arXiv:cond-mat/9708200 v2 28 Jan 1999
u ttesatntee h ocp f‘ons’i assumed. is discussion ‘hotness’ textbook of most concept beyond goes the that even rigor Te not and clarity start equilibrium. the thermal at and we and but pressure other) the the about stat from two accessible assumptions any adiabatically given is that one states least ma otherwi essence, that cons it concepts in entropy define main (which, the to principle The of made One is considerations. another. attempt these enter to no entr and state of states increase equilibrium equilibrium of one principle the take as that deduced is law second the
c
∗∗
97b h fti ril,b n mea any by article, this of Reproduction authors. the by 1997
∗
okprilyspotdb h dltinKitaso Fo Kristjansson Adalsteinn the by Foundati supported Science partially Work National . by supported partially Work
Abstract:
hsppri ceue oapa nPyisReports Physics in appear to scheduled is paper This 8 2000: and 1991 (MSC) Classification Sciences Mathematical .-a PACS: 1998
H EODLWO THERMODYNAMICS OF LAW SECOND THE
H HSC N AHMTC OF MATHEMATICS AND PHYSICS THE
eatet fPyisadMteais rneo Univers Princeton Mathematics, and Physics of Departments
h seta otltso lsia hroyaisaef are thermodynamics classical of postulates essential The
awnHl,PO o 0,Pictn J054 USA 08544, NJ Princeton, 708, Box . Hall, Jadwin
ntttfu hoeicePyi,Universit¨at Wien, Physik, f¨ur Theoretische Institut
otmngse5 00Ven,Austria Vienna, 1090 A 5, Boltzmanngasse
ao Yngvason Jakob
lit .Lieb H. Elliott
s spritdfrnncmeca purposes. mercial for permitted is ns,
1
nain nvriyo Iceland. of University undation,
ngatPHY95-13072A01. grant on
∗
∗∗
310
so h aeceia opsto position chemical same the of es
hwta tcnb eie rmsome from derived be can it that show
law. second the of s
p nirvril daai processes adiabatic irreversible in opy
e vrtigwr parison the is work everything kes
prtr sdrvdfo entropy, from derived is mperatur
The Physics And Mathematics Of The Second Law Of Thermodynamics (Princeton) 来自淘豆网www.taodocs.com转载请标明出处.