Entropy

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"Energy has to do with possibilities. Entropy has to do with the probabilities of those possibilities happening. It takes energy and performs a further epistemological step."
Constantino Tsallis [1]

Entropy was first described by Rudolf Julius Emanuel Clausius in 1865 [2]. The statistical mechanical desciption is due to Ludwig Eduard Boltzmann (Ref. ?).

Classical thermodynamics

In classical thermodynamics one has the entropy, S,

dS=δQreversibleT

where Q is the heat and T is the temperature.

Statistical mechanics

In statistical mechanics entropy is defined by

S:=−kB∑i=1Wpilnpi

where kB is the Boltzmann constant, i is the index for the microstates, and pi is the probability that microstate i is occupied. In the microcanonical ensemble this gives:

S=kBlnW

where W (sometimes written as Ω) is the number of microscopic configurations that result in the observed macroscopic description of the thermodynamic system. This equation provides a link between classical thermodynamics and statistical mechanics

Tsallis entropy

Tsallis (or non-additive) entropy [3] is defined as (Eq. 1)

Sq:=kB1−∑i=1Wpiqq−1

Arrow of time

Articles:

Books:

  • Steven F. Savitt (Ed.) "Time's Arrows Today: Recent Physical and Philosophical Work on the Direction of Time", Cambridge University Press (1997) ISBN 0521599458
  • Michael C. Mackey "Time's Arrow: The Origins of Thermodynamic Behavior" (1992) ISBN 0486432432
  • Huw Price "Time's Arrow and Archimedes' Point New Directions for the Physics of Time" Oxford University Press (1997) ISBN 978-0-19-511798-1

See also:

References

Related reading

External links