Statistical Mechanics
Boltzmann's entropy is a measure of the number of microstates corresponding to a given macrostate of a thermodynamic system, mathematically expressed as $S = k_B \ln \Omega$, where $S$ is the entropy, $k_B$ is Boltzmann's constant, and $\Omega$ is the number of accessible microstates. This concept emphasizes the connection between microscopic behaviors of particles and macroscopic thermodynamic properties, highlighting that higher entropy implies more disorder and a greater number of possible configurations within a system.
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