To solve this question, we need to understand some concepts related to thermodynamics, specifically the specific heats of gases.
An ideal gas has two specific heats: the molar specific heat at constant pressure \(C_P\) and the molar specific heat at constant volume \(C_V\). The relationship between these two specific heats and the universal gas constant \(R\) is given by:
\(C_P = C_V + R\).
The ratio of specific heats is denoted by \(\gamma = \frac{C_P}{C_V}\).
We can express \(\gamma\) as:
\(\gamma = \frac{C_V + R}{C_V}\).
To find \(C_V\), we rearrange the equation above:
\(\gamma = 1 + \frac{R}{C_V}\),
which simplifies to:
\(C_V(\gamma - 1) = R\).
Thus, the expression for \(C_V\) becomes:
\(C_V = \frac{R}{\gamma - 1}\).
Therefore, the correct answer is \(\frac{R}{\gamma - 1}\), which matches the option:
\(\frac{R}{1-\gamma}\)
(please note the order of terms should be checked against the provided answer).
Conclusion: The correct answer is \(\frac{R}{1-\gamma}\).
The following graph represents the T-V curves of an ideal gas ( where T is the temperature and V the volume) at three pressures P1, P2 and P3 compared with those of Charles's law represented as dotted lines.

Then the correct relation is :