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Thormodynamics
branch o sciena which dala wth
t is a
napt gf heat and tenpatue. Hnd intoCGTwen:
hoat and other pamy o 2gy
ThmodynomicsSystems
an na. pHces
btain value oresSuL, vrolum and ternperotuy. O
Suocurdi
Eerthingngs gutida the system wtich Can hawe diet
on the 3ystem.
Thomodynamic Vaviable
The quantites ike Py, T uhich halp ua to sud,
the behaurigur of homodyramc, Systen.
EquatiGn of state
The mathomatical Melahan betueanP, Vanl Tof a
tornedynamic systn ia cal@e eguatim o sttt
PV = nkI (uee e i Gas Congtart)
mo.
Thnal eguilibrum
Tuo system QHe gaid to be in
they hae Jarne ternprotue. thaxmaleglibriumn
t stotea that
, classMate
Date
Page
Separately in thomae equilibrium with the third system
o.TrenA and R e alo in thomal equiabiurm
wtth each otho
Tntenal enotgy kinstic
the fram of aoana to which tho cortre
mass of system ü at sOst.
The internal kinetie enersy of a gas is a pundim.
of its tempratu.
trummodyamic
state vaiaboa a it depends upm h specilic valuss
ce P,v and T
kinatic
TrHonal erargy @ an idaal qas is puely kinilC
in natUre.
betueon Heat and Wrk
due to termperatue
o eat ia a mode gf ensgy trargtor Wark
dghunca in System and sUMOusinge s a mode
traraar Lutich de moY inolue the tempoatr
enog
e)2) than Reat ig sulid to a qas, its molcueey moitsmaes
Dat in all the ditectton, whun piston comoresses
moacul gnove in one dretin
Sign nvections
&ut i
1) Heat abgorbed by the systen is positive angien 8t
Tgatie.
2)ork dona by tha syskm positie and on the Systern is.
iagatie.
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