According to the third law of thermodynamics, the entropy of a perfectly organized crystal at absolute zero is

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Multiple Choice

According to the third law of thermodynamics, the entropy of a perfectly organized crystal at absolute zero is

Explanation:
Entropy measures how many microscopic configurations fit a given macroscopic state. For a perfectly organized crystal at absolute zero, there is only one way to arrange the particles that matches that perfect order, so the number of accessible microstates is one. Using S = k_B ln Ω, with Ω = 1, gives S = 0. The third law sets this zero point for a perfectly crystalline substance at 0 K. In real materials there can be tiny residual entropy due to defects or degeneracy, but in the ideal case the entropy at absolute zero is zero. Therefore, the entropy is zero.

Entropy measures how many microscopic configurations fit a given macroscopic state. For a perfectly organized crystal at absolute zero, there is only one way to arrange the particles that matches that perfect order, so the number of accessible microstates is one. Using S = k_B ln Ω, with Ω = 1, gives S = 0. The third law sets this zero point for a perfectly crystalline substance at 0 K. In real materials there can be tiny residual entropy due to defects or degeneracy, but in the ideal case the entropy at absolute zero is zero. Therefore, the entropy is zero.

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