Newton's Second Law: Rotatory Version
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The rotational analogue of force is :
- 1.5 s
- 2 s
- 0.5 s
- 1 s
- 2.5 s
A uniform solid cylinder of mass 'M' and radius 'R' is resting on a horizontal platform (which is parallel to X-Y plane) with its axis along the Y-axis and free to roll on the platform. The platform is given a motion in X-direction given by x=Acosωt. There is no slipping between the cylinder and the platform. The maximum torque acting on the cylinder as measured about its centre of mass is
- 12MRAω2
- mRAωA2cos2ωt
- MRAω2
- 2mRAω2
A hollow sphere of radius 'R' rests on a horizontal surface of finite coefficient of friction. A point object of mass 'm' moved horizontally and hits the sphere at a height of 'R/2' above its center. The collision is instantaneous and completely inelastic. Which of the following is/are correct ?
- Total linear momentum of the system is not conserved
- Total angular momentum about center of mass of the system remains conserved
The sphere gets finite angular velocity immediately after collision
The sphere moves with finite speed immediately after collision
- d→Ldt is perpendicular to →L at all times.
the magnitude of →L does change with time.
- →L does not change with time.
the component of →L in the direction of →A does change with time.
Which of the following quantities measured from different inertial reference frames are the same?
Force
Velocity
Displacement
Kinetic energy
A constant force 'F' is applied at the top of a ring as shown in figure. Mass of the ring is 'M' and radius is 'R'. Angular momentum of particle about point of contact at time 't' is
- Is Zero
- Decreases linearly with time
- Is constant
- Increases linearly with time
When you drop a ball you find that the ball accelerates towards the Earth due to the mutual gravitational force experienced. By Newton’s third law, the Earth also should experience an equal and opposite force. Why do we not see the Earth accelerating towards the ball?
- t=4mr2ωτ
- t=2m(r2+2a2)ωτ
- t=2m(a2+2r2)ωτ
- t=2ma2ωτ
- 2g2L
- 2gL
- 3g2L
- gL
- Zero
- Maybe Zero.
- Non-Zero
- None of these
Point P is →r away from O and a force →F is applied at P as shown.
What can be said about →T of →F about O ?
→T ⊥ →F and →T || →r
→T ⊥ →F and is directed outside the plane containing →T ⊥ →F and →r and →F
→T || →F and →T ⊥ →r
→T ⊥ →F and →T ⊥ →r
and is directed inside the plane containing →r and →F
- 2.5 rad/s2
- 5 rad/s2
- π rad/s2
- 10 rad/s2
If net external force on a body adds up to zero, which of the following statements are not necessarily true?
Net External torque about any point need not be zero
Linear acceleration of the centre of mass is zero
Angular acceleration of the body has to be zero
Angular momentum about any axis may not be conserved
If the line of action of the applied force intersects the Axis of rotation, then the torque of this force about the axis of rotation is
Always zero
Sometime non-zero
Always non-zero perpendicular to the axis of rotation
Non-zero and along the axis of rotation
- 5
- 10
- 15
- 20
The torque of force about a line is dependent of the choice of the origin which lies on that line itself.
False
True
Which of the following are the necessary and sufficient conditions for a body to have some angular acceleration about a fixed Axis?
Net external force is non-zero
Net external torque is non-zero
Net external torque is zero
Angular momentum is not conserved
Which of following rotational physical quantities do not match to given translational analogies?
Angular velocity-linear velocity
Angular displacement - linear displacement
Torque - Kinetic Energy
Moment of Inertia - mass
Which of the following cases, a rigid body, necessarily has an angular acceleration.
Line of action of force is parallel to Axis of rotation
Line of action of force is perpendicular to the axis of rotation
Line of action of the force is perpendicular and skew to the Axis of rotation
Line of action of the force intersects the axis of rotation
- 1:3
- 1:2
- 3:1
- 2:1