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System of Particles and Rotational Motion Test - 27

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System of Particles and Rotational Motion Test - 27
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  • Question 1
    1 / -0
    Four identical particles each of mass $$"m"$$ are arranged at the corners of a square of side length $$"L"$$. If one of the masses is doubled the shift in the centre of mass of the system w.r.t. diagonally opposite mass.
    Solution

  • Question 2
    1 / -0
    The momentum of a system is defined
    Solution
    $$v_{cm}=\dfrac{m_1v_1+m_2v_2+.....+m_nv_n }{m_1+m_2+m_3+.....+m_n}$$;

    $$\therefore {m_1+m_2+m_3+.....+m_n})v_{cm} =({m_1v_1+m_2v_2+.....+m_nv_n })$$;

    Option(A) is LHS of the above equation.
    Option(B) is RHS of the above equation.
    Hence, (A) and(B) are same.
    Option(C) is correct since momentum can be defined for a body having  translational motion, it may have additionally rotational and oscillatory motion.
  • Question 3
    1 / -0
    The point through which the total weight appears to act for any orientation of the object is ______.
    Solution
    the point where the total weight appears to act for any orientation of the object is centre of gravity .
  • Question 4
    1 / -0
    A uniform meter scale balances horizontally on a knife-edge placed at 55 cm mark, when a mass of 25 g is supported from one end, then the mass of the scale is :
    Solution
    Since the metre rule is uniform, the CM will be at the middle i.e. 50 cm. Then, mass of ruler $$(w)\times (55-50)=25(100-55)$$
    $$w=\dfrac {25\times 45}{5}=225 g$$
  • Question 5
    1 / -0
    A couple always tends to produce :
    Solution
    A couple has the force balanced and thus does not produce the acceleration. 
    Throgh they produce a torque causing rotational motion.

  • Question 6
    1 / -0
    The momentum of a system with respect to centre of mass-
    Solution
    For a  system, total momentum is always zero in the cm frame by definition since the momentum of the cm is zero in this frame.
  • Question 7
    1 / -0
    The center of mass of a system of particle is at the origin. it follows that :
    Solution
    The number of particle on both sides of the origin need not be same. For example, 1 particle of mass m at a distance of say 4 units towards the right of origin and 2 particles of equal mass m at a distance 8 units also have the center of mass at the origin.
    Thus A, B and C are incorrect.
    Also if a particle lies on positive X axis and two other particles are placed towards the left of the origin such that the three particles make an equilateral triangle, the center is again at origin.
    Thus option D is incorrect

  • Question 8
    1 / -0
    The diameter of a solid disc is $$0.5m$$ and its mass is $$16kg$$.
    What torque is required to increase its angular velocity about an axis perpendicular to its plane from zero to $$120$$ rotations/minute in $$8$$ seconds?
    Solution
    We have torque as $$\tau=I\alpha$$.
    Also the final angular velocity $$\omega$$ is given as 120 rotations/min or 2 rotations/second or $$4\pi$$ radians/sec.
    Thus we have $$\alpha$$ as $$\displaystyle\frac{4\pi-0}{8}=\displaystyle\frac{\pi}{2}rad/s^2$$
    And moment of inertia I for solid disc is $$\displaystyle\frac{mr^2}{2}$$
    Thus we get torque as
    $$\tau=(\displaystyle\frac{mr^2}{2}\times \displaystyle\frac{\pi}{2})$$
    Substituting the values we get-
    $$\tau=\displaystyle \frac{\pi}{4} N/m$$
  • Question 9
    1 / -0
    A ball kept in a closed container moves in it making collision with the walls. The container is kept on a smooth surface. The velocity of the centre of mass of :
    Solution
    Since the container is closed, the collisions made by ball  with the walls of container will not affect the mass of container and in turn there is no change in velocity of center of mass hence, both container and ball remain fixed.
  • Question 10
    1 / -0
    A car sometimes overturns while taking a turn. When it overturns, :
    Solution
    The inner wheels leave the ground first as the center of gravity is some height above ground it will experience outside pseudo force which result in slight raising of inner wheels using outer wheels as axis.
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