A small body of mass m is placed i the top of a hemispherical
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HEY MATE!.....
F = mgsinθ - N
When the ball loses contact, the normal force (N) = 0
=> F = mgsinθ
Since the ball is moving in a circular path, F = mv² / R
mgsinθ = mv² / R
=> v² = Rgsinθ
From conservation of energy, you know that:
mgR = ½mv² + mgh
Rg = ½Rgsinθ + gh
h = R - ½Rsinθ
If you draw out a force diagram you'll see that sinθ = h / R
h = R - ½Rh / R
3h/2 = R
h = 2R/3
So it will lose contact (2/3)rd of the way up.
it may be helps u
F = mgsinθ - N
When the ball loses contact, the normal force (N) = 0
=> F = mgsinθ
Since the ball is moving in a circular path, F = mv² / R
mgsinθ = mv² / R
=> v² = Rgsinθ
From conservation of energy, you know that:
mgR = ½mv² + mgh
Rg = ½Rgsinθ + gh
h = R - ½Rsinθ
If you draw out a force diagram you'll see that sinθ = h / R
h = R - ½Rh / R
3h/2 = R
h = 2R/3
So it will lose contact (2/3)rd of the way up.
it may be helps u
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