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Show that for the one dimensional wave function \psi(x) = \begin{cases} \frac{1}{\sqrt{2a}} & , \quad |x| < a \\ 0 & , \quad |x| > a \end{cases} where a is a real constant, the rms uncertainty in momentum is infinite.

CSE 2008Paper II10 markscse-2008-subject-05-002

Explain the Debye model of specific heat of solids. What are its success and failures ?

CSE 2008Paper I10 markscse-2008-subject-04-006

Show that at T = 0, the Fermi distribution function has a value 1 for energies less than the Fermi energy \epsilon_F and is zero above it. For a system of non-interacting electrons at T = 0, show that the ground state energy of the system of N particles is \frac{3}{5} N \epsilon_F.

CSE 2008Paper I20 markscse-2008-subject-04-005

Consider N independent particles, each of which can be in either of two energy states +\epsilon and -\epsilon. Derive an expression for the entropy of a microcanonical ensemble for this system, where f = \sum_i \epsilon_i / N\epsilon is fixed, where \epsilon_i is the energy of the i-th particle.

CSE 2008Paper I10 markscse-2008-subject-04-004

State the law of equipartition of energy. Show how this law can be used to calculate specific heat of gases and hence find the ratio \gamma = C_p/C_v for diatomic and triatomic gases.

CSE 2008Paper I20 markscse-2008-subject-04-003

One mole of an ideal gas is compressed at constant temperature T from a volume V_1 to a volume V_2. Find the work done and heat absorbed by the gas. The gas now expands adiabatically to a volume 2V. Taking the gas to be diatomic, calculate the final temperature of the gas.

CSE 2008Paper I10 markscse-2008-subject-04-001

State second law of thermodynamics. Prove that no engine operating between two given temperatures is more efficient than a carnot engine operating between same two temperatures.

CSE 2008Paper I20 markscse-2008-subject-04-002

Explain how Maxwell modified Ampere's law of magnetostatics by introducing the concept of displacement current. How does it resolve the paradox of a charging capacitor ?

CSE 2008Paper I15 markscse-2008-subject-03-009

State Faraday's Law of induction in terms of emf and magnetic flux. Use Stoke's theorem to express the law in differential form. A uniform, time varying magnetic field \bar{B} = \bar{B}_0(1 + \alpha t)\hat{k} fills a circular region of radius R lying in the x-y plane with the centre at origin. Here \bar{B}_0 and \alpha are appropriately dimensioned constants. Find the induced electric field at a distance r from the centre where r < R.

CSE 2008Paper I10 markscse-2008-subject-03-008

Consider a plane electromagnetic wave entering a rarer medium from a denser medium. Show that the Brewster angle is less than the total internal reflection angle.

CSE 2008Paper I10 markscse-2008-subject-03-007

Show that the interaction energy of two magnetic dipoles \bar{m}_1 and \bar{m}_2 separated by a displacement \bar{r} is given by U = \frac{\mu_0}{4\pi} \cdot \frac{1}{r^3} \left[ \bar{m}_1 \cdot \bar{m}_2 - 3(\bar{m}_1 \cdot \hat{r})(\bar{m}_2 \cdot \hat{r}) \right]. If two magnetic dipoles are held at a fixed distance apart, but allowed to rotate freely, what would be the configuration for stable equilibrium ?

CSE 2008Paper I20 markscse-2008-subject-03-006

Find the vector potential due to a line segment from x = a to x = b carrying a current I at a point P which is at a distance d from the line segment.

CSE 2008Paper I20 markscse-2008-subject-03-005

State Gauss's Law of electrostatics both in integral form and differential forms. Two charged spheres of radius R each, have their centres a distance d apart such that d < 2R. One of the spheres has a uniform positive charge density \rho per unit volume while the other has opposite charge density -\rho. Show that the electric field in the region of overlap between two spheres is uniform.

CSE 2008Paper I20 markscse-2008-subject-03-004
Physics Diagram cse-q-3-238-fig-1

An infinite ladder network of resistances is connected across the points A and B, as shown in the above figure. Each of the resistance is 1\Omega. Calculate the effective resistance between points A and B.

CSE 2008Paper I10 markscse-2008-subject-03-003

A plane electromagnetic wave travelling in z-direction and polarized in x-direction is incident normally from left on to an interface between two media at z = 0. The medium to the left (z < 0) has a refractive index n_1, while that to the right is of refractive index n_2. The magnetic permeabilities of both the media are equal and \mu_1 = \mu_2 = \mu_0. Obtain expressions for reflection and transmission coefficients (R and T) and show that R + T = 1.

CSE 2008Paper I30 markscse-2008-subject-03-011

A point charge + q is held above a grounded conducting plane located at z = 0. If the position of the charge is (0, 0, d) obtain an expression for the induced charge density on the plane as a function of coordinates x and y.

CSE 2008Paper I10 markscse-2008-subject-03-002

Two identical black bodies A and B are respectively at temperatures T and 2T respectively. The heat energy radiated by A is collected for one minute and is used to heat a mass of water. The temperature of water is found to rise by 0.25 K. If the heat radiated by B were to be collected for one minute and used to heat the same mass of water, what would be the rise in the temperature of water ? Assume, specific heat of water to be temperature independent.

CSE 2008Paper I10 markscse-2008-subject-03-001

A plane electromagnetic wave is travelling in vacuum along a direction which makes an angle of 45^\circ each with the positive x and z-axes. The electric field at time t is given by the expression \bar{E} = E_0 (2 \cos \omega t \hat{j} - \sin \omega t (\hat{i} - \hat{k})) where \hat{i}, \hat{j} and \hat{k} are unit vectors along the x, y and z directions respectively and E_0 = 100 \text{ v/m}. Find the magnetic field vector \bar{B} at time t and obtain the average power transmitted per unit area by the wave.

CSE 2008Paper I15 markscse-2008-subject-03-010

Explain how inversion of population is achieved in a He-Ne laser.

CSE 2008Paper I10 markscse-2008-subject-02-005

Consider an ensemble of two-level atoms in thermal equilibrium. Show that the ratio of Einstein A and B coefficients is given by \frac{A}{B} = \frac{8\pi h \nu^3}{c^3}. Why is it not possible to achieve inversion of population in a two-level medium ?

CSE 2008Paper I20 markscse-2008-subject-02-006

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