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Question: A small bucket of mass,\(M\) kg, is attached to a long inextensible cord of length \(L\) m. The buck...

A small bucket of mass,MM kg, is attached to a long inextensible cord of length LL m. The bucket is released from rest when the cord is in a horizontal position. At its lowest position, the bucket scoops up mm kg of water and swings upto a height hh. The height hh in meter is:
A.(MM+m)2L{{\left( \dfrac{M}{M+m} \right)}^{2}}L
B.(MM+m)L\left( \dfrac{M}{M+m} \right)L
C.(M+mM)2L{{\left( \dfrac{M+m}{M} \right)}^{2}}L
D.(M+mM)L\left( \dfrac{M+m}{M} \right)L

Explanation

Solution

in this question we are going to find the correct option. Here gravitational force or conservative force is applied means non-conservatives force not applied means mechanical energy is constant. Use formula vi+ki=vf+kf{{v}_{i}}+{{k}_{i}}={{v}_{f}}+{{k}_{f}} where vi{{v}_{i}} and vf{{v}_{f}} is initial and final potential energy and ki{{k}_{i}} and kf{{k}_{f}} is initial and final kinetic energy respectively to solve this problem.

Complete answer:
Let us first find out the speed of the bucket when it touches the water, that is, at the lowest point. We use law of conservation of energy, we have
vi+ki=vf+kf{{v}_{i}}+{{k}_{i}}={{v}_{f}}+{{k}_{f}}
MgL+12M(0)2=0+12Mv2\Rightarrow MgL+\dfrac{1}{2}M{{(0)}^{2}}=0+\dfrac{1}{2}M{{v}^{2}}
v{{v}^{'}} MgL=12Mv2 v=2gL \begin{aligned} & \Rightarrow MgL=\dfrac{1}{2}M{{v}^{2}} \\\ & \Rightarrow v=\sqrt{2gL} \\\ \end{aligned}
It is the lowest position of velocity of MM mass.
Suppose v{{v}^{'}} is the velocity of the bucket plus water system, as the bucket scoops up the water.
Now we apply the law of conservation of linear momentum . we have
M2gL=(M+m)v v=M2gLM+m \begin{aligned} & M\sqrt{2gL}=(M+m){{v}^{'}} \\\ & \Rightarrow {{v}^{'}}=\dfrac{M\sqrt{2gL}}{M+m} \\\ \end{aligned}
Now, we again use the law of conservation of energy. We have
vi+ki=vf+kf{{v}_{i}}+{{k}_{i}}={{v}_{f}}+{{k}_{f}}
0+12(M+m)v2=(M+m)gh+12(M+m)(0)2 12(M+m)v2=(M+m)gh v22=gh v2=2gh h=v22g........(2) \begin{aligned} & \Rightarrow 0+\dfrac{1}{2}(M+m){{v}^{'}}^{2}=(M+m)gh+\dfrac{1}{2}(M+m){{(0)}^{2}} \\\ & \Rightarrow \dfrac{1}{2}(M+m){{v}^{'}}^{2}=(M+m)gh \\\ & \Rightarrow \dfrac{{{v}^{'}}^{2}}{2}=gh \\\ & \Rightarrow {{v}^{'}}^{2}=2gh \\\ & \Rightarrow h=\dfrac{{{v}^{'}}^{2}}{2g}........(2) \\\ \end{aligned}
Now apply the value of v{{v}^{'}} in equation (2), we get
h=(M2gLM+m)22g h=M22gL(M+m)22g h=M2(M+m)2L h=(MM+m)2L \begin{aligned} & h=\dfrac{{{(\dfrac{M\sqrt{2gL}}{M+m})}^{2}}}{2g} \\\ & h=\dfrac{{{M}^{2}}2gL}{{{(M+m)}^{2}}2g} \\\ & h=\dfrac{{{M}^{2}}}{{{(M+m)}^{2}}}L \\\ & h={{(\dfrac{M}{M+m})}^{2}}L \\\ \end{aligned}
It is the height of the swing above the lowest position.

Hence, option A. (MM+m)2L{{\left( \dfrac{M}{M+m} \right)}^{2}}L is the correct answer.

Note:
An alternative approach to the question is: first use the law of conservative energy and find the velocity of lowest position, then again apply law of conservation when the bucket scoops up the water, and find velocity of mass. Then equating first and second, you will get the answer.