Final answer:
During irreversible adiabatic compression and expansion, the final temperature of the gas is not the same as the initial temperature. More work is done on the gas during compression, leading to an increase in temperature. The expansion process becomes irreversible due to temperature gradients inside the gas.
Step-by-step explanation:
a) More work is done during compression because more weight is placed on the piston during compression than during expansion (only one weight is removed). So more work is transferred to the system during compression, and then this work adds to the system's internal energy, hence the temperature increase. Is this correct?
This explanation is not entirely accurate. The work done on or by gas during compression or expansion is determined by the area under the pressure-volume (P-V) curve on a thermodynamic diagram. In an irreversible adiabatic compression, the process is not efficient, and more work might be done on the gas compared to an ideal (reversible) process. The increase in internal energy is related to the work done on the gas and is manifested as a temperature increase.
So, the key point here is that during an irreversible adiabatic compression, more work is done on the gas, leading to an increase in internal energy and, consequently, an increase in temperature. This is not directly related to the number of weights on the piston but rather to the nature of the process.
b) When one of the weights is reduced (for expansion), the pressure on the piston drops suddenly, and the piston shoots up. There will be temperature gradients inside the gas, which will give rise to entropy, hence making the process irreversible.
This explanation is closer to the correct understanding. In an irreversible expansion, sudden changes in pressure and volume can lead to non-uniformities or gradients in temperature within the gas. These gradients contribute to entropy generation, making the process irreversible. The irreversibility is associated with the lack of equilibrium and the departure from a quasi-static process.