Boltzmann entropy is a measure of the amount of disorder or randomness in a system, defined by the equation $S = k_B \ln(W)$, where $S$ is the entropy, $k_B$ is the Boltzmann constant, and $W$ is the number of microstates corresponding to a macrostate. This concept links microscopic behavior of particles to macroscopic thermodynamic properties, illustrating how entropy can be understood in terms of probabilities and distributions of energy among particles.