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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

    QQ

    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

    QQ

    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

    QQ

    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