Solveeit Logo

Question

Physics Question on mechanical properties of solids

The length of a metal wire is L1L_1 when the tension is T1T_1 and L2L_2 when the tension is T2T_2. The unstretched length of the wire is

A

L2+L22\frac{L_{2}+L_{2}}{2}

B

L1L2\sqrt{L_{1}L_{2}}

C

T2L1T1L2T2T1\frac{T_{2}L_{1}-T_{1}L_{2}}{T_{2}-T_{1}}

D

T2L1T1L2T2+T1\frac{T_{2}L_{1}-T_{1}L_{2}}{T_{2}+T_{1}}

Answer

T2L1T1L2T2T1\frac{T_{2}L_{1}-T_{1}L_{2}}{T_{2}-T_{1}}

Explanation

Solution

Let the initial length of the metal wire is LL.
The strain at tension T1T_{1} is ΔL1=L1L\Delta L_{1}=L_{1}-L
The strain at tension T2T_{2} is ΔL2=L2L\Delta L_{2}=L_{2}-L
Suppose, the Young's modulus of the wire is YY, then
T1AΔL1L=T2AΔL2L\frac{\frac{T_{1}}{A}}{\frac{\Delta L_{1}}{L}}=\frac{\frac{T_{2}}{A}}{\frac{\Delta L_{2}}{L}}
where, AA is an cross-section of the wire. assume to be same at all the situations. T1A×LΔL1\Rightarrow \frac{T_{1}}{A} \times \frac{L}{\Delta L_{1}}
=T2A×LΔL2=\frac{T_{2}}{A} \times \frac{L}{\Delta L_{2}}
T1(L1L)=T2(L2L)\Rightarrow \frac{T_{1}}{\left(L_{1}-L\right)}=\frac{T_{2}}{\left(L_{2}-L\right)}
T1(L2L)=T2(L1L);T_{1}\left(L_{2}-L\right)=T_{2}\left(L_{1}-L\right) ;
L=T2L1T1L2T2T1L=\frac{T_{2} L_{1}-T_{1} L_{2}}{T_{2}-T_{1}}