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Systems of Particles and Rotational Motion Test - 79

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Systems of Particles and Rotational Motion Test - 79
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  • Question 1
    4 / -1
    Three masses of 2 kg, 4 kg and 4 kg are placed at the three points ( 1, 0, 0), (1, 1, 0) and (0, 1, 0) respectively. The position vector of its centre of mass is
    Solution

  • Question 2
    4 / -1
    A man of 50 kg mass it standing in gravity free space at a height of 10 m above the floor. He throws a stone of 0.5 kg mass downwards with a speed of 2 m/s. When the stone reached the floor, the distance of the man above the floor will be
    Solution

  • Question 3
    4 / -1

    Solution

  • Question 4
    4 / -1
    Two persons of masses 55 kg and 65 kg respectively, are at the opposite ends of a boat. The length of the boat is 3.0 m and weight 100 kg. The 55 kg man walks up to the 65 kg man and sits with him. If the boat is in still water the centre of mass of the system shifts by
    Solution

  • Question 5
    4 / -1
    In a bicycle the radius of rear wheel is twice the radius of front wheel. If rF and rr are the radius, vF and vr are speeds of top most points of wheel, then
  • Question 6
    4 / -1
    A wheel is rolling along the ground with a speed of 2 ms–1. The magnitude of the velocity of the points at the extremities of the horizontal diameter of the wheel is equal to
    Solution

  • Question 7
    4 / -1
    A point P on the rim of wheel is initially at rest and in contact with the ground. Find the displacement of the point P if the radius of the wheel is 5 m and the wheel rolls forward through half a revolution
    Solution

  • Question 8
    4 / -1
    A wheel has angular acceleration of 3.0 rad/sec2 and an initial angular speed of 2.00 rad/sec. In a time of 2 sec it has rotated through an angle (In radian) of
    Solution

  • Question 9
    4 / -1
    When a ceiling fan is switched on, it makes 10 revolutions in the first 3 seconds. Assuming a uniform angular acceleration, how many rotations it will make in the next 3 seconds?
    Solution

  • Question 10
    4 / -1
    The general motion of a rigid body can be considered to be a combination of (i) a motion of its centre of mass about an axis, and (ii) its motion about an instantaneous axis passing through the centre of mass.
    These axes need not be stationary. Consider, for example, a thin uniform disc welded (rigidly fixed) horizontally at its rim to a massless stick, as shown in the figure.
    When the disc-stick system is rotated about the origin on a horizontal frictionless plane with angular speed co, the motion at any instant can be taken as a combination of (i) a rotation of the centre of mass of the disc about the z-axis, and (ii) a rotation of the disc through an instantaneous vertical axis passing through its centre of mass (as is seen from the changed orientation of points P and Q).
    Both these motions have the same angular speed ω this case.

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