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Employing NAND gates, design a half adder circuit which can add two bits A and B and provide a sum S and a carry C as its output.

IFoS 2010Paper II10 marksifos-2010-subject-08-007

Predict from the single particle shell model, the shell configuration, ground state spin and parity for the following nuclei : {}^7_3\text{Li}, \quad {}^{13}_7\text{N}, \quad {}^{17}_8\text{O}, \quad {}^{27}_{13}\text{Al}

IFoS 2010Paper II12 marksifos-2010-subject-07-004

What are magic numbers ? Discuss the shell structure of a nucleus. How is this model able to explain various properties of nuclei ? Discuss the limitations of this model.

IFoS 2010Paper II28 marksifos-2010-subject-07-003

A star converts all its hydrogen into helium, achieving 100\% helium. It then converts the helium into carbon via the reaction {}^4_2\text{He} + ^4_2\text{He} + ^4_2\text{He} \xrightarrow{\quad} ^{12}_6\text{C} + 7.27\text{ MeV} The mass of the star is 5.0 \times 10^{32}\text{ kg} and it generates energy at the rate of 5 \times 10^{30}\text{ W}. How long will it take to convert all helium to carbon at this rate ?

IFoS 2010Paper II10 marksifos-2010-subject-07-002

Calculate the binding energy per nucleus for {}^{87}_{38}\text{Sr}.

IFoS 2010Paper II10 marksifos-2010-subject-07-001

Write the quark composition of the following :

(i) Neutron

(ii) Proton

(iii) \Lambda

(iv) \text{K}^-

(v) \pi^+

IFoS 2010Paper II10 marksifos-2010-subject-07-005

What is Raman effect ? Discuss its application to molecular structure.

IFoS 2010Paper II10 marksifos-2010-subject-06-003

Derive the combined vibration–rotation spectrum of a diatomic molecule. What are P and R branches ?

IFoS 2010Paper II20 marksifos-2010-subject-06-005

Consider a diatomic molecule as a rigid rotator. Obtain its rotational energy levels and hence the rotational spectra.

IFoS 2010Paper II20 marksifos-2010-subject-06-004

Describe Stern–Gerlach experiment. In performing this experiment, beams of neutral atoms are used. Why are electrons or ion beams not used ? Explain how it demonstrates the discrete nature of the magnetic moment of an atom.

IFoS 2010Paper II20 marksifos-2010-subject-06-002

State and explain the Heisenberg's uncertainty principle. Show that the natural line width of a spectral line follows from this principle. The lifetime of an excited state of an atom is 10^{-8}\text{ s}. Calculate the energy width of such a state.

IFoS 2010Paper II10 marksifos-2010-subject-06-001

Set up a time-independent Schrödinger equation for a linear harmonic oscillator and obtain the energy eigen values. Explain the significance of zero point energy.

IFoS 2010Paper II20 marksifos-2010-subject-05-003

A stream of particles of mass M and energy E is directed from left to a one-dimensional potential well, as shown below :

Physics Diagram ifos-q-5-026-fig-1

The potential is -V_0 in the region a \ge x \ge -a and zero elsewhere. Set up a time-independent Schrödinger equation and obtain an expression for the transmission ratio from region I to II. Discuss the result. Show that there is a finite reflection from such a potential well, which is a result of the wave nature of matter.

IFoS 2010Paper II20 marksifos-2010-subject-05-002

Estimate the number of states lying in an energy interval of 0.03\text{ eV} above the Fermi level in a potassium crystal of unit volume. (E_F = 2.12\text{ eV} for potassium)

IFoS 2010Paper II10 marksifos-2010-subject-05-001

The electron spin operator \hat{s} can be expressed in matrix form in terms of the Pauli spin operator, \hat{\sigma} as \hat{\sigma} = 2\hat{s} where \sigma_x = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix}, \quad \sigma_y = \begin{pmatrix} 0 & -i \\ +i & 0 \end{pmatrix}, \quad \sigma_z = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix} Show that \sigma_x^2 = \sigma_y^2 = \sigma_z^2 = 1 \quad \text{and} \sigma_x \sigma_y = -\sigma_y \sigma_x = i \sigma_z \sigma_y \sigma_z = -\sigma_z \sigma_y = i \sigma_x \sigma_z \sigma_x = -\sigma_x \sigma_z = i \sigma_y

IFoS 2010Paper II10 marksifos-2010-subject-05-005

Set up the time-independent Schrödinger equation for an electron moving in a Coulomb field, V(r) = \frac{-ze^2}{4\pi\varepsilon_0 r}, in polar coordinates. Solve the radial equation to get the energy eigen values.

IFoS 2010Paper II20 marksifos-2010-subject-05-004

(ii) -\left(\dfrac{\partial f}{\partial E}\right) is symmetric about the Fermi level.

IFoS 2010Paper I5 marksifos-2010-subject-04-004

N particles are distributed among three states having energies E = 0, E = kT and E = 2kT. If the total equilibrium energy of the system is 1000 kT, what is the value of N?

IFoS 2010Paper I15 marksifos-2010-subject-04-001

Let f be the Fermi-Dirac distribution function, then show that— (i) -\left(\dfrac{\partial f}{\partial E}\right) is a maximum at the Fermi level;

IFoS 2010Paper I20 marksifos-2010-subject-04-003

Explain why the distribution of speeds of molecules emerging through a small hole in an effusive molecular beam source is not a Maxwellian distribution.

IFoS 2010Paper I5 marksifos-2010-subject-04-002

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