Q:

Neglecting the vibrational motion, a diatomic molecule may be treated as a three-dimensional rigid rotator. The Hamil- tonian

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Neglecting the vibrational motion, a diatomic molecule may be treated as a three-dimensional rigid rotator. The Hamil tonian Hm of the molecule is written as a sum of a translational,Htr, plus a rotational,Hrot, term (that is,Hm =Htr +Hrot).

Consider a system of N very weakly interacting molecules of this kind, in a container of volume V , at a given temperature T .   

(a)Obtain an expression for Hrot in spherical coordinates. Show that there is a factorization of the canonical partition function of this system. Obtain an expression for the specific heat at constant volume.

(B)     Now suppose that each molecule has a permanent electric dipole moment μ and that the system is in the presence of an external  electric  field  E (with  the  dipole μ along  the  axis  of the rotor). What is the form of the new rotational part of the Hamiltonian? Obtain an expression for the polarization of the molecule as a function of field and temperature. Calculate the electric susceptibility of this system.

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The Lagrangian of a free rotator (two atoms of mass m and a fixed interatomic distance a) is given by

from which we have the Hamiltonian

Therefore,

In the presence on an electric field (taken along the x direction), and with the magnetic moment along the axis of the rotator, we have

The associated partition function is given by

Thus, we have

where L (x) is known as the Langevin function.

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