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Question: If the length of the wire is doubled, the strain produced will be given as, \(\begin{aligned} ...

If the length of the wire is doubled, the strain produced will be given as,
A.0.5 B.1 C.0.25 D.2 \begin{aligned} & A.0.5 \\\ & B.1 \\\ & C.0.25 \\\ & D.2 \\\ \end{aligned}

Explanation

Solution

The longitudinal stress is given as the ratio of the change in the length of the wire to the original length of the wire. As it is mentioned like the wire and the length has been varied, the strain produced will be longitudinal strain itself. And the value will not be having any units as the strain is a dimensionless quantity. Hope this may help you to solve this question.

Formula used:
The longitudinal stress is given as,
S=ΔLLoldS=\dfrac{\Delta L}{{{L}_{old}}}
Where ΔL\Delta L be the change in length and Lold{{L}_{old}} be the original length of the wire.

Complete step by step answer:

As we look into the question, we can see that the terms given in the questions can be written as,
The original length of the wire can be mentioned as LL.
Lold=L{{L}_{old}}=L
And now this length has been changed to double of its value which means that the length now becomes,
Lnew=2L{{L}_{new}}=2L
Therefore the change in length can be taken as the difference between these two lengths. That is we can write that,
ΔL=LnewLold\Delta L={{L}_{new}}-{{L}_{old}}
Substituting the values in it will give,
ΔL=2LL=L\Delta L=2L-L=L
Now we have to find the longitudinal strain acting on the wire. It is given as the ratio of the change in length of the wire to the actual or the original length of the wire. This can be expressed in the form of an equation given as,
S=ΔLLoldS=\dfrac{\Delta L}{{{L}_{old}}}
Substituting the values in it will give,
S=LL=1S=\dfrac{L}{L}=1

So, the correct answer is “Option B”.

Note: Stress is defined as the force acting on a surface per unit area. Stress can be the reason for the strain, when it is having the force to overcome the strength of the surface that is under stress. Strain is a variation in shape or size due to the applied forces.