A monoatomic ideal gas of \( n \) moles heated from temperature \( T_1 \) to \( T_2 \) under two different conditions (i) at constant pressure, (ii) at constant volume. The change in internal energy of the gas is:
Step 1: The change in internal energy \( \Delta U \) for an ideal gas depends only on the change in temperature and is given by: \[ \Delta U = n C_V \Delta T \] where:
- \( n \) is the number of moles,
- \( C_V \) is the molar heat capacity at constant volume,
- \( \Delta T = T_2 - T_1 \) is the change in temperature.
Step 2: For a monoatomic ideal gas, the molar heat capacity at constant volume is \( C_V = \frac{3}{2} R \). The change in internal energy is: \[ \Delta U = n \left( \frac{3}{2} R \right) (T_2 - T_1) \] Step 3: The change in internal energy depends only on the temperature change, not on whether the process is at constant pressure or constant volume. Thus, the change in internal energy is the same in both processes.