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321cse-2008-subject-03-006
CSE 2008Paper I20 Marks

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 ?

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322cse-2008-subject-03-008
CSE 2008Paper I10 Marks

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.

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323cse-2008-subject-03-011
CSE 2008Paper I30 Marks

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.

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324cse-2008-subject-03-009
CSE 2008Paper I15 Marks

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 ?

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325cse-2008-subject-03-007
CSE 2008Paper I10 Marks

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.

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326cse-2007-subject-03-003
CSE 2007Paper I20 Marks

Derive Poisson equation starting from the Coulomb's law for a set of point charges.

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327cse-2007-subject-03-001
CSE 2007Paper I20 Marks

What is a magnetic shell ? Define the strength of a magnetic shell. A 2\text{ mm} thick magnetic shell weighing 100\text{ gm} has magnetic moment of 1000\text{ units}. The density of the shell material is 10\text{ gm/cc}. Calculate the intensity of magnetisation and the strength of the shell.

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328cse-2007-subject-03-004
CSE 2007Paper I20 Marks

Obtain the solution of the Laplace equation in cylindrical coordinates.

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329cse-2007-subject-03-007
CSE 2007Paper I25 Marks

State Rayleigh-Jeans law. Show that the intensity of emissions at a particular wave-length is proportional to the temperature T. Discuss the limitations of this law in describing the intensity distribution of emission spectrum of a blackbody.

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330cse-2007-subject-03-008
CSE 2007Paper I40 Marks

Why does a spinning nucleus process in a magnetic field ? Explain the underlying principle of nuclear magnetic resonance (NMR) spectroscopy. Calculate the radio frequency at which NMR occurs in water kept in a uniform magnetic field of 2.4 T, the magnetic moment of proton being 2.793\\ \mu_N.

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331cse-2007-subject-03-006
CSE 2007Paper I20 Marks

State Amperes law of magnetostatics. Using this law, find the magnetic field at a point due to an infinitely long filamentary current.

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332cse-2007-subject-03-005
CSE 2007Paper I35 Marks

Explain the Rayleigh Scattering of light. Show that the energy density of light scattered from an isotropic homogenous medium of a gas is inversely proportional to the fourth power of the wavelength of the incident light.

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333cse-2007-subject-03-002
CSE 2007Paper I20 Marks

In an a.c. circuit, a resistance (R = 100\ \Omega) and a capacitance (C = 100\ \mu\text{F}) in series are connected to an a.c. source V = 200 \sin(100\ \pi t). Calculate the current through the circuit and the voltages across R and C. Draw a vector diagram representing the magnitudes and phases of the voltages.

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334cse-2006-subject-03-004
CSE 2006Paper I20 Marks

Find the magnetic field \vec{B} at the point P due to a short straight length of wire carrying current 'i'. Length of the wire is l. Point P is at a distance r away from the centre of the wire. Angle between \vec{l} and \vec{r} is \theta.

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335cse-2006-subject-03-007
CSE 2006Paper I20 Marks

What do you mean by a gauge transformation ? What is its importance ? Show that the Lorentz gauge condition \vec{\nabla} \cdot \vec{A} + \frac{1}{c} \frac{\partial \phi}{\partial t} = 0 is Lorentz invariant. Here \vec{A} and \phi are the vector and scalar potentials.

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336cse-2006-subject-03-006
CSE 2006Paper I20 Marks

Starting from Maxwell's equations of electromagnetic field in vacuum obtain the classical wave equations for the four field vectors \vec{E}, \vec{D}, \vec{B} and \vec{H} . Show that the field vectors can be propagated as waves in free space with the velocity of propagation equal to 3 \times 10^8\text{ m/s}, where for free space we have the vacuum permittivity \varepsilon_o = 8.854 \times 10^{-12}\text{ farad/m} & vaccum permeability \mu_o = 1.257 \times 10^{-6}\text{ henry/m}.

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337cse-2006-subject-03-005
CSE 2006Paper I20 Marks

Write down the different components of the electromagnetic field tensors F_{\mu\nu} and further prove that Maxwell's equations of electrodynamics are invariant to Lorentz transformations.

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338cse-2006-subject-03-010
CSE 2006Paper I30 Marks

In the case of proton NMR, state the expression for the energy of the dipole in an external magnetic field. How does the NMR originate ? Give the rough range of frequencies of the NMR signals, and the normal magnitude of the applied field.

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339cse-2006-subject-03-001
CSE 2006Paper I20 Marks

A potential in cylindrical coordinates is a function of r and \phi but not of z. Obtain the separated differential equations for R and \Phi, where V = R(r) \Phi(\phi) and solve them.

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340cse-2006-subject-03-009
CSE 2006Paper I20 Marks

Using Planck's radiation formula u(\nu) d\nu = \frac{8 \pi h}{c^3} \frac{\nu^3 d\nu}{e^{h\nu/kT} - 1} where the symbols have their usual meaning, find the wavelength of the region where energy density is the greatest. Also calculate the total energy density over all the frequencies

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