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Question: A spring whose stretched length is \(l\) has a force constant \(k\). The spring is cut into two piec...

A spring whose stretched length is ll has a force constant kk. The spring is cut into two pieces of unstretched lengths l1{l_1} and l2{l_2} where l1=nl2{l_1} = n{l_2} and nn is an integer. The ratio k1k2\dfrac{{{k_1}}}{{{k_2}}} of the corresponding force constants, k1{k_1} and k2{k_2} will be:
A. 1n2\dfrac{1}{{{n^2}}}
B. n2{n^2}
C. 1n\dfrac{1}{n}
D. nn

Explanation

Solution

The spring is divided into two components. The lengths of these components are l1{l_1} and l2{l_2}. The force constant kk is proportional to the length ll of the wire. Now, k1{k_1} and k2{k_2} are the force constant of lengths l1{l_1} and l2{l_2} respectively.

Complete step by step answer:
As given in the question, a spring of length ll is divided into two pieces of lengths l1{l_1} and l2{l_2} , therefore, we can say,
l1+l2=l{l_1} + {l_2} = l
Now, kk is the force constant and is given by
k1lk \propto \,\dfrac{1}{l}
k=Cl\Rightarrow \,k = \dfrac{C}{l}
Here, CC is the constant of proportionality and ll is the length of the wire.
Now, as the spring is divided into two parts of lengths l1{l_1} and l2{l_2}.

Therefore, the force constant of the spring having length l1{l_1} is given by
k1=Cl1{k_1} = \dfrac{C}{{{l_1}}}
Also. The force constant of the spring having length l2{l_2} is given by
k2=Cl2{k_2} = \dfrac{C}{{{l_2}}}
Now, dividing k1{k_1} by kk , we get
k1k=cl1cl2\dfrac{{{k_1}}}{k} = \dfrac{{\dfrac{c}{{{l_1}}}}}{{\dfrac{c}{{{l_2}}}}}
k1k=cl1×lc\Rightarrow \,\dfrac{{{k_1}}}{{{k_{}}}} = \dfrac{c}{{{l_1}}} \times \dfrac{l}{c}
k1k=ll1\Rightarrow \,\dfrac{{{k_1}}}{{{k_{}}}} = \dfrac{l}{{{l_1}}}
k1k=l1+l2l1\Rightarrow \,\dfrac{{{k_1}}}{k} = \dfrac{{{l_1} + {l_2}}}{{{l_1}}}
k1k2=1+l2l1\Rightarrow \,\dfrac{{{k_1}}}{{{k_2}}} = 1 + \dfrac{{{l_2}}}{{{l_1}}}
Now, it is given in the question that
l1=nl2{l_1} = n{l_2}
l1l2=n\Rightarrow \,\dfrac{{{l_1}}}{{{l_2}}} = n
Putting the value of l1l2\dfrac{{{l_1}}}{{{l_2}}} in the above equation, we get
k1k2=1+1n=n+1n\Rightarrow \,\dfrac{{{k_1}}}{{{k_2}}} = 1 + \dfrac{1}{n} = \dfrac{{n + 1}}{n}

Now, dividing k2{k_2} by k{k_{}}, we get
k2k=cl2cl\dfrac{{{k_2}}}{k} = \dfrac{{\dfrac{c}{{{l_2}}}}}{{\dfrac{c}{l}}}
k2k=cl2×lc\Rightarrow \,\dfrac{{{k_2}}}{k} = \dfrac{c}{{{l_2}}} \times \dfrac{l}{c}
k2k=ll2\Rightarrow \,\dfrac{{{k_2}}}{k} = \dfrac{l}{{{l_2}}}
k2k=l1+l2l2\Rightarrow \,\dfrac{{{k_2}}}{k} = \dfrac{{{l_1} + {l_2}}}{{{l_2}}}
k2k=l1l2+1\Rightarrow \,\dfrac{{{k_2}}}{k} = \dfrac{{{l_1}}}{{{l_2}}} + 1
Putting, the value of l1l2\dfrac{{{l_1}}}{{{l_2}}} in the above equation, we get
k2k=n+1\Rightarrow \,\dfrac{{{k_2}}}{k} = n + 1
Now, the ratio k1k2\dfrac{{{k_1}}}{{{k_2}}} can be calculated by dividing k1k\dfrac{{{k_1}}}{k} and k2k\dfrac{{{k_2}}}{k} as shown below
k1k2=k1kk2k\dfrac{{{k_1}}}{{{k_2}}} = \dfrac{{\dfrac{{{k_1}}}{k}}}{{\dfrac{{{k_2}}}{k}}}
k1k2=k1k×kk2\Rightarrow \,\dfrac{{{k_1}}}{{{k_2}}} = \dfrac{{{k_1}}}{k} \times \dfrac{k}{{{k_2}}}
k1k2=n+1n×1n+1\Rightarrow \,\dfrac{{{k_1}}}{{{k_2}}} = \dfrac{{n + 1}}{n} \times \dfrac{1}{{n + 1}}
k1k2=1n\Rightarrow \,\dfrac{{{k_1}}}{{{k_2}}} = \dfrac{1}{n}
Therefore, the ratio k1k2\dfrac{{{k_1}}}{{{k_2}}} is 1n\dfrac{1}{n} .

So, the correct answer is “Option C”.

Note:
Here, we can also divide K1K_1 by K2K_2 directly instead of dividing K1K_1 by KK and K2K_2 by KK respectively. Also, the length of an ideal spring is equilibrium. Now, if the spring is stretched, the force constant of the spring will be proportional to the increase in the length of the spring and this increase will be an increase in equilibrium length. Therefore, this force will pull each end towards the other.