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1481ifos-2013-subject-05-004
IFOS 2013Paper II35 Marks

Write down Schr"{o}dinger 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.

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1482ifos-2013-subject-05-005
IFOS 2013Paper II30 Marks

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?

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1483cse-2013-subject-05-004
CSE 2013Paper II10 Marks

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1484ifos-2013-subject-05-002
IFOS 2013Paper II8 Marks

(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.

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1485cse-2013-subject-04-004
CSE 2013Paper I10 Marks

The coefficient of viscosity of helium at 27^\circ\mathrm{C} is 2 \times 10^{-5}\ \mathrm{kg\,m^{-1}\,s^{-1}}. Calculate \begin{qroman}\item the average speed and \item the diameter of a helium molecule,\end{qroman} if it is assumed that the gas obeys Maxwell-Boltzmann distribution. Given Boltzmann constant k_{\mathrm B} = 1.38 \times 10^{-23}\ \mathrm{J\,K^{-1}} and mass of helium atom = 6.67 \times 10^{-27}\ \mathrm{kg}.

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1486cse-2013-subject-04-005
CSE 2013Paper I10 Marks

N particles obeying Classical Statistics are distributed among three states having energies \varepsilon_1 = 0, \varepsilon_2 = k_{\mathrm B}T and \varepsilon_3 = 2k_{\mathrm B}T, where k_{\mathrm B} is Boltzmann constant. If the total equilibrium energy of the system is 1000k_{\mathrm B}T, calculate the value of N.

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1487ifos-2013-subject-04-001
IFOS 2013Paper I10 Marks

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

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1488ifos-2013-subject-04-003
IFOS 2013Paper I5 Marks

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

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1489cse-2013-subject-04-001
CSE 2013Paper I10 Marks

A thermally insulated ideal gas is compressed quasi-statically from an initial state with volume V_0 and pressure P_0 to a final state of volume V_f and pressure P_f. Show that the work done on the gas in the process is given by W=\frac{C_V}{R}\left(P_fV_f-P_0V_0\right) where C_V and R having standard meanings.

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1490ifos-2013-subject-04-006
IFOS 2013Paper I20 Marks

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

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1491ifos-2013-subject-04-004
IFOS 2013Paper I20 Marks

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.

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1492ifos-2013-subject-04-002
IFOS 2013Paper I8 Marks

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}.

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1493ifos-2013-subject-04-005
IFOS 2013Paper I10 Marks

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

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1494cse-2013-subject-04-003
CSE 2013Paper I15 Marks

In Leh, temperature of ice on a cold winter night is measured as -20^\circ\mathrm{C}. Calculate the change in entropy when 1\ \mathrm{kg} of ice is converted into steam at 100^\circ\mathrm{C}. Given specific heat capacity of ice is 500\ \mathrm{cal\,kg^{-1}\,K^{-1}}, latent heat of ice is 3.36\times10^5\ \mathrm{J\,kg^{-1}}, latent heat of steam is 2.26\times10^6\ \mathrm{J\,kg^{-1}} and J=4.2\ \mathrm{J\,cal^{-1}}.

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1495cse-2013-subject-04-002
CSE 2013Paper I15 Marks

The vapour pressure, in mm of Hg, of a substance in solid state is given by the relation \ln p=23.03-\dfrac{3754}{T}, where T is in Kelvin. The vapour pressure, in mm of Hg, of the substance in liquid state is given by the relation \ln p=19.49-\dfrac{3063}{T}. Calculate \begin{qroman}\item the coordinates of the triple point, and \item the latent heat of vaporisation at the triple point.\end{qroman} Take Gas constant R=8.314\ \mathrm{J\,mol^{-1}\,K^{-1}}.

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1496ifos-2013-subject-03-008
IFOS 2013Paper I15 Marks

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

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1497ifos-2013-subject-03-007
IFOS 2013Paper I8 Marks

Show that Wien's law and Stefan-Boltzmann law are limiting cases of Planck's radiation law.

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1498cse-2013-subject-03-008
CSE 2013Paper I15 Marks

(i) Considering an isotropic, linear, non-conducting, non-magnetic and inhomogeneous dielectric medium with \vec{D}=\epsilon\vec{E}=\epsilon_0n^2(x,y,z)\vec{E}, show that the electromagnetic wave equation for the field \vec{E} is given by \nabla^2\vec{E}+\vec{\nabla}\left(\frac{1}{n^2}\vec{\nabla}n^2\cdot\vec{E}\right)-\mu_0\varepsilon_0n^2\frac{\partial^2\vec{E}}{\partial t^2}=0. \setcounter{enumi}{1}

(ii) Write down the scalar equation for E_x from the above equation.

(iii) Interpret physically the situation if we move from homogeneous to an inhomogeneous medium.

(iv) Obtain the similar vector equation for the magnetic field \vec{H} in inhomogeneous medium.

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1499ifos-2013-subject-03-006
IFOS 2013Paper I8 Marks

A plane electromagnetic wave is given by E_z = a \cos \omega x \cos \omega t and H_y = - a \sin \omega x \sin \omega t. Evaluate the instantaneous value of the Poynting vector \vec{S} and show that <\vec{S}> = 0.

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1500ifos-2013-subject-03-005
IFOS 2013Paper I8 Marks

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}.

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