An ideal gas undergoing a reversible adiabatic process is described by the equation relating pressure \(P\) and temperature \(T\) such that \(P \propto T^3\). To find the value of \(\frac{C_p}{C_v}\), we need to derive it using adiabatic process relations and the given proportionality.
For an adiabatic process, the relationship between pressure \(P\) and temperature \(T\) is given by:
\(P \propto T^3\) can be written as \(P = k \cdot T^3\), where \(k\) is a constant.
In a reversible adiabatic process, the adiabatic condition is:
\(P V^\gamma = \text{constant}\)
We also have the ideal gas law:
\(P V = nRT\)
From \(P \propto T^3\) and combining it with the ideal gas equation, we write:
\(R = \frac{C_p - C_v}{\mu}\)
Where \(\gamma = \frac{C_p}{C_v}\) and P = k \cdot T^3 and ideal gas relations:
Since \(PV^\gamma = \text{constant}\)
\((\frac{T^\gamma}{T^(3(\gamma-1))}) = \text{constant}\).
Equate powers of \(T\) to give \(3(\gamma-1)=\gamma\) which simplifies to \(\gamma = \frac{4}{3}\).
Thus, the value of \(\frac{C_p}{C_v}\) is 4/3, hence, the correct answer is: 4/3.