In an adiabatic process, there is no heat exchange with the surroundings, and the relation between the pressure, volume, and temperature of a gas is governed by the following equation:
\[
TV^{\gamma - 1} = \text{constant}
\]
Where:
- \( T \) is the absolute temperature,
- \( V \) is the volume,
- \( \gamma \) is the adiabatic index (ratio of specific heats \( C_p / C_v \)).
This equation states that in an adiabatic process, the product of the temperature and volume raised to the power of \( \gamma - 1 \) is constant.
Thus, the correct relation between volume and temperature for an adiabatic process is:
\[
\boxed{TV^{\gamma - 1} = \text{constant}}
\]