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Question: A thin copper wire of \(l\) length increases in length by \(1\% \) when heated from \(0^\circ {\text...

A thin copper wire of ll length increases in length by 1%1\% when heated from 0C0^\circ {\text{C}} to 100C100^\circ {\text{C}}, if a thin copper plate of area 2l×l2l \times l is heated from 0C0^\circ {\text{C}} to 100C100^\circ {\text{C}}, the percentage increase in its area will be.
A) 1%1\%
B) 2%2\%
C) 3%3\%
D) 4%4\%

Explanation

Solution

In this question, use the concept of the coefficient of the thermal expansion of the material that is when a solid material is heated or cooled, then the length of that object increases or decreases which depends on the coefficient of thermal expansion of the material.

Complete step by step answer:
As we know that in the Linear thermal expansion, when a solid material heated or cooled, then the change in length of solid material depends on the coefficient of thermal expansion of the material, the temperature difference, and the initial length of the object that is,
ΔL=αLΔT\Delta L = \alpha L\Delta T
Here, α\alpha is the thermal expansion of the solid material, LLis the original length of the solid material, and ΔT\Delta T is the change in temperature of the material.
Now we calculate the change in temperature of the copper wire when heated.
ΔT=100  C0  C ΔT=100  C  \Delta T = 100\;^\circ {\text{C}} - 0\;^\circ {\text{C}} \\\ \Rightarrow \Delta T = 100\;^\circ {\text{C}} \\\
So, the change in the temperature is 100  C100\;^\circ {\text{C}}.
Now, we substitute the value of the change in the length of the wire that is ΔLL=1100\dfrac{{\Delta L}}{L} = \dfrac{1}{{100}} and the value of the change in the temperature in the thermal expansion expression to calculate the coefficient of thermal expansion of the material as,
ΔL=αL(100)\Delta L = \alpha L\left( {100} \right)
Rearrange the equation as,
ΔLL=α100\Rightarrow \dfrac{{\Delta L}}{L} = \alpha 100
we substitute the value of the change in the length of the wire that is ΔLL=1100\dfrac{{\Delta L}}{L} = \dfrac{1}{{100}} as,
1100=α100\Rightarrow \dfrac{1}{{100}} = \alpha 100
After calculation we get,
α=104C\Rightarrow \alpha = {10^{ - 4}}\,{^\circ C}
So, the value of the coefficient of thermal expansion is 104C{10^{ - 4}}\,{^\circ C}.
In Area Thermal Expansion, when a solid material heated or cooled, then the change in the area of solid material is,
ΔA=βAΔT\Delta A = \beta A\Delta T
Here, β\beta is the thermal expansion of the solid material, AAis the original area of the solid material, and ΔT\Delta T is the change in temperature of the material.
As we know that the plate will expand in two directions when heated. So, β=2α\beta = 2\alpha
Now, we substitute the value of the thermal expansion in the above formula as,
ΔA=2αAΔT\Delta A = 2\alpha A\Delta T
Now, we rearrange the above expression as,
ΔAA=2αΔT\Rightarrow \dfrac{{\Delta A}}{A} = 2\alpha \Delta T
Now, we substitute 104{10^{ - 4}} for α\alpha and 100100 for ΔT\Delta T in the above equation to find the percentage increase in the area of the plate as,
ΔAA=2(104)100\Rightarrow \dfrac{{\Delta A}}{A} = 2\left( {{{10}^{ - 4}}} \right)100
After simplification we get,
ΔAA=0.02\Rightarrow \dfrac{{\Delta A}}{A} = 0.02
In the percentage form we get,
ΔAA=2%\therefore \dfrac{{\Delta A}}{A} = 2\%

\therefore The percentage increases in the area of the plate is 2%2\% . Hence, option (B) is correct.

Note:
When a solid material wire is heated or cooled, then the length of the wire increases or decreases which depends on the coefficient of thermal expansion of the material. The increase or decrease in the length of wire depends on the change in temperature and the coefficient of thermal expansion of the material of the wire.