Concept:
According to the First Law of Thermodynamics, the net heat change (\(\Delta Q_{\text{net}}\)) in a thermodynamic process is equal to the sum of the change in internal energy (\(\Delta U\)) and the net work done (\(W_{\text{net}}\)) by the system:
\[
\Delta Q_{\text{net}} = \Delta U + W_{\text{net}}
\]
For any complete cyclic process, the system returns precisely to its initial state. Because internal energy is a state function depending solely on the current state parameters, the net change in internal energy over a complete cycle is identically zero:
\[
\Delta U_{\text{cyclic}} = 0 \quad \Rightarrow \quad \Delta Q_{\text{net}} = W_{\text{net}}
\]
The net work done during a cyclic process plotted on a pressure-volume (\(p\)-\(V\)) diagram is equal to the geometric area enclosed by the loop. If the cycle runs in a clockwise direction, the work done is positive; if it runs counter-clockwise, the work done is negative.
Step 1: Determine the sign of the net work done from the cycle direction.
Looking closely at the arrow directions marked on the square loop inside the given diagram:
• The top horizontal line shows expansion to the right (clockwise movement).
• The right vertical line tracks a downward path, completing a standard clockwise loop orientation.
Therefore, the net work done (\(W_{\text{net}}\)) and the net heat absorbed (\(\Delta Q_{\text{net}}\)) are both positive values.
Step 2: Calculate the geometric dimensions of the enclosed square area.
The loop forms a geometric square on the graph. Let us determine its side lengths along both axes:
• Change in Volume along the horizontal axis (\(\Delta V\)):
\[
\text{Width} = V_{\text{max}} - V_{\text{min}} = 4\text{L} - 2\text{L} = 2\text{ L}
\]
• Change in Pressure along the vertical axis (\(\Delta p\)):
\[
\text{Height} = p_{\text{max}} - p_{\text{min}} = 3\text{ atm} - 1\text{ atm} = 2\text{ atm}
\]
Step 3: Compute the enclosed area to find the net heat absorbed.
Since it is a square loop, the area is simply the product of its dimensions:
\[
W_{\text{net}} = \text{Enclosed Area} = \text{Width} \times \text{Height}
\]
\[
W_{\text{net}} = 2\text{ L} \times 2\text{ atm} = 4\text{ L} \cdot \text{atm}
\]
By substituting this value back into our derived First Law relation:
\[
\Delta Q_{\text{net}} = W_{\text{net}} = 4\text{ L} \cdot \text{atm}
\]