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Physics Test - 18

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Physics Test - 18
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  • Question 1
    1 / -0

    A particle of mass m is moving in a circular path of constant radius r such that its centripetal acceleration ac is varying with time t as ac=k2 rt2, where k is a constant. The power delivered to the particle by the force acting on it is

    Solution

    ac=k2 rt2

    orv2e=k2rt2

    or v = krt

    Therefore, tangential acceleration, at =dvdt= kr

    or Tangential force,

    Ft= mat= mkr

    Only tangential force does work.

    Power = Ft v = (mkr)(krt)

    or Power=mk2 r2 t

  • Question 2
    1 / -0

    A conducting wire frame is placed in a magnetic field, which is directed into the paper, figure. The magnetic field is increasing at a constant rate. The directions of induced current in wires AB and CD are

    Solution

    As the magnetic field directed into the paper is increasing at a constant rate, therefore, induced current should produce a magnetic field directed out of the paper. Thus current in both the loops must be anti-clock-wise.

    As area of loop on right side is more, therefore, induced emf on right side of loop will be more compared to the emf induced on the left-side of the loop
    e=dϕdt=-AdBdt

    Hence net current will flow from D to C and B to A

  • Question 3
    1 / -0

    An artificial satellite is moving in a circular orbit around the earth with a speed equal to half the magnitude of escape velocity from the earth. The height of satellite above the surface of earth is -(where R=radius of earth)

    Solution

    escape velocityVs=2GmR

    orbital velocityV0=Gmr

    givenV0=12Ve

    GmR+h=122GmR

    ⇒ R+h=2R or h=R

  • Question 4
    1 / -0

    A ball of mass m1 is moving with velocity 3v. It collides head on elastically with a stationary ball of mass m2. The velocity of both the balls become v after collision. Then the value of the ratiom2m1 is

    Solution

    3m1v = m1v + m2v

    3m1v − m1v = m2v

    2m1v = m2v

    m2m1=2

  • Question 5
    1 / -0

    The ratio of work done by an ideal monoatomic gas to the heat supplied to it in an isobaric process is

    Solution
    \(\eta=\frac{\mathrm{w}}{\mathrm{Q}}=\frac{\mathrm{R}}{\mathrm{Cp}}=\frac{\mathrm{R}}{\frac{5 \mathrm{R}}{2}}=\frac{2}{5}\)
  • Question 6
    1 / -0

    Figure shows a smooth inclined plane of inclination θ fixed in a car. A sphere is set in pure rolling on the incline. For what value of 'a' (the acceleration of car in horizontal direction) the sphere will continue pure rolling?

    Solution

    The sphere will continue pure rolling if

    ma cos θ = mg sin θ

    or a =g tan θ

  • Question 7
    1 / -0

    While using travelling microscope in an experiment one find that one main scale division length is 1 mm and 10 VSD = 9 MSD. When this microscope is focused over a glass slab which is placed over a spot. Then which of the reading is correctly written -

    Solution

    LC=1mm10=0.1 mm=0.01 cm

    ∴ Reading should be written upto 2 places after decimal (in cm)

  • Question 8
    1 / -0

    Two bodies of masses 10 kg and 100 kg are separated by a distance of 2 m. The gravitational potential at the mid-point of the line joining the two bodies is:

    Solution

    As we know, gravitational potential
    V=-GMR
    Gravitational potential at mid point,

    \(=-\frac{G \times 10}{1}-\frac{G \times 100}{1}=-110 G\)
    \(=-110 \times 6.67 \times 10^{-11} \mathrm{J} \mathrm{kg}^{-1}\)
    \(=-7.3 \times 10^{-9} \mathrm{J} \mathrm{kg}^{-1}\)
  • Question 9
    1 / -0

    A particle moves along x-axis as x=4(t−2)+a(t−2)2. Which of the following is true?

    Solution

    Given, x=4 (t−2)+a(t−2)2

    v=dxdt=4+2a(t−2)

    At t=0, v=4(1−a)

    Acceleration a=d2xdt2=2a

  • Question 10
    1 / -0

    A heavy uniform chain lies on horizontal table top. If the coefficient of friction between the chain and the table surface is 0.25, then the maximum fraction of the length of the chain that can hang over one edge of the table is

    Solution

    The force of friction on the chain lying on the table should be equal to the weight of the hanging chain. Let

    ρ= mass per unit length of the chain

    μ= coefficient of friction

    l= length of the total chain

    x= length of hanging chain

    Now, \(\mu(l-x) \rho g=x \rho g\) or \(\mu(l-x)=x\)
    \(\Rightarrow \mu l=(\mu+1) x\) or \(x=\frac{\mu l}{(\mu+1)}\)
    \(\therefore x=\frac{0.25 l}{(0.25+1)}=\frac{0.25 l}{1.25}=0.2 l\)
    \(\therefore \frac{x}{l}=0.2=20 \%\)
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