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Discuss the vibrational spectra of a diatomic molecule treating potential energy function as a representation of Hooke's law type of interaction.

IFoS 2013Paper II20 marksifos-2013-subject-06-003

Explain the concept of shared pair of electrons with antiparallel spins forming a covalent bond in \text{H}_2-like molecule with reference to total energy.

IFoS 2013Paper II8 marksifos-2013-subject-06-001

Explain why the separation between vibrational levels is smaller in an excited electronic state than in the ground electronic state.

IFoS 2013Paper II20 marksifos-2013-subject-06-004

A substance shows a Raman line at 4567\text{ \AA} when exciting line 4358\text{ \AA} is used. Estimate the positions of Stokes and anti-Stokes lines for the same substance when exciting line 4047\text{ \AA} is used.

IFoS 2013Paper II8 marksifos-2013-subject-06-002

The particle in a box has a ground state wave function given as \psi(x) = \frac{1}{\sqrt{l}} \cos \frac{\pi x}{2l} The box width is 2l and the particle is confined within (-l, +l). Calculate the expectation value of x^2.

IFoS 2013Paper II8 marksifos-2013-subject-05-003

(i) Enumerate the possible values of quantum numbers j and m_j for state in which l = 2 and s = 1/2.

(ii) Draw the corresponding vector model diagram.

IFoS 2013Paper II8 marksifos-2013-subject-05-002

Write down Schrödinger equations for a particle of energy E < V_0, incident on a step potential height V_0. Solve them to find out the transmission and reflection coefficients in terms of k and k', where k = \sqrt{\frac{2mE}{\hbar^2}} and k' = \sqrt{\frac{2m(V_0 - E)}{\hbar^2}}. Show that in this case, there is a finite probability of finding the particle in a classically forbidden region.

IFoS 2013Paper II35 marksifos-2013-subject-05-004

A particle is bound in a potential well given by V(x) = \begin{cases} \infty & \text{for } x \le 0 \\ cx & \text{for } x > 0 \end{cases} Estimate the ground state energy of the system from uncertainty principle.

IFoS 2013Paper II8 marksifos-2013-subject-05-001

Show that the spherical harmonics Y_{lm}(\theta, \phi) are simultaneous eigenfunctions of L^2, L_z and L_z^2. What are their corresponding eigenvalues?

IFoS 2013Paper II30 marksifos-2013-subject-05-005

Develop and write down the expressions of L^2, L_z and L_z^2 in angular momentum operator algebra.

IFoS 2013Paper II10 marksifos-2013-subject-05-006

State Dulong-Petit's law and discuss its limitations in explaining heat capacities of solids. How were these efficiencies overcome by Debye ?

IFoS 2013Paper I10 marksifos-2013-subject-04-005

What is transport phenomenon ? Obtain the expression for the coefficient of viscosity. Discuss its temperature dependence.

IFoS 2013Paper I20 marksifos-2013-subject-04-006

Discuss the significance of Saha's ionisation formula in classification of stars.

IFoS 2013Paper I10 marksifos-2013-subject-04-001

Calculate the net change in entropy when 10\text{ g} water at 60^\circ\text{C} is mixed with 30\text{ g} water at 20^\circ\text{C}.

IFoS 2013Paper I8 marksifos-2013-subject-04-002

Establish Van der Waals equation of state for a real gas. Deduce expressions for critical constants and show that critical coefficient is independent of the nature of gas.

IFoS 2013Paper I20 marksifos-2013-subject-04-004

For a completely degenerate BE gas, discuss the condition for onset of BE condensation.

IFoS 2013Paper I5 marksifos-2013-subject-04-003

What do you understand by the term polarization in dielectrics ? Obtain Clausius-Mossotti formula for linear dielectrics.

IFoS 2013Paper I20 marksifos-2013-subject-03-003

Using Poisson equation and spherical co-ordinates, calculate the density of continuous charge distribution that will provide the Yukawa potential \phi = \frac{\exp(-\alpha r)}{r}, where \alpha is a constant.

IFoS 2013Paper I8 marksifos-2013-subject-03-002

Sea water has resistivity 0\cdot 3\ \Omega\text{m} and its dielectric constant is 81. Calculate the ratio of the amplitudes of the conduction and polarisation current intensities when the applied field is oscillating at 100\text{ MHz}.

IFoS 2013Paper I8 marksifos-2013-subject-03-005

Define a black body. How can we realise a black body in practice ? Derive expression for Planck's radiation law.

IFoS 2013Paper I15 marksifos-2013-subject-03-008

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