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    Air-Standard Cycles

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    Higher ratios produce

    autoignition andknocking

    Analysis of Otto cycleAnalysis of Otto cycle

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    Air

    Combustion

    mixture

    He

    Analysis of Otto cycleAnalysis of Otto cycle

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    5

    Analysis of Otto cycleAnalysis of Otto cycle

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    Analysis of Otto cycle

    Thermal efficiency vs. compression ratio for

    different values of the adiabatic exponent

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    Analysis of Otto cycle

    Thermal efficiency vs. compression ratio for

    different values of the adiabatic exponent

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    Analysis of Otto cycle

    Thermal efficiency vs. compression ratio for

    different values of the adiabatic exponent

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    Analysis of Otto cycle

    ( ) ( ) ( ) ( )1 1 1

    1 1m

    p rp

    r

    = +

    ( )

    ( ) ( )1

    1

    1 1m

    p rp

    r

    =

    1=

    Mean effective pressure vs. pressure ratio for different values of

    compression ratio r.

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    5. Analysis of Diesel cycle

    ( ) ( )11

    11 1r

    =

    +

    For dual cycle, thermal efficiency has been

    defined as

    is used for thermal efficiency of Diesel

    cycle. We get

    (.1!"

    #

    1p

    p= =

    ( )11 11

    1r

    =

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    5. Analysis of Diesel cycle

    Figure $.# Thermal efficiency vs. cut%off

    ratio at different compression ratios and

    adiabatic exponents.

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    5. Analysis of Diesel cycle

    Mean effective

    pressure,

    ( ) ( ) ( ) ( )1 1 1

    1 1m

    p rp

    r

    = +

    1=

    ( ) ( ) ( )1 1

    1 1m

    p rpr

    =

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    6. Comparison of the cycles

    The significant parameters in cycle analysis are compression

    ratio, pea& pressure, pea& temperature, heat addition, heat

    re'ection, and the net or&. )n order to compare the

    performance of these cycles, some of the parameters are &eptfixed.

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    6. Comparison of the cycles

    6.1. For the same compression ratio and heat addition

    Figure *.1. p%+ and T%s diagrams having the same compression

    ratio and heat addition for the three cycles.

    Otto Dual Diesel > >

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    6. Comparison of the cycles

    6.2. For the same compression ratio and heat rejection

    Figure *.#. p%+ and T%s diagrams having the same compression

    ratio and heat re'ection for the three cycles.

    Otto Dual Diesel > >

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    6. Comparison of the cycles

    6.3. For the same same peak pressure, peak temperature

    and heat rejection

    Figure *.. p%+ and T%s diagrams having the same pea&

    pressure, pea& temperature and heat re'ection for the three

    cycles.Diesel Dual Otto > >

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    6. Comparison of the cycles

    6.4. For the same maximum pressure and heat input

    Figure *.. p%+ and T%s diagrams having the same maximum

    pressure and heat input for the three cycles.

    Diesel Dual Otto > > (for the same,1Q

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    6. Comparison of the cycles

    6.6. For the same maim!m press!re and "or# o!tp!t

    Figure *.-. T%s diagrams having the same maximum pressure

    and heat input for the three cycles.

    Diesel Dual Otto > >

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    The net cycle work of an engine can be increased by either:

    i) Increasing ther!"#)ii) Increase Qin#$%)

    &

    '# '!

    QinWcycle

    !

    #

    $

    i)

    (

    ii)

    Factors Affecting Work per Cycle

    !"

    ("

    (""

    $""th

    incycle

    r

    r

    V

    Q

    VV

    Wimep

    =

    =1

    1#1

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    Effect of Compression Ratio on Thermal Efficiency and ME

    =

    k

    in

    rr

    r

    VP

    Q

    P

    imep 11

    1111

    k ! "#$

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    /0T)23

    Than& you for your attention