INDIAN INSTITUTE OF TECHNOLOGY GUWAHATI Department of Physics Statistical Mechanics: PH404 Tutorial-II 1. One of the equations of state of black body radiation in a box of volume V and at temperature T is given by E P = 3V where E is the internal energy and P is the pressure. Using thermodynamic principles, obtain the Stefan-Boltzmann law, the other equation of state. Knowing two equations of state, find the fundamental equation of the system. 2. Compute the Helmholtz free energy for a van der Waals gas. The equation of state is P = NkB T aN 2 − 2 V − Nb V where a and b are constants which depend on the type of gas and N is the number of molecules. Assume that heat capacity is CV = 3NkB /2. 3. Consider the following pair of equations 3 E = PV 2 and P = a V Tn N where a is a constant and n is an arbitrary integer. For which value of n, these equations would represent a compatible pair of thermodynamic equations of state? For that value of n calculate the Helmholtz free energy of the system. 4. A thermodynamic system is described by the fundamental equation S −a N 4 =b V E4 , N3 where a and b are constants. Obtain an expression for the Gibbs free energy G(N, P, T ) of the system. 5. Compute the entropy, enthalpy, Helmholtz free energy, and Gibbs free energy for a paramagnetic substance and write them explicitly in terms of their natural variables if possible. Assume that mechanical equation of state is M = cH/T where M is the total magnetization, H is the external magnetic field, c is the Curie constant, and T is the temperature. The heat capacity at constant magnetization CM can be taken as constant, 6. Show that for a magnetic system 2 χT (CH − CM ) = T αH and CH /CM = χT /χS where αH is the coefficient of magnetization expansion and χT , χS are the isothermal and isentropic susceptibilities respectively. 1 7. Show that ∂CP ∂P = −T V αP2 + T ∂αP ∂T . P 8. Compute the heat capacity CP , the compressibilities, κT and κS , and the thermal expansion coefficient αP of a monatomic van der Waals gas for which the mechanical equation of state is NkB T aN 2 P = − 2 V − Nb V and the heat capacity is CV = 3NkB /2, where V is the volume. Is this gas stable for all values of P and V ? 9. The internal energy of a model paramagnet is given by E = NkB T0 exp S M2 + 2 2 NkB N M0 where T0 and M0 are positive constants. Calculate χT and χS , the isothermal and isentropic magnetic susceptibilities, of the system. Obtain χT as a function of T and χS as a function of T and H. 10. The following two equations are assumed to be fundamental equations of physical systems N 5/2 T 1/2 S 3/2 V 2 (ii) F = b (i) E = a 5/2 , N V 3/2 where a and b are positive constants. Do they satisfy stability criteria of thermodynamic systems? 2
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