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1841ifos-2010-subject-02-004
IFOS 2010Paper I5 Marks

(i) Between multimode and single-mode fibers, explain critically how and why single-mode fiber is chosen for communication.

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1842ifos-2010-subject-02-005
IFOS 2010Paper I5 Marks

(ii) Why are the two wavelengths 1\cdot 30\ \mu\text{m} and 1\cdot 55\ \mu\text{m} important in single-mode fiber-optical communication system?

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1843ifos-2010-subject-02-006
IFOS 2010Paper I15 Marks

(i) What is birefringence? Indicate how it can be used to obtain plane and circularly polarized light.

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1844ifos-2010-subject-02-007
IFOS 2010Paper I10 Marks

(ii) A left circularly polarized beam of light having \lambda_0 = 5893\text{ \AA} is incident on a calcite crystal with its optic axis cut parallel to the surface. The crystal has thickness d = 0\cdot 005141\text{ mm}, n_o = 1\cdot 65836 and n_e = 1\cdot 48641 at this \lambda_0. What will be the state of polarization of the incident beam?

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1845ifos-2010-subject-02-010
IFOS 2010Paper I5+5=10 Marks

Consider a bare fiber having n_1 = 1\cdot 48 and n_2 = 1\text{ (air)}. Find out the NA. What is the maximum incident angle up to which light can be guided through the fiber?

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1846ifos-2010-subject-02-011
IFOS 2010Paper I5 Marks

Why is the NA of the single-mode optical fiber low as compared to multimode fiber?

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1847ifos-2010-subject-02-001
IFOS 2010Paper I6 Marks

(ii) Determine its quality factor Q and width of resonance \Delta f.

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1848cse-2010-subject-02-001
CSE 2010Paper I15 Marks

In the propagation of longitudinal waves in a fluid contained in an infinitely long tube of cross-section A, show that \rho=\rho_0\left(1-\frac{\partial\xi}{\partial x}\right) where, \rho_0 = equilibrium density \rho = density of the fluid in the disturbed state \frac{\partial\xi}{\partial x}=\text{volume strain}\quad\left(\left|\frac{\partial\xi}{\partial x}\right|\ll1\right)

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1849cse-2010-subject-01-005
CSE 2010Paper I10 Marks

What is the significance of the null result of Michelson-Morley experiment? Does it disprove the existence of ether? Justify.

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1850ifos-2010-subject-01-004
IFOS 2010Paper I5 Marks

(iii) Discuss the important role of Coriolis forces in the circulation pattern of winds.

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1851cse-2010-subject-01-004
CSE 2010Paper I10 Marks

When a sphere of radius r falls down a homogeneous viscous fluid of unlimited extent with the terminal velocity v, the retarding viscous force acting on the sphere depends on the coefficient of viscosity \eta, the radius r and its velocity v. Show how Stokes' law was arrived at connecting these quantities from the dimensional considerations.

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1852ifos-2010-subject-01-002
IFOS 2010Paper I10 Marks

How can one introduce the constraints of motion through the concept of generalized coordinate systems? Write down the set of transformation equations for a system of N particles relating the generalized coordinates with the real coordinates.

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1853cse-2010-subject-01-001
CSE 2010Paper I10 Marks

A planet revolves around the Sun in an elliptic orbit of eccentricity e. If T is the time period of the planet, find the time spent by the planet between the ends of the minor axis close to the Sun.

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1854ifos-2010-subject-01-006
IFOS 2010Paper I15 Marks

(i) For a particle of mass m moving with velocities \vec{v}_s and \vec{v}_r relative to the space and rotating axis, respectively, show that the equation of motion is obtained as \vec{F}-2m(\vec{\omega}\times\vec{v}_r)-m\vec{\omega}\times(\vec{\omega}\times\vec{r}) = m\vec{a}_r with \vec{\omega} and \vec{a}_r being the angular velocity and acceleration in rotating coordinates.

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1855ifos-2010-subject-01-008
IFOS 2010Paper I5 Marks

(ii) At what velocity, the electron momentum will be m_0 c?

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1856ifos-2010-subject-01-003
IFOS 2010Paper I5 Marks

(ii) Which term in the above equation represents the Coriolis force?

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1857ifos-2010-subject-01-001
IFOS 2010Paper I10 Marks

Establish the relation between the angular momentum and torque of a particle. Show that this relation leads one to the principle of conservation of angular momentum.

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1858cse-2010-subject-01-002
CSE 2010Paper I10 Marks

A uniform solid sphere of radius R having moment of inertia I about its diameter is melted to form a uniform disc of thickness t and radius r. The moment of inertia of the disc about an axis passing through its edge and perpendicular to the plane is also equal to I. Show that the radius r of the disc is given by r=\dfrac{2R}{\sqrt{15}}.

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1859cse-2010-subject-01-003
CSE 2010Paper I25 Marks

What are Eulerian angles? A body with rotational symmetry about an axis is rotating under gravity about a point on the axis without friction. What are the quantities remaining constant during the motion? Find them in terms of suitable Eulerian angles. Explain 'precession' and 'nutation' of such a body.

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1860ifos-2010-subject-01-007
IFOS 2010Paper I10 Marks

(i) An electron of rest mass m_0 moves with a velocity v such that its total energy is double of its rest mass energy. What is the electron velocity?

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