Step 1: In statistical thermodynamics, entropy is understood as a measure of the number of microscopic configurations \( W \) that correspond to a thermodynamic system’s macroscopic state.
Step 2: The statistical definition of entropy is given by Boltzmann’s famous equation: \[ S = k \ln W \] where:
- \( S \) is the entropy,
- \( k \) is Boltzmann’s constant,
- \( W \) is the number of accessible microstates.
Step 3: As the number of accessible microstates increases (i.e., as the system becomes more disordered or more energy levels are populated), the entropy also increases.
Why the other options are incorrect: - (A) Entropy is fundamentally dependent on the number of microstates.
- (B) It increases—not decreases—with more microstates.
- (D) Entropy varies with state variables and is not constant even for ideal gases.