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Question: If the work done by stretching a wire by \[1\text{mm}\] is \[2\text{J}\] , the work necessary for st...

If the work done by stretching a wire by 1mm1\text{mm} is 2J2\text{J} , the work necessary for stretching another wire of the same material and area of cross-section and stretching length is halved is :
(A) 1/4J
(B) 4J
(C) 8J
(D) 16J

Explanation

Solution

We know that the formula of work done in stretching the wire is given by : w=12 YAl2Lw=\dfrac{1}{2}\text{ }\dfrac{\text{YAl}_{{}}^{2}}{L}. We are provided with the values of W and l for the first wire.
For the second wire , the value of A and l is halved.
On comparing the equations for the two cases , we can get the required value of work .

Formula Used:
w=1/2×stretching force ×change in length (1) we know that Y=FALl or F=YAlL(2) w=1/2\times {\text{stretching force }}\times {\text{change in length }}\to { (1)} \\\ {\text{we know that Y=}} \dfrac{F}{A}\centerdot \dfrac{L}{l}\text{ or F=}\dfrac{YAl}{L} \to (2)\\\
l= Change in length
L=Original Length
Putting values of (2) in (1) we get
w=12× YAl2L × l w=\dfrac{1}{2}\times \text{ }\dfrac{\text{YAl}_{{}}^{2}}{L}\text{ }\times \text{ l} \\\

Complete Step by step solution:
Given:- Work done in stretching a wire is
w1=2J l=1mm w_1 = 2J \\\ l=1mm \\\
Now, when are of cross section and stretching length is halved, we get: -
w2= 12×Y(A2)×1L×1mm2×1mm2{{w}_{2=}}\text{ }\dfrac{1}{2}\times Y\left( \dfrac{A}{2} \right)\times \dfrac{1}{L}\times \dfrac{1mm}{2}\times \dfrac{1mm}{2}
We get,
w2=18×w1 w2=28=14J w2=14J w_2 =\dfrac{1}{8}\times w_1\\\ w_2 =\dfrac{2}{8}=\dfrac{1}{4}J\\\ w_2 =\dfrac{1}{4}J\\\
Correct answer is (A).

Additional information:
In stretching the wire, work is done against internal restoring forces. This work is stored as elastic potential energy or strain energy.
In force F\text{F} acts along the length L\text{L} of the wire of cross section A\text{A} and stretches it by xx, then:
Young’s modulus γ=StressStrain=FAxL\gamma =\dfrac{\text{Stress}}{\text{Strain}}=\dfrac{\dfrac{\text{F}}{\text{A}}}{\dfrac{x}{\text{L}}}
So work done for additional small increase dxdx in length,
dw=Fdx=γALx.dxdw=\text{F}dx=\dfrac{\gamma \text{A}}{\text{L}}x.dx
Hence, total work done in increasing the length ll,
w=dw=F.dx=12γALl2w=\int{dw=\int{\text{F}\text{.}dx=\dfrac{1}{2}\dfrac{\gamma \text{A}}{\text{L}}{{l}^{2}}}}
This work done is stored in the wire.
Hence, energy stored in the wire
U = 12γAl2L=12Fl\text{U = }\dfrac{1}{2}\dfrac{\gamma \text{A}{{l}^{2}}}{\text{L}}=\dfrac{1}{2}\text{F}l (As F =γAlL)\left( \text{As F =}\dfrac{\gamma \text{A}l}{\text{L}} \right)

Note: Young modulus is a mechanical property that measures the tensile stiffness of a solid material.
Y=FALlY=\dfrac{F}{A}\centerdot \dfrac{L}{l}
Where F= stretching force
L=original length of body
A= area of body
l=change in length of body after stretching.