neighboring particles. In the above expression, we adopt the convention that tex2html_wrap_inline168 and tex2html_wrap_inline170 .

We now want to calculate the canonical partition function of this polymer at temperature T.

a.
Write down the expression for tex2html_wrap_inline174 . Why does Q have these arguments?

b.
Consider the following change of integration variables in the expression for tex2html_wrap_inline178 :

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By performing this change of variables, calculate the canonical partition function.

Hint: Note that the transformation is defined recursively. How should you start the recursion?

c.
Suppose the endpoints at tex2html_wrap_inline156 and tex2html_wrap_inline158 are no longer fixed. A quantity of central interest in the study of polymers is the so called mean-square end-to-end distance tex2html_wrap_inline184 , which can be measured by light scattering experiments. Determine this ensemble average when the endpoints are free to move.




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Mark Tuckerman
Wed Feb 19 17:44:26 EST 2003