For an isolated system:
- No exchange of heat or work with surroundings: \(q = 0,\ w = 0\).
- Hence, \(\Delta U = 0\) always (energy is conserved).
However, entropy is different:
- The second law of thermodynamics states that for an isolated system:
- \(\Delta S \ge 0\)
- \(\Delta S = 0\) for a reversible process (true equilibrium change).
- \(\Delta S > 0\) for a spontaneous/irreversible process.
Conclusion:
Even though \(\Delta U = 0\) for an isolated system, \(\Delta S\) is:
- \(\Delta S = 0\) if the change is reversible.
- \(\Delta S > 0\) if the process is spontaneous/irreversible.
So, in general for an isolated system: \(\boxed{\Delta S \ge 0}\).