A rod of mass m and length l is kept on a smooth wedge of mass m
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We can use conservation of energy to solve this... or by using forces (normal) between wedge M and the rod m.
Here on the system of rod m and wedge M, work is done only by the gravitational force on rod m.
The PE lost by the rod : m g H
Wedge displaces horizontally by x. The rod displaces vertically by y.
=> y = x tanФ. Differentiate wrt time, to get:
=> v1 = v2 tanФ
=> a1 = a2 tanФ
When the rod touches the ground, velocity of wedge = v2.
KE of Wedge = 1/2 M v2²
KE of the rod = 1/2 m v1² = 1/2 m v2 tan²Ф
Using conservation of energy: m g H = 1/2 v2² (M + m tan²Ф)
v2² = 2 m g H /(M + m tan²Ф)
v_{wedge}=\sqrt{\frac{2mgH}{M+mtan^\phi}}vwedge=M+mtanϕ2mgH
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If we use the method of forces, then Normal reaction force N between the rod m and wedge M gives the acceleration to Wedge.
Draw the Free body diagram for wedge and the rod.
N SinФ = M a₂
m g - N CosФ = m a₁ = m a₂ tanФ
=> m g - M a₂ CotФ = m a₂ TanФ
=> a₂ = mg Tan Ф /(M+m tan²Ф )
Distance traveled by the wedge: H CotФ (the base of wedge)
=> v₂² = 2 a₂ H CotФ
Hence we get the same answer as above.
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