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Chapter 9 Vapor and Combined Power Cycles
9-16 A steam power plant that operates on a simple ideal Rankine cycle is considered. The quality of thesteam at the turbine exit, the thermal efficiency of the cycle, and the mass flow rate of the steam are to be
determined.
Assumptions 1 Steady operating conditions exist. 2 Kinetic and potential energy changes are negligible.
Analysis (a) From the steam tables (Tables A-4, A-S, and A-6),
hl = hf@ IOkPa = 191.83 kJ/kg T
VI =Vf@IOkPa =O.OO101m3/kg
3/
~
lkJ ...qin
~J,
)~~/ 1 qOUl ""'
Wp.in = VI(P2 -PI)
= ~.00101 m3/kg}10.000-10kPa{ ~\I kPa.m
= 10.09kJ/kg
h2 = hl + wp.in = 191.83+ 10.09 = 201.92 kJ/kg
PJ = 10 MPa hJ = 3373.7 kJ/kg
TJ =500°C JsJ =6.5966kJ/kg.K
s
P4 = 10 kPa
S4 = S3
~ = 6.5966- 0.6493 = 0.793X4 =
Sfg 7.5009
h4 = h f + x4h fg = 191.83 + (0.793 X2392.8 ) = 2089.3 kJ/kg
(b) qin = h3 -~ = 3373.7- 201.92 = 3171.78 kJ/kg
qout = h4 -hl = 2089.3-191.83 = 1897.47 kJ/kg
wne( = qin -qOU( = 3171.78 -1897.47 = 1274.31 kJ /kg
and
Ulrt -1274.31 kJ /kg = 4Q2>/o'1 th = -q::- -3171. 78 kJ /kg
= 165 kg/s(c) m=
,,t;;,~,
i,!
I~J
Chapter 9 Vapor and Combined Power Cycles
vqin
2~//!V IOkPa
4s 4J-qOUl
9-23 A steam power plant operates on a simple non ideal Rankine cycle between the specified pressurelimits. The thermal efficiency of the cycle, the mass flow rate of the steam, and the temperature rise of thecooling water are to be determined.
Assumptions 1 Steady operating conditions exist. 2 Kinetic and potential energy changes are negligible.
Analysis (a) From the steam tables (Tables A-4, A-5, and A-6),
Thl = hf@ IOkPa = 191.83 kJ/kg
VI =Vf@IOkPa =0.00101 m3/kg
Wp,in =VI(P2 -PI)/1lp
= (0.00101 m3/kg)7,000-10 kPa { -1:!!, 1/(0.87)\ 1 kPa .m )
= 8.11 kJ/kg
h2 =hl +Wp,in =191.83+8.11=199.94kJ/kg
PJ = 7 MPa } hJ = 3410.5 kJ/kgTJ = 500°C $3 = 6.7975 kJ/kg .K
P4 = 10 kPa
S4 = S3
!!1::.!!!-
h3 -h4.,
T]T = ~ h4 = h3 -1lT (h3 -h4., )
= 3410.5- (0.87X3410.5 -2153.93) = 2317.28 kJ/kg
Thus,
and
qin = h3 -h2 = 3410.5 -199.94 = 3210.56 kJ Ikg
qout = h4 -hl = 2317.28 -191.83 = 2125.45 kJ Ikg
Wnet = qin -qout = 3210.56- 2125.45 = 1085.11 kJ Ikg
U1Et 1005.11 kJ /kg1]1h = -= = 3l.8:1/ol1in ~10.ffi kJ /kg
45.(00 kJ /s(b) fn- ~ --Utrl -1005.11 kJ /kg
(c) The rate of heat rejection to the cooling water and its temperature rise are
QOUI = mqoul = (41.5 kg/sX2125.45 kJ/kg)= 88,143 kJ/s
LlT = Qout = 88,143 kJ/s = 1054°Ccoo1lngwater ( . ) ( 00 X kJ oC) . mC cooling water 2 O kg/s 4.18 /kg .
= 41.5 kg /s
9-13
Chapter 9 Vapor and Combined Power Cycles
~
5
32
//
9.30 A steam power plant that operates on the ideal reheat Rankine cycle is considered. The quality (or
temperature, if superheated) of the steam at the turbine exit, the thermal efficiency of the cycle, and themass flow rate of the steam are to be determined.
Assumptions 1 Steady operating conditions exist. 2 Kinetic and potential energy changes are negligible.
Analysis (a) From the steam tables (Tables A-4, A-S, and A-6),
hl = h I@' 10 kPa = 191.83 kJ/kg T
VI =:vI@ 10kPa = 0.00101 m3/kg
w p.in = VI (P2 -~ ) ,
= ~.00101 m3/kg}10,000-10kPa{ ~-~ -
\lkPa.m= 10.09 kJ/kg
h2 = hl + W p.in = 191.83 + 10.09 = 201.92 kJ/kg
sP3 = 10 MPa
T 3 = 500°C
h3 = 3373.7 kJ/kg
53 = 6.5966 kJ/kg .K
P6 = 10 kPa
S6 = Ss
(b) WT,ou! = (h3 -h4 )+ (h5 -h6 ) = 3373.7 -2782.5 + 3478.5- 2460.2 = 1609.5 kJ/kg
qin = (h3 -h2 )+ (h5 -h4 ) =3373.7 -201.92 + 3478.5- 2782.5 = 3867.78 kJ/kg
Wnet = WT.out -W p,in = 1609.5 -10.09 = 1599.41 kJ/kg
.w:m=~=
UlEt
OO.(XX) kJ /s
IW3.41 kJ /kg= 50.0 kg Is
9-17
Chapter 9 Vapor and Combined Power Cycles
5
4
~
l-y
7
MPa
~~j( 20 kPa \~,,-~
II q.:;,
9-38 A steam power plant that operates on an ideal regenerative Rankine cycle with an open feed waterheater is considered. The net work output per kg of steam and the thermal efficiency of the cycle are to bedetermined.
Assumptions 1 Steady operating conditions exist. 2 Kinetic and potential energy changes are negligible.
Analysis (a) From the steam tables (Tables A-4, A-5, and A-6),
ThJ = hf@ ZOkPa = 251.40 kJ/kg
3VI =vf@ZOkPa =0.001017 m /kg
wpl.in = Vl(PZ -PJ)
= ~.001017 m3/kg}400- 20 kPa { ~! 31
\lkPa.m= 0.39 kJ/kg
hz = hJ + wpl,in = 251.40+0.39 = 251.79 kJ/kg
P3 = 0.4 MPa h3 = h f@ 04 MPa = 604.74 kJ/kg
sat.liquid .V3 = V f@ 04 MPa = 0.001084 m3/kg
Wpl/jn = V3(P4 -P3)
= (0.001084 m3/kg}6000-400 kPa { ~
= 6.07 kJ/kg \ kPa .m
h4 = h3 + w pl/jn = 604.74 + 6.07 = 610.81 kJ/kg
lkJ
P5 =6MPa
T 5 = 450°C
h5 = 3301.8 kJ/kg
S5 = 6.1193 kJ/kg .K
6.7193-1.7766$6 -$ fP6 =0.4 MPalx6 ===0.9655
~ $ fg 5.1193$6 = $S
h6 =hf +x6hfg =604.74+(0.9655X2133.8)=2664.93kJ/kg
6.7193-0.8320S7 -S fP7 =20kPa }X7 =-;;:-= 7.0766S7 = s5
( X )h7 =hf +x7hfg =251.40+ 0.8319 2358.3 =2213.3kJ/kg
The fraction of steam extracted is determined from the steady-flow energy balance equation applied to the
feed water heater. Noting that Q = W = Me = f1pe = 0 ,
.Mh' "
= 0.8319
E E -A 1:' ",v\sleaay) -Oin -out -ilLs)'stem -
Ein = Eout
Lni;hi = Lniehe ~ ni6h6 + ni2h2 = ni3h3 ~ yh6 + (1- y }112 = l(h3)
where y is the fraction of steam extracted from the turbine ( = ni6 / ni3 ). Solving for y,
h3 -hz ---
y-~-hz
604.74 -251.79
2664.93-251.79= 0.1463
Then,
qin = h5 -h4 = 3301.8 -610.81 = 2691.0 kJ/kg
qout = (1- y Xh7 -hi ) = (1- 0. 1463X2213.3 -251.4) = 1674.9 kJ/kg
9-21
1Chapter 9 Vapor and Combined Power Cycles
Wnet = qin -qout = 2691.0 -1674.9 = 1016.1 kJ I kg
(b) The thermal efficiency is determined from
TJth = 1-i2!!L = 1- 1674.9 kJ Ikg = 37.8%
qin 2691.0 kJ Ikg
~
and
!!.
~~
Chapter 9 Vapor and Combined Power Cycles
/
1~ "/7l-y
9-43 A steam power plant operates on an ideal reheat-regenerative Rankine cycle with an open feedwater
heater. The mass flow rate of steam through the boiler and the thermal efficiency of the cycle are to be
determined.
Assumptions 1 Steady operating conditions exist. 2 Kinetic and potential energy changes are negligible.
Analysis (a) From the steam tables (Tables A-4, A-S, and A-6), T ,
hi = hf@ IOkPa = 191.83 kJ/kg
3vI=vf@IOkPa=0.00101m/kg :
Wpl.in = Vi(P2 -PI)= (0.00101 m3/kg)800-10kPa{ ~
\1 kPa.m= 0.80 kJ/kg
h2 =hl +Wpl,in =191.83+0.80=192.63kJ/kg
8PJ = 0.8 MPa 1 hJ = hf@ O.8MPa = 721.11 kJ/kg
sat.liquid Is
lkJ
3
5
6
'-l.:.
7l-y
I 8
V3 [email protected] =0.001115 m3/kg
Wpl/~n = V3(P4 -P3)= ~.001115 m3/kg)10,000- 800 kPa { -
= 10.26 k1/kg \ 1 kPa .m
h4 = h3 + w pl/ ~n = 721.11 + 10.26 = 731.37 k1/kg
P5 = 10 MPa h5 = 3500.9 k1/kg
T5 = 550°C s5 = 6.7561 kJ/kg. K
P6 = 0.8 MPa } h6 = 2811.9 kJ/kgS6 = S5
P7 = 0.8 MPa 1 -
T 7 = 500°C
6
~~:n ~.
-.::-J.
13
4
2
-0~-::--~Pg = 10 kPa
Sg = S7
h7 = 3480.6 kJ/kg
.S7 = 7.8673 kJ/kg. K
X8 =~=!.8673-Q.6493=0.9623s fg 7.5009
h8 = h f + x8h fg = 191.83 + (0. 9623X2392.8) = 2494.4 kJ/kg
The fraction of steam extracted is determined from the steady-flow energy balance equation applied to the
feed water heaters. Noting that Q = W = Me = Llpe = O .
E. E.."O(sle.dy) ..in -OUI = !J.Esyslem = 0 ~ Ein = Eoul
Lniihi = Lniehe --+ ni6h6 + ni2h2 = ni3h3 ---+ yh6 + (1- y }JI2 = l(h3)
where y is the fraction of stearn extracted from the turbine ( = ~ / ~ ). Solving for y,
=~= 721.11-192.63 =0.2018y h6 -~ 2711.9-192.63
qin = (h5 -h4)+ (1- y Xh7 -h6 ) = (3500.9- 731.37)+ (1- 0.2098X3480.6 -2811.9) = 3297.9 kJ/kg
qoul = (1- y Xh8 -h1 )= (1- 0.2098X2494.4 -191.83) = 1819.5 kJ/kg
~'net = qin -qout = 3297.9 -1819.5 = 1478.5 kJ/kg
.Wm 8),00) ~ /sm=-=
lqa
Then,
and 1478.4kJ/kg = 54.1 kg /s
-1478.4 kJ/kgWnet(b) 77lh = -=- "" = 44.8%
3297.9 kJ/kg
9-29
Chapter 9 Vapor and Combined Power Cycles
9.84 An ideal reheat-regenerative Rankine cycle with one open feedwater heater is considered. The fraction
of steam extracted for regeneration and the thermal efficiency of the cycle are to be determined.
Assumptions 1 Steady operating conditions exist. 2 Kinetic and potential energy changes are negligible.
Analysis
-5 I -J,
T I5
~6
7~
6 l-yI 7
y/iI 0.6 MPa /-
4
2
~
3
-&~ 9 s(a) From the steam tables (Tables A-4, A-5, and A-6),
hi = hf @ 15kPa = 225.94 kJ/kg
VI =Vf@15kPa =0.001014 m3/kg
PJ = 0.6 MPa
sat.liquid
h3 = h f @ 0.6 MPa = 670.56 kJ/kg
V3 =Vf@06MPa =0.001101 m3fkg
P5 = 10 MPa } h5 = 3373.7 kJ/kgT5 = 500°C S5 = 6.5966 kJ/kg .K
P9 = 15 kPa
S9 = S7
9-63
Chapter 9 Vapor and Combined Power Cycles
The fraction of steam extracted is determined from the steady-flow energy balance equation applied to the
feedwater heaters. Noting that Q = W = Me = ~e = O .
...