In thermodynamics,
entropy is commonly associated with the amount of order, disorder, or
chaos in a
thermodynamic system. This stems from
Rudolf Clausius' 1862 assertion that any
thermodynamic process always "admits to being reduced to the alteration in some way or another of the
arrangement of the constituent parts of the
working body" and that internal work associated with these alterations is quantified energetically by a measure of "entropy" change, according to the following differential expression:
- where Q = ... and T = ...