Velocity of COM
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According to the principle of conservation of momentum
When no external torque acts on a system of particles, then the total angular momentum of the system always remains constant.
When no external torque acts on a system of particles, then the total angular momentum of the system always remains zero.
When an external torque acts on a system of particles, then the total angular momentum of the system always remains zero.
When an external torque acts on a system of particles, then the total angular momentum of the system always remains zero.
- m1m2m1+m2(v1−v2)2
- 12m1m2m1+m2(v1−v2)2
- 12m1m2m1+m2(v1+v2)2
- 12(m1m2)(v1−v2)2
A nucleus moving with a velocity →v emits anα-p article. Let the velocities of the α-particle and the remaining nucleus be →v1 and →v2 and their masses be m1, and m2.
, and must be parallel to each other.
+ must be parallel to .
None of the two of , and should be parallel to each other.
must be parallel to .
A block of mass m is pushed by applying a force F at an angle θ with the horizontal surface. The normal force on the block is given as -
F = mg
F = F sin θ
F = mg + F sin θ
F = mg - F sin θ
Two spheres of masses m1 and m2 (m1>m2) respectively are tied to the ends of a light, inextensible string which passes over a light frictionless pulley. When the masses are released from their initial state of rest, the acceleration of their centre of mass is: