An ideal gas undergoes a cyclic transformation, meaning it starts and returns to the same point. In a cyclic process, the change in internal energy (\(\Delta U\)) of an ideal gas is determined by the first law of thermodynamics: \[ \Delta U = Q - W \] where \(Q\) is the heat added to the system and \(W\) is the work done by the system. Since the system returns to its initial state, the internal energy, a state function, remains unchanged at the end of the cycle. Thus for any cyclic transformation, \(\Delta U = 0\). Therefore, regardless of the path taken (whether it's Case I, II, or III), the change in internal energy (\(\Delta U\)) will be the same for all cases. This means:
\(\Delta U({Case-I}) = \Delta U({Case-II}) = \Delta U({Case-III})\)