topic 8 property cet
TRANSCRIPT
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The Advanced ChemicalEngineering Thermodynamics
The thermodynamics properties offluids (II)
Q&A_-10- 11/17/2005(10)
Ji-Sheng Chang
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Property relations
The residual Gibbs ree energ! The deini"i#n # residual $r#$er"ies
%& (T') %(T') - %*G(T')
+ esidual $r#$er"!
*G + *deal gas beha,i#r $r#$er"!
%&
(T') %(T') - %*G
(T')'% are "he $r#$er"ies as ' G' .' S'
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Property relations
The residual $r#$er"ies & (T') (T') - *G(T') - T/
asi "her3#d!na3is rela"i#nshi$ #ralula"i#ns
G& (T') G(T') - G*G(T')%#re i3$#r"an" in "radi"i#nal Che3ial4ngineering Ther3#d!na3is
.& (T') .(T') - .*G(T')
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Property relations
eri,ing "he residual $r#$er"ies in"er3s # "he T $r#$er"ies6
r#3 "he genera"ing un"i#n # Gibbsree energ!' & /T 8∂(G& /T)/∂9T'
Then d(G& /T) (& /T)d'
"# in"egra"e r#3 0 "# a" #ns"an" T6
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Property relations
The in"egra"ed resul" in "er3s # T$r#$er"! as "he #r3ula (:6;5)
T)(constant,)1(0∫ −= P
R
P
dP Z
RT
G
T)(constant,)1
(0∫ −=
P R
dP P RT
V
RT
G
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Property relations
The residual en"hal$!' .& /T - T8∂(G& /T)/∂T9'The in"egra"ed resul" in "er3s # T$r#$er"! as "he #r3ula (:6;:)
T)(constant,0∫
∂∂−= P
P
R
P
dP
T
Z T RT
H
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Property relations
*n $re,i#us se"i#n S ./T - G/T'"hen "he residual en"r#$! S& / .& /T - G& /TThe resul" in "er3s # T $r#$er"!as "he #r3ula (:6;
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Property relations
=sing "he inde$enden" $r#$er"! # Tand
%#re #33#nl! as "he #r3 ('T) #"he T e>ua"i#ns # s"a"e' es$eiall!"he ubi e>ua"i#ns # s"a"e6
?T/' ?ρT as ρ 1/
dTd(?ρ)T(?dρ@ρd?)a" #ns"an" T
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Property relations
d/dρ /ρ@d?/?' as "he #r3ula (:65
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Property relations
Calula"ing "he residual $r#$er"ies The T da"a'
=sing gra$hial in"egra"i#n 3e"h#d "#
alula"e "he residual Gibbs ree energ! r#3s"ea3 da"a6
T)(constant,1
0∫
−
= P
R
dP P
Z
RT
G
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Phase diagram
0 2 0 0 4 0 0 0 0 ! 0 0 " 0 0 0
T #$
0
" 0 0
2 0 0
% 0 0
4 0 0
& 0 0
P
# '
a
r
S#lidi>uid
Gas
C'TC
16 T $hase diagra3 # Ba"er
26 The S#lid/i>uid e>uilibriu3 ur,e
#r Ba"er
#r 3#s" #3$#nen"
200C $a"h
Cri"ial $r#$er"ies
C220655 bar
TC:;761 D
TTri27E61: D
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apor#i*uid e*uili'rium curve
The An"#ine e>ua"i#n The #ns"an" # An"#ine
e>ua"i#n #r Ba"er A1:6E
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Property
Cri"ial $r#$er"ies # Ba"er
C220655 bar
TC:;761 D
Tri06:11 a
TTri27E61: D TnE7E615 D
a" 1601E25 bar 1 a"3
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Property relations
r#ble3s
Calula"e "he residual Gibbs
energ! # "he 200°C su$erhea"s"ea3 a" 10 bar' using "he Tda"a r#3 s"ea3 "ables
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Properties
P/kPa P/bar V/cm3g-
1
V/cm3mol-1
Z (Z-1)/P
1 0.01 218350 3933575 0.999951 -0.00493
50 0.5 4356.0 78473.34 0.997432 -0.00514100 1 2172.3 39133.98 0.994822 -0.00518
200 2 1080.4 19463.41 0.989555 -0.00522
300 3 716.35 12905.05 0.984174 -0.00528
400 4 534.26 9624.694 0.978674 -0.00533500 5 424.96 7655.654 0.973069 -0.00539
600 6 352.04 6342.001 0.967317 -0.00545
700 7 299.92 5403.059 0.961455 -0.00551
800 8 260.79 4698.132 0.955446 -0.00557
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Properties
P/kPa P/bar V/cm3g-
1
V/cm3mol-1
Z (Z-1)/P
900 9 230.32 4149.215 0.949291 -0.00563
1000 10 205.92 3709.649 0.943027 -0.0057
1100 11 185.92 3349.349 0.936579 -0.00577
1200 12 169.23 3048.678 0.930002 -0.00583
1300 13 155.09 2793.946 0.923321 -0.0059
1400 14 142.94 2575.064 0.916447 -0.005971500 15 132.38 2384.826 0.909367 -0.00604
1550 15.5 127.61 2298.894 0.90582 -0.00608
1554.9 15.55 127.20 2291.508 0.905764 -0.00606
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+esidual ,i''s free energy
properties
0 4 ! " 2 " 2 0P - ' a r .
/ 0 0 0 !
/ 0 0 0
/ 0 0 0 4
/ 0 0 0 2
0
( 1
/ "
) # P
-
'
a
r /
"
.
, + # + T o f s u p e r h e a t s te a m
2 0 0 C
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E3ample "
Calula"ing "he residual $r#$er"ies The T e>ua"i#ns # s"a"e
=sing "he "B# "er3 ,irial e>ua"i#n #s"a"es' es"i3a"e "he 3#lar ,#lu3e'residual en"hal$!' residual en"r#$!' andresidual Gibbs ree energ! # "hecarbon dioxide a" "he s"a"es #
"e3$era"ure # 25°C and $ressure # 1bar6
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eriving the
formulas
The e>ua"i#ns #residual Gibbs reeenerg!
Three "!$e # "he
"B# "er3 ,iriale>ua"i#n
The residual Gibbsree energ! #r a gasa" eah and T
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eriving the
formulas
Se#nd ,irial#eiien" r#3 T da"a
r#3 generaliHed
#rrela"i#ne>ua"i#ns
ased 3#leular
"her3#d!na3i' i"is in"egra"ed r#3$#"en"ial un"i#n
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E3ample 2
Calula"ing "he residual $r#$er"ies The T e>ua"i#ns # s"a"e
=sing "he "B# "er3 ,irial e>ua"i#n #s"a"es' es"i3a"e "he 3#lar ,#lu3e'residual en"hal$!' residual en"r#$!' andresidual Gibbs ree energ! # "hemethane a" "he s"a"es # "e3$era"ure
# 25°C and $ressure # 1 bar6
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E3ample %
Calula"ing "he residual $r#$er"ies The T e>ua"i#ns # s"a"e
(? )=sing "he "B# "er3 ,irial e>ua"i#n #s"a"es' es"i3a"e "he 3#lar ,#lu3e'residual en"hal$!' residual en"r#$!' andresidual Gibbs ree energ! # "he
benzene a" "he s"a"es # "e3$era"ure# 25°C and $ressure # 1 bar6
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Theorem of
corresponding states
TB#-$ara3e"er "he#re3 ##rres$#nding s"a"es
Gi,en T and inding T'
Calula"e Tr' r
=sing Tr' r "# inding "he redued$r#$er"ies r#3 Table 461 "# 461:
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Theorem of
corresponding states
Three-$ara3e"er "he#re3 ##rres$#nding s"a"es
Gi,en T and inding T' ' ω Calula"e Tr' r
=sing Tr' r' ω "# inding "heredued $r#$er"ies r#3 Table 461 "#461:
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Theorem of
corresponding states
ased #n "he #rres$#nding s"a"es$rini$les The ee/Desler generaliHed #rrela"i#n
"ables' A$$endiI 4 a" "eI" b##s # $agesr#3 :F5 "# 7116
The $r#$er"ies # s#3e $ure s$eies"ables' A$$endiI a" "eI" b##s # $agesr#3 :7F "# :
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E3ample 4
A$$lia"i#n # "he "he#re3 ##rres$#nding s"a"es "# es"i3a"e "he"her3#d!na3is $r#$er"ies # "he
$ure #3$#nen"s6 A" "e3$era"ure # 25°C and $ressure # 1
bar' es"i3a"e "he 3#lar ,#lu3e' residualen"hal$!' residual en"r#$!' and residual
Gibbs ree energ! # "he carbon dioxide6
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E3ample &
A$$lia"i#n # "he "he#re3 ##rres$#nding s"a"es "# es"i3a"e "he"her3#d!na3is $r#$er"ies # "he
$ure #3$#nen"s6 A" "e3$era"ure # 25°C and $ressure # 1
bar' es"i3a"e "he 3#lar ,#lu3e' residualen"hal$!' residual en"r#$!' and residual
Gibbs ree energ! # "he methane6
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E3ample
A$$lia"i#n # "he "he#re3 ##rres$#nding s"a"es "# es"i3a"e "he"her3#d!na3is $r#$er"ies # "he
$ure #3$#nen"s6 (? )
A" "e3$era"ure # 25°C and $ressure # 1bar' es"i3a"e "he 3#lar ,#lu3e' residualen"hal$!' residual en"r#$!' and residualGibbs ree energ! # "he benzene6