Boltzmann Entropy is a fundamental concept in statistical mechanics that quantifies the amount of disorder or randomness in a thermodynamic system. It is defined by the famous equation:
where is the entropy, is the Boltzmann constant, and represents the number of possible microstates corresponding to a given macrostate. Microstates are specific configurations of a system at the microscopic level, while macrostates are the observable states characterized by macroscopic properties like temperature and pressure. As the number of microstates increases, the entropy of the system also increases, indicating greater disorder. This relationship illustrates the probabilistic nature of thermodynamics, emphasizing that higher entropy signifies a greater likelihood of a system being in a disordered state.
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