Answer:
(a)
P.E. of stone at the height \[y=mgy\]
When stone falls
through height \[y,\] then
Elastic
potential energy stored in the spring
\[=\frac{1}{2}k{{(y-L)}^{2}}=mgy\]
Using
the value of conservation of energy
\[\frac{1}{2}k{{(y-L)}^{2}}=mgy\]
or \[k{{(y-L)}^{2}}=mgy\]
or \[k{{(y-L)}^{2}}=2mgy\]
or \[k({{y}^{2}}+{{L}^{2}}-2yL)=2mgy\]
or \[k{{y}^{2}}-2y(kL+mg)+k{{L}^{2}}=0\]
\[\therefore
\] \[y=\frac{2(kL+mg)\pm \sqrt{4{{(kL+mg)}^{2}}-4{{k}^{2}}{{L}^{2}}}}{2k}\]
\[=\frac{(kL+mg)\pm
\sqrt{{{(kL+mg)}^{2}}-{{k}^{2}}{{L}^{2}}}}{k}\]
Since
\[y\] is positive, therefore,
\[y=\frac{(kL+mg)+\sqrt{{{(kL+mg)}^{2}}-{{k}^{2}}{{L}^{2}}}}{k}\]
(b)
Let \[x\] be the extension in the spring when stone drops, then at the equilibrium
position.
\[mg(L+x)=\frac{1}{2}m{{\upsilon
}^{2}}+k{{x}^{2}}\]
Also
\[mg=kx\] or \[x=\frac{mg}{k}\]
\[\therefore
\] \[mg\left( L+\frac{mg}{k} \right)=\frac{1}{2}m{{\upsilon
}^{2}}+\frac{1}{2}\frac{{{(mg)}^{2}}}{k}\]
or \[\frac{1}{2}m{{\upsilon
}^{2}}=mgL+\frac{{{(mg)}^{2}}}{k}-\frac{{{(mg)}^{2}}}{2k}\]
or \[\frac{1}{2}m{{\upsilon
}^{2}}=mgL+\frac{{{(mg)}^{2}}}{2k}\]
or \[\upsilon
=\sqrt{2gL+\frac{m{{g}^{2}}}{R}}\]
You need to login to perform this action.
You will be redirected in
3 sec