Two similar springs P and Q have spring constants KP and KQ, such that KP>KQ. They are stretched, first by the same amount (case a), then by the same force (case b). The work done by the springs WP and WQ are related as, in  case (a) and case (b), respectively

  • WP =WQ ;WP> WQ

  • WP =WQ ;WP= WQ

  • WP > WQ ;WQ> WP

  • WP > WQ ;WQ> WP


C.

WP > WQ ;WQ> WP

Given KP>KQ
In case (a) the elongation is same
 

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A block of mass 10 kg, moving in the x-direction with a constant speed of 10 ms-1 , is subjected to a retarding force F= 0.1x J/m during its travel from x = 20 m to 30 m. Its final KE will be

  • 475 J

  • 450 J

  • 275 J

  • 275 J


A.

475 J

From work energy theorem
work done = change in KE

⇒ W = Kf -Ki

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A body of mass (4m) is lying in x-y plane at rest. It suddenly explodes into three pieces. Two pieces each of mass m move perpendicular to each other with equal speed (v). The total kinetic energy generated due to explosion is,

  • mv2

  • 3 over 2 m v squared
  • 2mv2

  • 2mv2


B.

3 over 2 m v squared
As per the question, the third part of mass 2m will move because the total momentum of the system after explosion must remain zero.

Let the velocity of the third part be v'.

According to the law of conservation of momentum,


Total kinetic energy generated by the explosion,

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A car of mass m starts from rest and accelerates so that the instantaneous power delivered to the car has a constant magnitude Po. The instantaneous velocity of this car is proportional to

  • t2Po

  • t1/2

  • t-1/2

  • t-1/2


B.

t1/2

Power Po = Fv

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Two particles of masses m1,m2 move with initial velocities u1 and u2. On collision, one of the particles gets excited to a higher level, after absorbing energy (E). If final velocities of particles be v1 and v2, then we must have

  • straight m subscript 1 superscript 2 straight u subscript 1 space plus straight m subscript 2 superscript 2 straight u subscript 2 space minus straight epsilon space equals space straight m subscript 1 superscript 2 space straight v subscript 1 space plus straight m subscript 2 superscript 2 straight v subscript 2
  • 1 half m subscript 1 u subscript 1 superscript 2 space plus 1 half m subscript 2 u subscript 2 superscript 2 space equals space 1 half m subscript 1 v subscript 1 superscript 2 space plus 1 half m subscript 2 v subscript 2 superscript 2 minus epsilon
  • 1 half m subscript 1 u subscript 1 superscript 2 space plus 1 half m subscript 2 u subscript 2 superscript 2 space minus straight epsilon space equals space 1 half m subscript 1 v subscript 1 superscript 2 space plus 1 half m subscript 2 v subscript 2 superscript 2
  • 1 half m subscript 1 u subscript 1 superscript 2 space plus 1 half m subscript 2 u subscript 2 superscript 2 space minus straight epsilon space equals space 1 half m subscript 1 v subscript 1 superscript 2 space plus 1 half m subscript 2 v subscript 2 superscript 2


C.

1 half m subscript 1 u subscript 1 superscript 2 space plus 1 half m subscript 2 u subscript 2 superscript 2 space minus straight epsilon space equals space 1 half m subscript 1 v subscript 1 superscript 2 space plus 1 half m subscript 2 v subscript 2 superscript 2
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