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Question: Coefficient of cubical expansion of a solid is \(0.000027{}^{\circ }{{C}^{-1}}\). If the temperature...

Coefficient of cubical expansion of a solid is 0.000027C10.000027{}^{\circ }{{C}^{-1}}. If the temperature is measured on Fahrenheit scale, numerical value of coefficient of linear expansion of solid is :
A. 0.000009F10.000009{}^{\circ }{{F}^{-1}}
B. 0.000005F10.000005{}^{\circ }{{F}^{-1}}
C. 0.000015F10.000015{}^{\circ }{{F}^{-1}}
D. 0.000018F10.000018{}^{\circ }{{F}^{-1}}

Explanation

Solution

Coefficient of volume/linear expansion is defined as the fraction by which the volume/length of solid changes for a unit change in its temperature. The coefficient of volume expansion is three times the coefficient of linear expansion for a given solid. Use the relation between the Celsius and Fahrenheit scale.

Formula used:
ΔVV=γΔT\dfrac{\Delta V}{V}=\gamma \Delta T
α=γ3\alpha =\dfrac{\gamma }{3}
Here, γ\gamma is a proportionality constant called coefficient of volume expansion and α\alpha is coefficient of linear expansion.
F=9C5+32F=\dfrac{9C}{5}+32
where FF represents temperature in F{}^{\circ }F and CC represents temperature in C{}^{\circ }C.

Complete step by step solution:
It is found that ratio of the volume expansion (contraction) of a solid to its original volume is directly proportional to the change in its temperature.
Therefore, we can write that ΔVVΔT\dfrac{\Delta V}{V}\propto \Delta T.
ΔVV=γΔT\dfrac{\Delta V}{V}=\gamma \Delta T …. (i)
Here, γ\gamma is a proportionality constant called coefficient of volume expansion.
From (i), we can write that
γ=ΔVV.1ΔT\gamma =\dfrac{\Delta V}{V}.\dfrac{1}{\Delta T}.
With this, the coefficient of volume expansion is defined as the fraction by which the volume of solid changes for a unit change in its temperature. Similar, we have some known coefficient of linear expansion (α\alpha ). Coefficient of linear is the fraction by which the length of the solid changes for a change in temperature of one unit.And it is found that, α=γ3\alpha =\dfrac{\gamma }{3}.
In the question it is given that λ=0.000027C1\lambda =0.000027{}^{\circ }{{C}^{-1}}.
α=0.000027C13 α=0.000009C1\alpha =\dfrac{0.000027{}^{\circ }{{C}^{-1}}}{3}\\\ \Rightarrow \alpha = 0.000009{}^{\circ }{{C}^{-1}}.
This means that if we increase the temperature by 1C1{}^{\circ }C, then the length of the solid will increase by a fraction of 0.0000090.000009. The relation between the Fahrenheit scale and the Celsius scale is given as F=9C5+32F=\dfrac{9C}{5}+32 ….. (ii).
where F represents temperature in F{}^{\circ }F and C represents temperature in C{}^{\circ }C.
Therefore, if we change the temperature by 1C1{}^{\circ }C, then in Fahrenheit scale it is equal to a change in temperature of 95F\dfrac{9}{5}{}^{\circ }F. Hence, the linear expansion of the solid can be written as
α=0.00000995F α=0.000005F1\alpha =\dfrac{0.000009}{\dfrac{9}{5}{}^{\circ }F}\\\ \therefore \alpha =0.000005{}^{\circ }{{F}^{-1}}.

This means that the correct option is B.

Note: By looking at the equation (ii), students may think that the change in
temperature by 1C1{}^{\circ }C is equal to (95+32)F\left( \dfrac{9}{5}+32 \right){}^{\circ }F.However, the equation (2) gives us the absolute value of the temperature in the degree Fahrenheit for a given value of the temperature in degree Celsius. While calculating the change in temperature, the constant term (i.e. 32) will not be counted.