A measure of the energy that is not available for work during a
→ thermodynamic process.
It is defined by dS = dQ/T, where dS is the differential change in
entropy, dQ is the differential amount of heat introduced to the system in
a → reversible process, and T the
→ absolute temperature of the system.
Entropy remains constant during → reversible processes
and increases during → irreversible processes without ever
decreasing. According to the → second law of thermodynamics, an
→ isolated system evolves toward a state of maximum entropy.
See also → Maxwell’s demon.
Statistical physics:
A measure of → disorder of the configuration of
→ microstates which make up a → macrostate.
→ Boltzmann’s relation,
→ Boltzmann’s entropy formula.
Highly disordered systems have a large entropy; highly ordered systems have low entropy.
Math.: A measure of information content.
→ information entropy.
Etymology (EN): From Ger. Entropie, coined 1865 by physicist Rudolf Clausius (1822-1888) from
Gk. entropia “a turning toward,” from en- “in” + trope
“a turning, change,” related to tropos “a turn, way, manner,”
from tropein “to turn,” from PIE base *trep- “to turn”
(cf. L. trepit “he turns”).
Etymology (PE): Dargâšt, from dar “in” + gâšt present stem of
gâštan “to cause to revolve, to turn,” transitive of gaštan,
variant gardidan “to turn,
to change” (Mid.Pers. vartitan; Av. varət- “to turn, revolve;”
cf. Skt. vartati; L. vertere; O.H.G. werden “to become;”
PIE base *wer- “to turn, bend”).