The correct relation between $\gamma=\frac{ c _{ p }}{ c _{ v }}$ and temperature $T$ is :
To determine the correct relationship between \(\gamma = \frac{c_p}{c_v}\) and temperature \(T\), we need to understand what \(\gamma\) represents and how it is influenced by temperature.
\(\gamma\) is known as the adiabatic index or heat capacity ratio, where \(c_p\) is the specific heat at constant pressure, and \(c_v\) is the specific heat at constant volume.
For an ideal gas, the relationship between \(\gamma\) and temperature depends largely on the molecular structure of the gas:
As temperature increases, more rotational and vibrational modes are excited, which can affect \(c_v\) more than \(c_p\). However, \(\gamma\) tends to decrease with increasing temperature for non-monoatomic gases because \(c_v\) increases faster than \(c_p\).
In the options provided:
Therefore, the correct relation is \(\gamma \propto T^{\circ}\), indicating \(\gamma\) is mostly independent of temperature for ideal monoatomic gases.
Hence, the answer is: \(\gamma \propto T^{\circ}\).