Step 1: Recall the key property of enthalpy for an ideal gas.
For an ideal gas, enthalpy is a function of temperature alone, \(h = h(T)\), and does not depend on pressure or volume. Internal energy \(u\) is a function of \(T\) only, and \(h = u + Pv = u + RT\), both terms depending only on \(T\).
Step 2: Use the condition that states 2 and 3 lie on the same isotherm.
"Lying on the same isotherm" means states 2 and 3 have the same temperature, \(T_2 = T_3\), even though they were reached by two different processes starting from state 1.
Step 3: Connect temperature equality to enthalpy equality.
Since \(h\) depends only on \(T\) for an ideal gas, and \(T_2 = T_3\), it follows that \(h_2 = h_3\), regardless of what the pressures \(P_2\) and \(P_3\) turn out to be.
Final Answer:
Equal temperature on the same isotherm forces equal enthalpy for an ideal gas.
\[ \boxed{h_2 = h_3} \]