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Compute the electrostatic energy of a conducting solid sphere of radius R and having total charge Q using the expression for the electrostatic energy in terms of the electric field \bar{E} of the above sphere.

IFoS 2014Paper I8 marksifos-2014-subject-03-003

Prove Stefan's law of radiation from thermodynamic considerations.

IFoS 2014Paper I8 marksifos-2014-subject-03-001

State and explain Stefan-Boltzmann Law. Show that \log P = \log K + 4\log R, where P is the power emitted by black body and R is the resistance of the black body, K is a constant.

CSE 2014Paper I10 markscse-2014-subject-03-007

Show that the energy flow due to a plane electromagnetic wave propagating along z-direction in a dielectric medium is given by \hat{z}\frac{k}{\omega\mu}E_0^2\cos^2(kz-\omega t), where \mathbf{k} and \omega are the propagation vector and angular frequency, E_0 is electric field amplitude, \mu is the relative permeability of the medium.

CSE 2014Paper I10 markscse-2014-subject-03-006

Starting from Maxwell's equation, obtain the wave equation for the electric field \vec{E} in free space and appropriate wave equation for the electric field \vec{E}=E_z(x,y,z)\hat{z}.

CSE 2014Paper I10 markscse-2014-subject-03-005

When connected in series, L_1, C_1 have the same resonant frequency as L_2, C_2 also connected in series. Prove that if all these circuit elements are connected in series, the new circuit will have the same resonant frequency as either of the circuits first mentioned.

CSE 2014Paper I15 markscse-2014-subject-03-004

Using Ampere's Law and continuity equation, show that the divergence of the total current density is zero.

CSE 2014Paper I15 markscse-2014-subject-03-003

For initial current conditions I=I_0 and \frac{dI}{dt}=0 at t=0, show that the time dependent current in the critical damping case for an LCR circuit is given by I=I_0\left(1+\frac{\gamma t}{2}\right)e^{-\gamma t/2} where \gamma=\frac{R}{L}, \omega_0^2=\frac{1}{LC}, \omega=\sqrt{\omega_0^2-\frac{\gamma^2}{4}} and \tan\delta=\frac{-\gamma}{2\omega}.

CSE 2014Paper I20 markscse-2014-subject-03-002

In deriving radiation laws, we consider a cubical container of volume V containing a photon gas in equilibrium. Calculate the differential number of allowed normal modes of frequency \omega.

CSE 2014Paper I10 markscse-2014-subject-03-001

How does the population inversion in an active medium lead to the amplification of light in a laser ? Explain in details.

IFoS 2014Paper I10 marksifos-2014-subject-02-005

What are the step index and graded index optical fibers ? What are the conventional optical windows for light propagation through optical fibers ?

IFoS 2014Paper I15 marksifos-2014-subject-02-006

A left circularly polarized beam (\lambda = 5893^\circ\text{A}) is incident normally on a calcite crystal (with its optic axis cut parallel to the surface) of thickness 0.005141\text{ mm}. What will be the state of polarization of the emergent beam ? Justify your answer. Here the refractive indices for the ordinary and the extraordinary rays are 1.65836 and 1.48641 respectively.

IFoS 2014Paper I8 marksifos-2014-subject-02-004

Draw a neat diagram to show how light propagates through a graded index optical fiber from the entrance to the fiber end and explain.

IFoS 2014Paper I10 marksifos-2014-subject-02-007

Explain how you can construct a zone plate from Fresnel's half period zone. Show that a zone plate has multiple foci.

IFoS 2014Paper I15 marksifos-2014-subject-02-002

Write down the mathematical representation of Fermat's principle and explain all the notations used. With the help of a neat diagram, show that this principle can be used to obtain the law of refraction : n_1 \sin \theta_1 = n_2 \sin \theta_2 , where n_1 and n_2 are the refractive indices of the two media while \theta_1 and \theta_2 are the angles of incidence and refraction of the light beam.

IFoS 2014Paper I8 marksifos-2014-subject-02-003

Starting with the rate equations for matter-radiation interaction, show that the ratio of the Einstein's A and B coefficients is proportional to the third power of the frequency of radiation.

IFoS 2014Paper I15 marksifos-2014-subject-02-008

If the system matrix for a thin lens of focal length f is given by : S = \begin{bmatrix} 1 & -1/f \\ 0 & 1 \end{bmatrix} , show that the system matrix for a combination of two thin lenses of focal lengths f_1 and f_2 separated by a distance d can be obtained as S_{12} = \begin{bmatrix} 1 - d/f_2 & -(1/f_1 + 1/f_2 - d/f_1 f_2) \\ d & 1 - d/f_1 \end{bmatrix}

IFoS 2014Paper I8 marksifos-2014-subject-02-001

How does holography differ from conventional photography? What are the requirements for the formation and reading of a hologram?

CSE 2014Paper I10 markscse-2014-subject-02-008

Explain the working principle of a 3-level laser with a specific example. Comment on why the third level is needed.

CSE 2014Paper I10 markscse-2014-subject-02-007

For a multimode step index optical fibre, the core refractive index is 1.5 and fractional index difference is 0.001. Calculate the pulse broadening for 1\,\mathrm{km} length of the fibre. Over a length of 2\,\mathrm{km} of the fibre, calculate the minimum pulse separation that can be transmitted without overlap.

CSE 2014Paper I10 markscse-2014-subject-02-006

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