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What led van der Waals to modify the ideal gas equation? Using the concepts of critical temperature T_c, pressure P_c and volume V_c, show that the critical constant for a real gas is 8/3.

CSE 2011Paper I5/15 markscse-2011-subject-04-001

Find out the expressions for van der Waals constants a and b.

CSE 2011Paper I20 markscse-2011-subject-04-002

Write down the expression for the Bose-Einstein distribution function and explain the meaning of the symbols used.

IFoS 2011Paper I10 marksifos-2011-subject-04-002

Consider a gas of photons in equilibrium and contained in a volume V at a temperature T. Using the Bose-Einstein statistics, calculate the total energy of the photon gas.

IFoS 2011Paper I20 marksifos-2011-subject-04-003

Write down the expressions for Bose-Einstein and Fermi-Dirac distribution functions, and show how Fermi-Dirac distribution leads to the explanation of Pauli's exclusion principle.

CSE 2011Paper I10 markscse-2011-subject-04-004

Show that the elemental quantity of heat \delta Q is not a total differential.

IFoS 2011Paper Iifos-2011-subject-04-001

Consider one mole of an ideal gas whose pressure changes with volume as P=\alpha V, where \alpha is a constant. If it is expanded such that its volume increases m times, find the change in internal energy, work done by the gas and heat capacity of the gas.

CSE 2010Paper I25 markscse-2010-subject-04-003

Calculate the change in pressure for a change in freezing point of water equal to -0.91^\circ\mathrm{C}. Given, the increase of specific volume when 1 gm of water freezes into ice is 0.091 cc/gm and latent heat of fusion of ice is 80 cal/gm.

CSE 2010Paper I10 markscse-2010-subject-04-002

Derive an expression for the thermal efficiency of a reversible heat engine operating on the Diesel cycle with an ideal gas of constant heat capacity as the working medium.

CSE 2010Paper I25 markscse-2010-subject-04-004

1 kmol of an ideal gas is compressed isothermally at 400 K from 100 kPa to 1000 kPa in a piston and cylinder arrangement. Calculate the entropy change of the gas, the entropy change of the surroundings and the total entropy change resulting from the process if the process is mechanically reversible and the surroundings consist of a heat reservoir at 400 K.

CSE 2010Paper I10 markscse-2010-subject-04-001

Calculate the number of different arrangements of 10 indistinguishable particles in 15 cells of equal a priori probability, considering that one cell contains only one particle.

CSE 2010Paper I10 markscse-2010-subject-04-005

Consider the following statement: ``The Fermi energy of a given material is the energy of that quantum state which has the probability equal to \frac{1}{2} of being occupied by the conduction electrons.'' Is the above statement correct? Give reasons for your answer.

CSE 2010Paper I10 markscse-2010-subject-04-006

Explain why the distribution of speeds of molecules emerging through a small hole in an effusive molecular beam source is not a Maxwellian distribution.

IFoS 2010Paper I5 marksifos-2010-subject-04-002

N particles are distributed among three states having energies E = 0, E = kT and E = 2kT. If the total equilibrium energy of the system is 1000 kT, what is the value of N?

IFoS 2010Paper I15 marksifos-2010-subject-04-001

(ii) -\left(\dfrac{\partial f}{\partial E}\right) is symmetric about the Fermi level.

IFoS 2010Paper I5 marksifos-2010-subject-04-004

Let f be the Fermi-Dirac distribution function, then show that— (i) -\left(\dfrac{\partial f}{\partial E}\right) is a maximum at the Fermi level;

IFoS 2010Paper I20 marksifos-2010-subject-04-003

State Gibbs phase rule. Show that for a 1-component closed thermodynamic system having two phases, the condition for equilibrium between the phases is that their specific Gibbs functions are equal.

CSE 2009Paper I10 markscse-2009-subject-04-001

Derive an expression for the specific heat of a solid on the basis of Debye's model. Show that it converges to Dulong and Petit's law at high temperatures.

CSE 2009Paper I25 markscse-2009-subject-04-005

Energy distribution for n_i particles in classical statistical mechanics is given by n_i = g_i e^{-\alpha -\beta \varepsilon_i} where \alpha and \beta are constants. g_i is the single particle states in the i\text{ th} level. Using equipartition theorem, show that correct thermodynamic interpretation is \beta = \frac{1}{kT} (Use \int_0^\infty e^{-x} x^{1/2} \, dx = \frac{\sqrt{\pi}}{2} and \int_0^\infty e^{-\beta x} x^{3/2} \, dx = \frac{3\sqrt{\pi}}{4\beta^{5/2}})

CSE 2009Paper I20 markscse-2009-subject-04-004

Define entropy. How is it related to disorder? Hence, derive the Boltzmann relation S = k \log \Omega, where \Omega is the probability and k is the Boltzmann constant. Show that for any type of process, involving a closed system \Delta S \ge \frac{\Delta Q}{T} where the equality sign applies for internally reversible processes and the inequality for internally irreversible processes.

CSE 2009Paper I20 markscse-2009-subject-04-003

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