Angular Analogue of Linear Momentum
Trending Questions
- 2GMxR2[1x−1√R2+x2]
- 2GMxR2[1√R2+x2]
- GMxR2[1√R2+x2]
- GMxR2[1x−1√R2+x2]
Four identical solid spheres each of mass and radius are placed with their centres on the four corners of a square of side . The moment of inertia of the system about one side of square where the axis of rotation is parallel to the plane of the square is:
- angular momentum changes in direction but not in magnitude.
- angular momentumchanges both in direction and in magnitude.
- angular momentum is conserved.
- angular momentum changes in magnitude but not in direction.
A frame of reference that is accelerated with respect to an inertial frame of reference is called a non-inertial frame of reference. A coordinate system fixed on a circular disc rotating about a fixed axis with a constant angular velocity ω is an example of a non-inertial frame of reference. The relationship between the force →Frot experience by a particle of mass m moving on the rotating disc and the force →Fin experienced by the particle in an inertial frame of reference is
→Frot=→Fin+2m(→vrot×→ω)+m(→ω×→r)×→ω,
where →vrot is the velocity of the particle in the rotating frame of reference and →r is the position vector of the particle with respect to the centre of the disc. Now consider a smooth slot along a diameter of a disc of radius R rotating counterclockwise with a constant angular speed ω about its vertical axis through its center. We assign a coordinate system with the origin at the center of the disc, the x−axis along the slot, the y− axis perpendicular to the slot and the z− axis along the rotation axis →ω=ω→k. A small block of mass m is gently placed in the slot at →r=(R/2)→i at t=0 and is constrained to move only along the slot.
The distance r of the block at time t is
- R2cos2ωt
- R2cosωt
- R4(eωt+e−ωt)
- R4(e2ωt+e−2ωt)
A circular race track of radius 300 m is banked at an angle of 15 degrees. If the coefficient of friction between the wheels of a race car and the road is 0.2, what is the optimum speed of the race car to avoid wear and tear on its tires ?
Explain circular motion of car on a level road for 5 marks
The moment of inertia is constant, the time period is doubled, and what happens to the angular momentum of the body?
- is zero
- remains constant
- goes on increasing
- goes on decreasing
A body is moving in a low circular orbit about a planet of mass and radius . The radius of the orbit can be taken to be itself. Then the ratio of the speed of this body in the orbit to the escape velocity from the planet is:
- tan−1[gT22R]
- tan−1[2R2gT]
- tan−1[2Rg2π]
- tan−1[2RgT]
- mv2sin2θcosθ2g
- mv3sinθcosθg
- mv3sin2θcosθ2g
- mv3sin2θcosθg
- 3√24√3
- 5√2√3
- 4√35
- 4√25√5
- X-axis
- Y-axis
- Z-axis
- Line at equal angles to all the three axes
A flywheel of moment of inertia 5.0kg−m2 is rotated at a speed of 60rad/s. Because of the friction at the axle, it comes to rest in 5.0 minutes.
Find
(a) the average torque of the friction,
(b) the total work done by the friction and
(c) the angular momentum of the wheel 1 minute before it stops rotating.
- 12 kg m2/s
- 6 kg m2/s
- 8 kg m2/s
- 10 kg m2/s
A particle is projected at time t =0 from a point P with a speed v0 at an angle of 45∘ to the horizontal. Find the magnitude and the direction of the angular momentum of the particle about the point P at time t =v0g.