The coefficient of volume expansion ($\alpha_V$) for an ideal gas is defined as the fractional change in volume per unit change in temperature at constant pressure:
$\alpha_V = \frac{1}{V} \left(\frac{\partial V}{\partial T}\right)_P$
For an ideal gas, the equation of state is given by $PV = nRT$, where:
At constant pressure, we can write:
$V = \frac{nR}{P}T$
Taking the derivative with respect to temperature:
$\left(\frac{\partial V}{\partial T}\right)_P = \frac{nR}{P}$
Substituting this back into the expression for $\alpha_V$:
$\alpha_V = \frac{1}{V} \left(\frac{nR}{P}\right) = \frac{nR}{PV} = \frac{nRT}{PV \cdot T} = \frac{1}{T}$
Therefore, $\alpha_V = \frac{1}{T}$.
Since the x-axis of the graphs is $\frac{1}{T}$, and $\alpha_V = \frac{1}{T}$, the graph of $\alpha_V$ vs. $\frac{1}{T}$ should be a straight line with a slope of 1, passing through the origin.
The correct answer is (B)
A thin rod having a length of \(1 m\) and area of cross-section \(3 \times 10^{-6} m ^2\) is suspended vertically from one end. The rod is cooled from \(210^{\circ} C\) to \(160^{\circ} C\) After cooling, a mass \(M\) is attached at the lower end of the rod such that the length of rod again becomes \(1m\). Young's modulus and coefficient of linear expansion of the rod are \(2 \times 10^{11} N m ^{-2}\) and \(2 \times 10^{-5} K ^{-1}\), respectively. The value of \(M\) is ____ \(kg\). (Take \(g =10 \ m s ^{-2}\))