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System of Particles and Rotational Motion Test - 23

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System of Particles and Rotational Motion Test - 23
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  • Question 1
    1 / -0
    The kinetic energy of a moving body is given by $$K = 2v^{2}$$, $$K$$ being in joules and $$v$$ in m/s. Its momentum when traveling with a velocity of $$2\ ms^{-1}$$ will be :
    Solution
    $$K=\dfrac{1}{2}mv^{2}=2v^{2}$$
    $$\Rightarrow m=4kg$$
    $$\vec{p}=m.\vec{v}$$
        $$=4\times 2$$
        $$=8\ kg m/s$$
  • Question 2
    1 / -0
    A torque of $$0.5  Nm$$ is required to drive a screw into a wooden frame with the help of a screw driver. If one of the two forces of couple produced by screw driver is $$50  N$$, the width of the screw driver is:
    Solution
    Let width be $$x$$. So the torque due to couple is $$2\times50\times x/2=50x$$
    $$50x = 0.5\Rightarrow x=0.01m=1\ cm$$
  • Question 3
    1 / -0
    The position of axis of rotation of a body is changed so that its moment of inertia decreases by 36%. Find the % change in its radius of gyration.
    Solution
    $$\textbf{Step 1 - Finding relation between}$$ $$k_{1}\ and\ k_{2}$$
    We know  that $$I = mk^{2}$$
              Initially, $$I_{1} = mk_{1}^{2}$$
         and finally, $$I_{2} = mk_{2}^{2}$$
    given that initial moment of inertia decrease by $$36\%$$
    $$\therefore I_{2} = I_{1} - \dfrac {36}{100}I_{1}$$
    $$\Rightarrow I_{2} = 0.64 I_{1}$$
    $$\Rightarrow mk_{2}^{2} = 0.64\ mk_{1}^{2}$$
    $$\Rightarrow k_{2} = 0.8 k_{1}$$, so $$k_{1} > k_{2}$$

    $$\textbf{Step 2 - Calculating change in radius of gyration}$$
    Change in radius of gyration $$= \dfrac {k_{1} - k_{2}}{k_{1}}\times 100$$
                                                     $$= \dfrac {k_{1} - 0.8k_{1}}{k_{1}} \times 100$$
                                                     $$= 20$$

    Hence, the radius of gyration decreases by $$20\%$$
  • Question 4
    1 / -0
    The radius of gyration of a rotating metallic disc is independent of which of the following physical quantity.
    Solution
    $$I=mk^{2}$$
    $$k=\sqrt{\dfrac{T}{m}}$$
    $$I=\dfrac{mR^{2}}{2}$$
    $$k=\dfrac{R}{\sqrt{2}}$$
    $$\therefore r=R_{0} (1+ \alpha  \Delta T)$$
    $$\therefore$$ k is independent of mass.

  • Question 5
    1 / -0
    A wheel of radius $$R$$ is free to rotate about its natural axis and $$I$$ is its moment of inertia. If a tangential force $$F$$ is applied on the wheel along its rim, then angular acceleration of wheel is:
    Solution
    The torque is given using the relation
    $$\vec{\tau} = \vec{F} \times \vec{R}$$
    or
    $$\tau=I\alpha$$
    or
    $$\alpha=\dfrac{FR}{I}$$
  • Question 6
    1 / -0
    A flywheel making $$120$$ r.p.m is acted upon by a retarding torque producing angular retardation of $$\pi  \ rad/s^{2}$$. Time taken by it to come to rest is:
    Solution
    $$T=I  \alpha $$
    $$\omega =\dfrac{120\times 2\pi }{60}$$
    $$\omega =4\pi $$
    $$\omega =\omega _{0}+\alpha   t$$
    $$0=4\pi -\pi t$$
    $$t=4 s$$
  • Question 7
    1 / -0
    A brass disc is rotating about its axis. If temperature of the disc is increased then its:
    Solution
    Radius of gyration and
    moment of inertia will increase.
    $$\because I=mk^{2}$$
    $$k=\sqrt{\dfrac{I}{m}}$$
    $$I=\dfrac{mR^{2}}{2}$$
    $$k=\dfrac{R}{\sqrt{2}}$$
    $$A=A_{0}(1+ 2\alpha  \Delta T)  (eq^{n} $$ of thermal expansion)
    $$\pi r^{2}=\pi R_{0}^{2} (1+ 2\alpha \Delta T)$$
    $$r^{2}=R_{0}^{2} (1+ 2\alpha  \Delta T)$$
    $$\therefore$$ r will increase on increasing the temperature
    $$\therefore I\  and \ k$$ will increase on increasing the $$temperature$$


  • Question 8
    1 / -0
    Mass of thin long metal rod is 2 kg and its moment of inertia about an axis perpendicular to the length of rod and passing through its one end is $$0.5  kgm^{2}$$. Its radius of gyration is:
    Solution
    $$I= 0.5kgm^2$$
    m= 2kg
    K= radius of gyration

    $$2k^2= 0.5$$

    $$k^2= \sqrt{0\cdot 25}$$

    $$\therefore k =\sqrt{0.25} m = 50\: cm$$

  • Question 9
    1 / -0
    A wheel of moment of inertia $$5\times 10^{-3}kgm^{2}$$ is making $$20 \  rev/s$$. The torque required to stop it in $$10 \  s$$ is :
    Solution
    $$\omega =20\times 2\pi$$
    $$\tau = I\omega$$
    So, $$ \tau \Delta t=5\times 10^{-3}\omega$$
    $$\tau =\dfrac{5\times 10^{-3}\times 20\times 2\pi}{10}=2\pi\times 10^{-2} Nm$$
  • Question 10
    1 / -0
    Four point size bodies each of mass $$m$$ are fixed at four corners of a light square frame of side length $$L$$. The radius of gyration of these four bodies about an axis perpendicular to the plane of frame passing through its centre is:
    Solution
    $$I= 4\left (m \left (\dfrac{L}{\sqrt2}  \right )^2 \right )$$
    $$= 2mL^2$$
    So we have radius of gyration equivalence equation as,
    $$4mk^2= 2mL^2$$
    $$k= \dfrac{L}{\sqrt2} $$
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