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Physics Test - 11

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Physics Test - 11
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  • Question 1
    1 / -0

    Two blocks of masses m1 = m and m2 = 2m are connected by a light string passing over a frictionless pulley. The mass m1 is placed on a smooth inclined plane of inclination θ= 30o and mass m2 hangs vertically as shown in the figure.

    If the system is released, the blocks move with an acceleration equal to:

     

    Solution
    the equation of the block are
    \(T-m_{1} g \sin \theta=m_{1} a \ldots \ldots\)(1)
    \(m_{2} g-T=m_{2} a \ldots \ldots \ldots\)(2)
    Equation (1) and (2)
    \(a=\frac{\left(m_{2}-m_{1} \sin \theta\right) g}{\left(m_{1}+m_{2}\right)}\)
    \(=\frac{\left(2 m-m \times \sin 30^{\circ}\right) g}{(m+2 m)}\)
    \(=\frac{g}{2}\)
    Hence the correct option is \(C\)
  • Question 2
    1 / -0
    Water is falling on the blades of a turbine at the rate of 6000 kg/min. The height of the fall is 100 m. The power given to the turbine is (Take g = 10 m/s2)
    Solution
    Mass of water falling on the turbine, \(m=6 \times 10^{3} \mathrm{kg}\)
    Rate at which the water is flowing, \(t=1 \min =60\) s
    Height of the fall, \(h=100 \mathrm{m}, g=10 \mathrm{m} / \mathrm{s}^{2}\)
    So, power given to the turbine, \(P=\frac{\text { Work done }}{\text { time taken }}\)
    \(=\frac{m g h}{t}=\frac{6 \times 10^{3} \times 10 \times 100}{60}=10^{5} W=100 \mathrm{kW}\)
  • Question 3
    1 / -0
    A small ball is pushed from a height 'h' along a smooth hemispherical bowl. With what speed should the ball be pushed, so that it just reaches the top of the opposite end of the bowl? (The height of the top of the bowl is R.)
    Solution
    when the ball \(n\) at height \(h\) the \(P . E_{1}\) of the ball in \(m g h\)
    when the ball is pushed with velocity \(v\) it reaches
    The bottom with \(K . E_{1}=\frac{1}{2} m v^{2}\)
    Thus by inertia the ball Travel upto \(R\) when its
    \(P . E_{2}=m g R\) and velocity \(=0\)
    \(K \cdot E_{2}=0\)
    \(\therefore\) From low of conservation of energy
    \(P E_{1}+K E_{1}=P E_{2}+K E_{2}\)
    \(m g h+\frac{1}{2} m v^{2}=m g R+0\)
    so \(\therefore v=\sqrt{2 g(R-h)}\)
  • Question 4
    1 / -0

    A body of mass m accelerates uniformly from rest to v1​ in time t1​ . As a function of t, the instantaneous power delivered to the body is:

    Solution
    From \(v=u+a t, v_{1}=0+a t_{1}\)
    \(\therefore a=\frac{v_{1}}{t_{1}}\)
    \(F=m a=m v_{1} / t_{1}\)
    Velocity acquired in \(\mathrm{t} \mathrm{sec}=a t=\frac{v_{1}}{t_{1}} t\)
    Power\(=F \times v=\frac{m v_{1}}{t_{1}} \times \frac{v_{1} t}{t_{1}}=\frac{m v_{1}^{2} t}{t_{1}^{2}}\)
  • Question 5
    1 / -0
    A ball P of mass 2 kg undergoes an elastic collision with another ball Q at rest. After the collision, ball P continues to move in its original direction with a speed one-fourth of its original speed. What is the mass of ball Q?
    Solution
    By conservation of linear momentum
    \(2 v_{0}=2\left(\frac{v_{0}}{4}\right)+m v \Rightarrow 2 v_{0}=\frac{v_{0}}{2}+m v \Rightarrow \frac{3 v_{0}}{2}=m v \ldots\)
    since collision is elastic
    \(v_{\text {separation }}=v_{\text {approach }} \Rightarrow v-\frac{v_{0}}{4}=v_{0} \Rightarrow \frac{5 v_{0}}{4}=v \ldots .(2)\)
    equating (2) and (1)
    \(\frac{3 v_{0}}{4}=m\left(\frac{5 v_{0}}{4}\right) \Rightarrow m=\frac{6}{5}=1.2 \mathrm{kg}\)
  • Question 6
    1 / -0
    The pressure and density of a diatomic gas \(\left(\gamma=\frac{7}{5}\right)\) change adiabatically from \(\left(\mathrm{P}_{1}, \rho_{1}\right)\) to \(\left(\mathrm{P}_{2}, \rho_{2}\right)\). If \(\frac{\rho_{2}}{\rho_{1}}=32\), then what should be the value of \(\frac{\mathrm{P}_{2}}{\mathrm{P}_{1}}\) ?
    Solution
    For an adiabatic process.
    \(P V^{\gamma}=\) constant
    \(P \rho^{-\gamma}=\) constant
    \(\frac{P_{2}}{P_{1}}=\left(\frac{\rho_{1}}{\rho_{2}}\right)^{-\gamma}=\left(\frac{1}{32}\right)^{-7 / 5}=(32)^{7 / 5}=128\)
  • Question 7
    1 / -0
    Kepler's second law states that the straight line joining a planet to the sun sweeps out equal areas in equal time. This statement is equivalent to the statement that
    Solution
    Velocity of particle accelerating uniformly in time \(t_{1}\)
    \(v=a t_{1}\)
    \(a=\frac{v}{t_{1}}\)
    Velocity of particle in time \(t\)
    \(v^{\prime}=a t=\frac{v t}{t_{1}}\)
    According to work-energy theorem, work done = change in kinetic energy i.e., \(\quad W_{\mathrm{ext}}=\Delta K\) or \(W_{\text {ext }}=\frac{1}{2} m v^{2}-0\)
    \(=\frac{1}{2} m\left(\frac{v t}{t_{1}}\right)^{2}\)
    \(=\frac{1}{2} \frac{m v^{2}}{t_{1}^{2}} t^{2}\)
  • Question 8
    1 / -0
    Two bodies A and B have masses 'M' and 'm' respectively, where M > m, and they are at a distance 'd' apart. Equal forces are applied to them so that they approach each other. The position where they hit each other is
    Solution
    since the collision is elastic, both momentum and kinetic energy are conserved. If \(m\) is mass of ball \(\) and v' its speed after the collision, the law of conservation of momentum gives
    \(2 v=2 \times \frac{v}{4}+m v^{\prime}\)
    where \(v\) is the original speed of ball \(P\). Thus
    \(m v^{\prime}=\frac{3 v}{2}\) or \(v^{\prime}=\frac{3 v}{2 m}\)
    The law of conservation of energy gives
    \(\frac{1}{2} \times 2 \times v^{2}=\frac{1}{2} \times 2 \times\left(\frac{v}{4}\right)^{2}+\frac{1}{2} m v^{\prime 2}\)
    or \(m v^{2}=\frac{15 v^{2}}{8}\)
    Using
    (i) in (ii) we get \(m=1.2 \mathrm{kg}\)
  • Question 9
    1 / -0
    Two satellites of Earth, S1 and S2, are moving in the same orbit. The mass of S1 is four times the mass of S2. Which of the following statements is true?
    Solution

    W = F.s = (ma).s

    \(W=m \frac{v}{t} s=m \frac{8}{t^{2}} s=m \frac{s^{2}}{t^{2}} \quad\) (where \(m\) is the mass, \(s\) is the displacement and \(t\) is the time)

    Now, mass, length and time are doubled. \(\mathrm{SO}_{\text {, }}\)

    \(\mathrm{W}^{\prime}=2 \mathrm{m} \frac{4 \mathrm{s}^{2}}{4 t^{2}}=2 \mathrm{m} \frac{\mathrm{s}^{2}}{\mathrm{t}^{2}}=2 \mathrm{W}\)

  • Question 10
    1 / -0

    The mass of the moon is \(\frac{1}{12} \mathrm{M}_{\mathrm{e}}\). If the acceleration due to gravity on the moon is \(\frac{\mathrm{g}}{6},\) then its radius is

    Solution
    The total energy \(=\mathrm{KE}+\mathrm{PE}\) remains constant during the free fall, i.e.
    \[
    \begin{aligned}
    m g h+\frac{1}{2} & m v^{2}=\mathrm{constant} \\
    g h+\frac{v^{2}}{2} &=\mathrm{constant}
    \end{aligned}
    \]
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