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    MAJOR COMBUSTOR COMPONENTS

    Compressor

    Tu

    rbine

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    MAJOR COMBUSTOR COMPONENTS

    Key Questions:

    Why is combustor configured this way?

    What sets overall length, volume and geometry of device?

    Compre

    ssor

    Tu

    rbine

    Fuel

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    COMBUSTOR EXAMPLE (F101)

    Henderson and Blazowski

    Fuel

    Compressor

    Turb

    ine

    NG

    V

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    VORBIX COMBUSTOR (P&W)

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    COMBUSTOR REQUIREMENTS

    Complete combustion (hb 1)

    Low pressure loss (pb 1)

    Reliable and stable ignition Wide stability limits

    Flame stays lit over wide range of p, u, f/a ratio)

    Freedom from combustion instabilities

    Tailored temperature distribution into turbine with no hot spots Low emissions

    Smoke (soot), unburnt hydrocarbons, NOx, SOx, CO

    Effective cooling of surfaces

    Low stressed structures, durability

    Small size and weight

    Design for minimum cost and maintenance

    Futuremultiple fuel capability (?)

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    CHEMISTRY REVIEW

    OHmnCOOmnHC mn 22224

    478.4

    1

    m

    n

    s

    22222

    478.3

    278.3

    4N

    mnOH

    mnCONO

    mnHC mn

    Stoichiometric Molar fuel/air ratio Stoichiometric Mass fuel/air ratio

    General hydrocarbon, CnHm (Jet fuel H/C~2)

    Complete oxidation, hydrocarbon goes to CO2 and water

    For air-breathing applications, hydrocarbon is burned in air

    Air modeled as 20.9 % O2 and 79.1 % N2 (neglect trace species)

    Complete combustion for hydrocarbons means all C CO2and all H H2O

    2878.3324

    12

    mn

    mns

    Stoichiometric = exactly correct ratio for complete combustion

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    COMMENTS ON CHALLENGES

    Based on material limits of turbine (Tt4), combustors must operate below

    stoichiometric values

    For most relevant hydrocarbon fuels, s~ 0.06 (based on mass)

    Comparison of actual fuel-to-air and stoichiometric ratio is called equivalence ratio

    Equivalence ratio = f = /stoich

    For most modern aircraft f ~ 0.3

    Summary

    Iff = 1: Stoichiometric

    Iff > 1: Fuel Rich

    Iff < 1: Fuel Lean

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    VARIATION OF FLAME TEMPERATURE WITH f

    FlameTem

    perature

    Flammability LimitsStill too hot

    for turbine

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    WHY IS THIS RELEVANT?

    Most mixtures will NOT burn so far away fromstoichiometric

    Often called Flammability Limit

    Highly pressure dependent

    Increased pressure, increasedflammability limit

    Requirements for combustion, roughly f > 0.8

    Gas turbine can NOT operate at (or even near)stoichiometric levels

    Temperatures (adiabatic flame temperatures)associated with stoichiometric combustion areway too hot for turbine

    Fixed Tt4 implies roughly f < 0.5

    What do we do?

    Burn (keep combustion going) nearf=1 withsome of compressor exit air

    Then mix very hot gases with remaining air tolower temperature for turbine

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    SOLUTION: BURNING REGIONS

    Air

    Compressor

    Turbine

    f ~ 1.0

    T>2000 K

    f~0.3

    Primary

    Zone

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    COMBUSTOR ZONES: MORE DETAILS

    1. Primary Zone

    Anchors Flame

    Provides sufficient time, mixing, temperature for complete oxidation of fuel Equivalence ratio nearf=1

    2. Intermediate (Secondary Zone)

    Low altitude operation (higher pressures in combustor)

    Recover dissociation losses (primarily CO CO2) and Soot Oxidation

    Complete burning of anything left over from primary due to poor mixing High altitude operation (lower pressures in combustor)

    Low pressure implies slower rate of reaction in primary zone

    Serves basically as an extension of primary zone (increased tres)

    L/D ~ 0.7

    3. Dilution Zone (critical to durability of turbine) Mix in air to lower temperature to acceptable value for turbine

    Tailor temperature profile (low at root and tip, high in middle)

    Uses about 20-40% of total ingested core mass flow

    L/D ~ 1.5-1.8

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    COMBUSTOR DESIGN

    Combustion efficiency, hb = Actual Enthalpy Rise / Ideal Enthalpy Rise

    h=heat of reaction (sometimes designated as QR) = 43,400 KJ/Kg

    34 tt

    Rb

    P TTQ

    cf

    h

    General Observations:1. hb as p and T (because of dependency of reaction rate)

    2. hb as Mach number (decrease in residence time)

    3. hb as fuel/air ratio

    Assuming that the fuel-to-air ratio is small

    hm

    TmTmmc

    f

    tatfaP

    b

    34 h

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    COMBUSTOR TYPES (Lefebvre)

    Single Can

    Tubular

    or Multi-Can

    Tuboannular

    Can-Annular

    Annular

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    COMBUSTOR TYPES (Lefebvre)

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    EXAMPLES

    CAN-TYPERolls-Royce Dart

    ANNULAR-TYPEGeneral Electric T58

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    EXAMPLES

    CAN-ANNULAR-TYPE

    Rolls-Royce Tyne

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    CHEMICAL EMISSIONS

    Aircraft deposit combustion products at high altitudes, into upper troposphere and

    lower stratosphere (25,000 to 50,000 feet)

    Combustion products deposited there have long residence times, enhancing impact NOx suspected to contribute to toxic ozone production

    Goal: NOx emission level to no-ozone-impact levels during cruise

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    AFTERBURNER (AUGMENTER)

    Spray in more fuel to use up more oxygen

    Main combustion can not use all air

    Exit Mach number stays same (choked Mexit = 1) Temp

    Speed of sound

    Velocity = M*a

    Therefore Thrust

    Penalty:

    Pressure is lower so thermodynamic efficiency is poor

    Propulsive efficiency is reduced (but dont really care in this application)

    As turbine inlet temperature keeps increasing less oxygen downstream for AB and

    usefulness decreases Requirements

    VERY lightweight

    Stable and startable

    Durable and efficient

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    RELATIVE LENGTH OF AFTERBURNER

    Why is AB so much longer than primary combustor?

    Pressure is so low in AB that they need to be very long (and heavy)

    Reaction rate ~ pn (n~2 for mixed gas collision rate)

    J79 (F4, F104, B58)

    Combustor Afterburner

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    INTRA-TURBINE BURNING

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    BURNER-TURBINE-BURNER (ITB) CONCEPTS

    Improve gas turbine engine performance using an interstage turbine burner (ITB)

    With a higher specific thrust engine will be smaller and lighter

    Increasing payload

    Reduce CO2 emissions

    Reduce NOx emissions by reducing peak flame temperature

    Initially locate ITB in transition duct between high pressure turbine (HTP) and low

    pressure turbine (LPT)

    Conventional

    Intra Turbine Burner (schematic only)

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    SIEMENS WESTINGHOUSE ITB CONCEPT

    Tt4

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    UNDERSTANDING BENEFIT FROM CYCLE ANALYSISFrom Turbojet and Turbofan Engine Performance Increases Through Turbine Burners, by

    Liu and Sirignano, JPP Vol. 17, No. 3, May-June 2001

    Conventional Intra Turbine Burner

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    2 additional burners 5 additional burners

    UNDERSTANDING BENEFIT FROM CYCLE ANALYSISFrom Turbojet and Turbofan Engine Performance Increases Through Turbine Burners, by

    Liu and Sirignano, JPP Vol. 17, No. 3, May-June 2001

    Continuous burning

    in turbine