The Boltzmann Distribution describes the distribution of particles among different energy states in a thermodynamic system at thermal equilibrium. It states that the probability of a system being in a state with energy is given by the formula:
where is the Boltzmann constant, is the absolute temperature, and is the partition function, which serves as a normalizing factor ensuring that the total probability sums to one. This distribution illustrates that as temperature increases, the population of higher energy states becomes more significant, reflecting the random thermal motion of particles. The Boltzmann Distribution is fundamental in statistical mechanics and serves as a foundation for understanding phenomena such as gas behavior, heat capacity, and phase transitions in various materials.
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