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Concepts Of Physics MCQ Edition [Volume 1]
Exam
Concepts Of Physics MCQ Edition [Volume 1]
Subject
Physics
Chapter
Centre of Mass, Linear momentum, Collision

Concepts Of Physics MCQ Edition [Volume 1] · Physics · Centre of Mass, Linear momentum, Collision

A small body of mass m is placed over a larger mass M whose surface...

A small body of mass mm is placed over a larger mass MM whose surface is horizontal near the small body and gradually curves to become vertical. The small body is pushed on the larger mass at a speed vv and the system is subsequently left to itself. Assume all surfaces are frictionless. Find the maximum height (measured from the ground) that the small body ascends.

Options

  1. AMv2g(M+m)\dfrac{Mv^2}{g(M + m)}
  2. Bmv22g(M+m)\dfrac{mv^2}{2g(M + m)}
  3. CMv22g(M+m)\dfrac{Mv^2}{2g(M + m)}
  4. D(M+m)v22gM\dfrac{(M+m)v^2}{2gM}

Correct answer

C. Mv22g(M+m)\dfrac{Mv^2}{2g(M + m)}

Step-by-step solution

Let the initial velocity of the small body of mass mm be vandthelargermassv and the larger massMbeatrest.<br><br>Sincethereisnoexternalforceactingonthesysteminthehorizontaldirection,thehorizontalcomponentofmomentumisconserved.<br><br>Atthemaximumheightbe at rest.<br><br>Since there is no external force acting on the system in the horizontal direction, the horizontal component of momentum is conserved.<br><br>At the maximum heighth,thesmallbodyisatrestrelativetothelargermass.Thus,bothmassesmovewiththesamehorizontalvelocity, the small body is at rest relative to the larger mass. Thus, both masses move with the same horizontal velocityV.<br><br>Applyingconservationoflinearmomentuminthehorizontaldirection:<br><br>.<br><br>Applying conservation of linear momentum in the horizontal direction:<br><br>mv = (M + m)V<br><br><br><br>V = \dfrac{mv}{M + m}<br><br>Applyingconservationofmechanicalenergyforthesystem:<br><br><br><br>Applying conservation of mechanical energy for the system:<br><br>\dfrac{1}{2}mv^2 = \dfrac{1}{2}(M + m)V^2 + mgh<br><br>Substitutingthevalueof<br><br>Substituting the value ofV:<br><br>:<br><br>\dfrac{1}{2}mv^2 = \dfrac{1}{2}(M + m)\left(\dfrac{mv}{M + m}\right)^2 + mgh<br><br><br><br>\dfrac{1}{2}mv^2 = \dfrac{m^2v^2}{2(M + m)} + mgh<br><br><br><br>mgh = \dfrac{1}{2}mv^2 - \dfrac{m^2v^2}{2(M + m)}<br><br><br><br>mgh = \dfrac{mv^2}{2} \left(1 - \dfrac{m}{M + m}\right)<br><br>mgh = mv22(M+m−mM+m)\dfrac{mv^2}{2}\left(\dfrac{M + m - m}{M + m}\right)

mgh=mMv22(M+m)mgh = \dfrac{mMv^2}{2(M + m)}

h=Mv22g(M+m)h = \dfrac{Mv^2}{2g(M + m)}
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