8
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 the steam 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 = 0.793 X4 = 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 '1th = -q::- -3171. 78 kJ /kg = 165 kg/s (c) m= , , t ;; , ~ , i , ! I ~ J

qin ~J, )~~/ 1 qOUl · h2 = hl + W p.in = 191.83 + 10.09 = 201.92 kJ/kg P3 = 10 MPa s 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

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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 .

    ...