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8/7/2019 Gaspowercycles
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Reciprocating engines
(internal combustion)
Reciprocating engines
(internal combustion)
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Ericsson cycleEricsson cycle
same as Stirling cyclesame as Stirling cyclewit h th e P=const processeswit h th e P=const processessubstituted for v=constsubstituted for v=constsh ould involve regenerationsh ould involve regenerationimpracticalimpractical
s
P=const
Ex ample 9.9Ex ample 9.9
regenerationregeneration
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Efficiency of Stirling andEricsson cycles wit h
regeneration
Efficiency of Stirling andEricsson cycles wit h
regeneration
11 s ts t law for thi s cycle:law for thi s cycle: W Q QH L!
energy conver s ion efficiency i s :energy conver s ion efficiency i s :
L ! ! !useful work heat input
W Q
Q QQ
H
H L
H
H
L
H
L
T
T
Q
Q!! 11L
E fficiency i s the s ame a s for E fficiency i s the s ame a s for Carnot Cycle but it would beCarnot Cycle but it would be
much lower if regenerationmuch lower if regenerationwere not pre s entwere not pre s ent
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Cylinder Cylinder
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V alveV alve
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4- stroke engine4- stroke engine
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4- stroke engine4- stroke engine
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A ctual Otto cycleA ctual Otto cycle
PP
VV
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A ir - Standard
Power Cycles
A ir - Standard
Power CyclesA ssumptions:A ssumptions:
we analyse a control mass of we analyse a control mass of an ideal gas, meaning.....an ideal gas, meaning.....exh aust and air intake areexh aust and air intake aresubstituted wit h h eat transfer substituted wit h h eat transfer
from t h e system to t h efrom t h e system to t h esurroundingssurroundingscombustion is replaced bycombustion is replaced byh eat transfer from an externalh eat transfer from an externalsource to t h e systemsource to t h e systemall processes are internallyall processes are internallyreversible, meaning....reversible, meaning....
gas specific h eat is constantgas specific h eat is constant
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I deal Otto
Cycle
I deal Otto
CycleA pproximates a spark A pproximates a spark -- ignition engineignition engine
ss
v v
QH
QL
s=const
QH
QL
v=const
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I deal Otto
Cycle (cont.)
I deal Otto
Cycle (cont.)11 s ts t law for thi s cycle:law for thi s cycle: W Q QH L!
energy conver s ion efficiency i s :energy conver s ion efficiency i s :
L ! ! !useful work heat input
W Q
Q QQH
H L
H
L ! ! 1 1 4 13 2
mC
mC L
H
v
v
L ! 11
1
1 4 1
2 3 2
T T T
T T T
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I deal Otto
Cycle (cont.)
I deal Otto
Cycle (cont.)P v const k !for an i s entropic proce ss :for an i s entropic proce ss :
P v P vk k 1 1 2 2!
T
T
V
V
V
V
T
T
k k
2
1
1
2
1
4
3
1
3
4!
!
!
in ca s e of an ideal ga s :in ca s e of an ideal ga s :
T
T
T
T
3
2
4
1
!
L ! ! ! 1 1 11
2
1
2
1
1T
T
V
V r
k
v
k
compre ss ioncompre ss ionratioratio
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I deal Otto Cycle
(cont.)
I deal Otto Cycle
(cont.)
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Otto Cycle (cont.)Otto Cycle (cont.)
Deviations of the Otto cycleDeviations of the Otto cyclefrom an openfrom an open- -cycle spark cycle spark- -ignition engineignition engineCp, Cv increase wit h Cp, Cv increase wit h temperaturetemperature
combustion (incomplete)combustion (incomplete)replaces t h e h eat transfer processreplaces t h e h eat transfer processpressure drop across t h e ex h austpressure drop across t h e ex h austvalvesvalvesh eat transfer between t h e gas andh eat transfer between t h e gas andth e cylinder wallsth e cylinder wallsirreversibility associated wit h irreversibility associated wit h
pressure and temperaturepressure and temperaturegradientsgradients
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s
'
'
'
''
v
Closed Brayton
cycle (cont.)
Closed Brayton
cycle (cont.)QH
QL
s=const
QH
QL
p=const
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Efficiency of a
Brayton cycle
Efficiency of a
Brayton cycle11 s ts t law for thi s cycle:law for thi s cycle: W Q QH L!
energy conver s ion efficiency i s :energy conver s ion efficiency i s :
L ! ! !useful work heat input
W Q
Q QQH
H L
H
L ! ! 1 1 4 13 2
mC T T
mC T T L
H
P
P
L ! 11
1
1 4 1
2 3 2
T T T
T T T
ff fff f
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Efficiency of a
Brayton cycle (cont.)
Efficiency of a
Brayton cycle (cont.)for an i s entropic proce ss :for an i s entropic proce ss :
P P V V k
1 2 2 1!
T
T
P
P
P
P
T
T
k k
k k
2
1
12
1
3
4
3
4
1
! ! !
in ca s e of an ideal ga s :in ca s e of an ideal ga s :
T T
T T
3
2
4
1
!
L ! ! 1 112
1
2
1
T T
P P
k k
PV P V T T 1 1 2 2 1 2!
P v const k !
Effi i fEffi i f
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Efficiency of a
Brayton cycle (cont.)
Efficiency of a
Brayton cycle (cont.)
is entropicis entropic
press
urepress
ureratioratio
L ! 1
1
2 1
1
P P k
k
0
10
20
30
40
50
60
0 5 10 15
P re ssu re ra ti o
Thermal efficiency %
Ex ample 9.6Ex ample 9.6
Th lTh l
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Th e actual gas
turbine process
Th e actual gas
turbine process
s
T
1
42 4s2 s
L compsh h
h h
! 2 12 1
L turbs
h hh h
! 3 43 4
Ex ample 9.7Ex ample 9.7
B t lB t l
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Brayton cycle
with
regeneration
Brayton cycle
with
regeneration
v
P
1 4
2 3
y
s
T
14
2 '
3
2 y
3 '
x
a c d
Effi i fEffi i f
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Efficiency of a
regenerative cycle
Efficiency of a
regenerative cycleL ! ! !net wor
heat in tw
qw w
qH
t c
H
q h h C T T H x P x! ! 3 3
w h h C T T
t P ! ! 3 4 3 4
for an ideal regenerator:for an ideal regenerator:
T T x4
w qt H !
s o:s o:
Effi i fEffi i f
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Efficiency of a
regenerative cycle
Efficiency of a
regenerative cycle
L ! ! 1 1 2 1
3 4
w
w
C T T
C T T
c
t
P
P
1
11
434
121!
T T T
T T T L
for an i s entropic proce ss :for an i s entropic proce ss :
T
T
P
P
P
P
T
T
k
k
k
k 2
1
12
1
3
4
3
4
1
! ! !
4
1
1 T T
!
Closed BraytonClosed Brayton
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heatheate x changer e x changer
Closed Brayton
cycle
Closed Brayton
cycle
22
11 44
turbineturbinecompre ss or compre ss or
W W net net
QQH H
QQLL
heatheate x changer e x changer
33
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Open Brayton cycleOpen Brayton cycle
turbineturbine
e x hau s te x hau s t
compre ss or compre ss or
air intakeair intake
combu s tioncombu s tionchamber chamber
Gas turbine cycleGas turbine cycle
fuelfuel
W W net net
Brayton cycleBrayton cycle
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Brayton cycle
with
regeneration
Brayton cycle
with
regeneration
turbineturbine
e x hau s te x hau s t
compre ss or compre ss or
air air intakeintake
combu s tioncombu s tionchamber chamber
fuelfuel
W W net net
regenerator regenerator
xx
11
22
33
yy
M odified BraytonM odified Brayton
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M odified Brayton
cycle
M odified Brayton
cyclemultimulti --stage compression wit h stage compression wit h intercoolingintercoolingmultimulti --stage expansion wit h stage expansion wit h reh eatreh eat
s
T
3
8
47
1
6
5
2 9
10
M odified BraytonM odified Brayton
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M odified Brayton
cycle
M odified Brayton
cycle
turbine sturbine s
e x hau s te x hau s t
compre ss or scompre ss or s
combu s tioncombu s tionchamber chamber
regenerator regenerator 99
8811
55
66 77
1010
fuelfuel
air air
intakeintake
22 33
intercooler intercooler
44
Brayton cycle forBrayton cycle for
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Brayton cycle for
jet propulsion
Brayton cycle for
jet propulsion
turbineturbine e x hau s te x hau s tcompress or compre ss or
air air intakeintake
combus
tioncombus
tionchamber chamber fuelfuel
22
33
5544
11
Ex ample 9. 10Ex ample 9. 10
Th e DieselTh e Diesel
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Th e Diesel
Cycle
Th e Diesel
Cycle
v
P
14
2
3'
4'
3 3''
s
T
1
42'
3
2 4'
3' 3''
Ideal cycle for the Die s el engineIdeal cycle for the Die s el engine
QH
QL
s=const
v=const
P=const
Th e DieselTh e Diesel
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e Diesel
Cycle(cont.)
e Diesel
Cycle(cont.)
11 s ts t law for thi s cycle:law for thi s cycle: W Q QH L!
energy conver s ion efficiency i s :energy conver s ion efficiency i s :
L ! ! !useful work heat input
W Q
Q QQH
H L
H
L ! ! 1 1 4 13 2
mC T T
mC T T L
H
v
P
L ! 11
1
1 4 1
2 3 2
T T T
k T T T