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A small block of mass mi is released from rest at the top of a curve-shaped, frictionless wedge which sits on a frictionless
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Answer #1

Solution:

Net External Force = Gravity in Y-Direcion

Total Momentum is conserved in X-Direction.

i.e., m_{1}v_{1} - m_{2}v_{2} = 0 ................. (Eq-1)

Total Mechanical Energy is Conserved.

i.e., m_{1}gh=\frac{1}{2} m_{1} v_{1}^{2} +\frac{1}{2} m_{2} v_{2}^{2} ------------- (Eq-2)

From Eq -1

v_{2} =\frac{m_{1}v_{1}}{m_{2}}

m_{1}gh=\frac{1}{2}m_{1} v_{1}^{2} + \frac{1}{2} \frac{m_{1}^{2} v_{1}^{2}}{m_{2}}

Therefore we get,

v_{1}^{2}= \frac{2gh}{1+\frac{m_{1}}{m_{2}}}

when v_{1}= 4m/s => 16 = \frac{2*10*5}{1+\frac{m_{1}}{m_{2}}}

\frac{m_{1}}{m_{2}}=5.25

Now When the mass is doubled, we get

\frac{m_{1}}{m_{2}}=10.50

v_{1}=\sqrt{\frac{2*10*5}{1+10.5}}=2.95 m/s

Therefore the 2.92 m/s is the speed when it leaves the wedge.

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