In thermodynamics, the first law of thermodynamics is given by:
\[
\Delta U = Q - W
\]
where:
- \( \Delta U \) is the change in internal energy of the system,
- \( Q \) is the heat absorbed by the system,
- \( W \) is the work done by the system.
Since the gas is taken from state A to state B along two different paths, the change in internal energy, \( \Delta U \), is the same for both paths, as internal energy depends only on the initial and final states of the system, not on the path taken. Therefore, we have:
\[
\Delta U = Q_1 - W_1 = Q_2 - W_2
\]
This shows that the difference between the heat absorbed and the work done is the same for both paths. Thus, the correct relationship is:
\[
Q_1 - W_1 = Q_2 - W_2
\]