Disorder is far more likely than order, which can be seen statistically. The entropy of a system in a given state (a macrostate) can be written as \(s = KLNw,\) where \(k = 1.38 \times 10^{-23} \space...Disorder is far more likely than order, which can be seen statistically. The entropy of a system in a given state (a macrostate) can be written as \(s = KLNw,\) where \(k = 1.38 \times 10^{-23} \space J/K\) is Boltzmann’s constant, and \(lnW\) is the natural logarithm of the number of microstates \(W\) corresponding to the given macrostate.
Disorder is far more likely than order, which can be seen statistically. The entropy of a system in a given state (a macrostate) can be written as \(s = KLNw,\) where \(k = 1.38 \times 10^{-23} \space...Disorder is far more likely than order, which can be seen statistically. The entropy of a system in a given state (a macrostate) can be written as \(s = KLNw,\) where \(k = 1.38 \times 10^{-23} \space J/K\) is Boltzmann’s constant, and \(lnW\) is the natural logarithm of the number of microstates \(W\) corresponding to the given macrostate.