Let \(\omega_{1},\omega_{2}\) and \(\omega_{3}\) be the angular speed of the second hand, minute hand, and hour hand of a smoothly running analog clock, respectively. If \(x_{1},x_{2}\) and \(x_{3}\) are their respective angular distance in \(1\) minute then the factor which remains constant \((k)\) is:
1. \(\frac{\omega_1}{x_1}\text=\frac{\omega_2}{x_2}\text=\frac{\omega_3}{x_3}\text={k}\)
2. \(\omega_{1}x_{1}\text=\omega_{2}x_{2}\text=\omega_{3}x_{3}\text={k}\)
3. \(\omega_{1}x_{1}^{2}\text=\omega_{2}x_{2}^{2}\text=\omega_{3}x_{3}^{2}\text={k}\)
4. \(\omega_{1}^{2}x_{1}\text=\omega_{2}^{2}x_{2}\text=\omega_{3}^{2}x_{3}\text={k}\)
Subtopic:  Rotational Motion: Kinematics |
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The angular acceleration of a body, moving along the circumference of a circle, is:
1. along the axis of rotation
2. along the radius, away from centre
3. along the radius towards the centre
4. along the tangent to its position
Subtopic:  Rotational Motion: Kinematics |
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A constant torque of \(100\) N-m turns a wheel of moment of inertia \(300\) kg-m2 about an axis passing through its centre. Starting from rest, its angular velocity after \(3\) s is: 
1. \(1\) rad/s 
2. \(5\) rad/s
3. \(10\) rad/s
4. \(15\) rad/s
Subtopic:  Rotational Motion: Kinematics |
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The angular speed of a flywheel moving with uniform angular acceleration changes from \(1200\) rpm to \(3120\) rpm in \(16\) s. The angular acceleration in rad/s² is:
1. \(104 \pi\)
2. \(2\pi\)
3. \(4\pi\)
4. \(12\pi\)
Subtopic:  Rotational Motion: Kinematics |
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The angular speed of the wheel of a vehicle is increased from \(360~\text{rpm}\) to \(1200~\text{rpm}\) in \(14\) seconds. Its angular acceleration will be:
1. \(2\pi ~\text{rad/s}^2\)
2. \(28\pi ~\text{rad/s}^2\)
3. \(120\pi ~\text{rad/s}^2\)
4. \(1 ~\text{rad/s}^2\)

Subtopic:  Rotational Motion: Kinematics |
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A particle starting from rest moves in a circle of radius \(r\). It attains a velocity of \(v_0~\text{m/s}\) on completion of \(n\) rounds. Its angular acceleration will be:
1. \( \dfrac{v_0}{n} ~\text{rad} / \text{s}^2\)
2. \( \dfrac{v_0^2}{2 \pi {nr}^2}~ \text{rad} / \text{s}^2 \)
3. \( \dfrac{v_0^2}{4 \pi {n}{r}^2}~ \text{rad} / \text{s}^2 \)
4. \( \dfrac{v_0^2}{4 \pi {nr}} ~\text{rad} / \text{s}^2 \)

Subtopic:  Rotational Motion: Kinematics |
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Three objects, A: (a solid sphere), B: (a thin circular disk) and C: (a circular ring), each have the same mass \(\mathrm{M}\) and radius \(\mathrm{R}.\) They all spin with the same angular speed about their own symmetry axes. The amount of work (\(\mathrm{W}\)) required to bring them to rest, would satisfy the relation:

1. \(\mathrm{W_C}>\mathrm{W_B}>\mathrm{W_A} ~~~~~~~~\)
2. \(\mathrm{W_A}>\mathrm{W_B}>\mathrm{W_C}\)
3. \(\mathrm{W_B}>\mathrm{W_A}>\mathrm{W_C}\)
4. \(\mathrm{W_A}>\mathrm{W_C}>\mathrm{W_B}\)

Subtopic:  Rotational Motion: Kinematics |
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A solid sphere of mass \(m\) and radius \(R\) is rotating about its diameter. A solid cylinder of the same mass and same radius is also rotating about its geometrical axis with an angular speed twice that of the sphere. The ratio of their kinetic energies of rotation (sphere/cylinder) will be:

1. \(2:3\) 2. \(1:5\)
3. \(1:4\) 4. \(3:1\)

Subtopic:  Rotational Motion: Kinematics |
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The instantaneous angular position of a point on a rotating wheel is given by the equation,
\(\theta(t)=2t^{3}-6t^{2}\)
The torque on the wheel becomes zero at:
1. \(t=0.5\) s 2. \(t=0.25\) s
3. \(t=2\) s 4. \(t=1\) s
Subtopic:  Rotational Motion: Kinematics |
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A wheel has an angular acceleration of \(3.0\) rad/s2 and an initial angular speed of \(2.0\) rad/s. In a time of \(2\) s, it has rotated through an angle (in radians) of:

1. \(6\) 2. \(10\)
3. \(12\) 4. \(4\)

Subtopic:  Rotational Motion: Kinematics |
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