\(\frac{2}{T}\)
\(\frac{3}{T}\)
\(\frac{1}{2T}\)
\(\frac{1}{T}\)
To determine the volume expansion coefficient of the gas given the relation \( PT^2 = \text{constant} \), we start by analyzing the ideal gas law and the provided relation.
According to the ideal gas law, the state of an ideal gas is given by:
PV = nRT
where \( P \) is pressure, \( V \) is volume, \( n \) is number of moles, \( R \) is the universal gas constant, and \( T \) is temperature in Kelvin.
The given thermodynamic process is characterized by the relation \( PT^2 = \text{constant} \), let's denote this constant as \( C \):
P T^2 = C \quad \Rightarrow \quad P = \frac{C}{T^2}
Substitute this expression for \( P \) into the ideal gas law:
\frac{C}{T^2} \cdot V = nRT \quad \Rightarrow \quad V = \frac{nRT^3}{C}
The volume expansion coefficient, \( \gamma \), is defined as:
\gamma = \frac{1}{V} \left( \frac{\partial V}{\partial T} \right)_P
Now differentiate the expression for \( V \) with respect to \( T \) while keeping \( P \) constant:
The differential of \( V = \frac{nRT^3}{C} \) with respect to \( T \) gives:
\frac{\partial V}{\partial T} = \frac{3nRT^2}{C}
Now substitute back into the expression for \( \gamma \):
\gamma = \frac{1}{V} \left( \frac{\partial V}{\partial T} \right)_P = \frac{C}{nRT^3} \cdot \frac{3nRT^2}{C}
Simplifying this expression, we find:
\gamma = \frac{3}{T}
Thus, the volume expansion coefficient of the gas is \frac{3}{T}, which verifies that the correct option is indeed \frac{3}{T}.
