Question:medium

In statistical thermodynamics, Stirling's Approximation ($\ln N! \approx N \ln N - N$) is valid only when

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Stirling's approximation is essential for deriving Boltzmann's entropy formula ($S = k_B \ln \Omega$).
It works because macroscopic thermodynamic systems always have an extremely large number of particles ($N \approx 10^{23}$).
Updated On: Jul 7, 2026
  • N is a small integer
  • N is very large
  • The system is at 0 K
  • The gas behaves non-ideally
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The Correct Option is B

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