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    UNIVERSITY OF WEST BOHEMIAFACULTY OF MECHANICAL ENGINEERING

    DEPARTMENT OF POWER SYSTEM ENGINEERING

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    JET ENGINESJET ENGINES

    GAS TURBINESSGAS TURBINESS

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    INTRODUCTION

    In turbines is converted heat and pressureenergy to kinetic energy and mechanical workwith very high efficiency

    The conversion is provided in stator and rotorcanals

    In stator vanes is converted heat and pressure

    energy to kinetic energy In rotor blades is converted heat and pressure

    energy to kinetic energy and mechanical work

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    INTRODUCTION

    Obtained performance on turbines is exploitedfor compressor and assembly drive. In case ofturboshaft engines, performance is also used

    for propeller or rotor drive. Ground power unit use converted energy for

    drive of electric generators or compressors andmany types of equipments.

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    INTRODUCTION

    REQUIREMENTS

    High performance

    High reliability

    High lifetime

    High efficiency

    Minimal weight and dimensions Simple construction and maintenance

    Low price

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    GAS TURBINE TYPES

    TYPES BY DIRECTION OF FLOW

    Radial

    Centrifugal

    Centripetal

    Axial

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    GAS TURBINE TYPES

    Fig. Centrifugal and centripetal gas turbine

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    GAS TURBINE TYPES

    Fig. Parts of centripetal gas turbine

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    GAS TURBINE TYPES

    Fig. Engine with centrifugal compressor and centripetal turbine

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    GAS TURBINE TYPES

    TYPES BY INLET FLOW FIELD

    Turbines with homogeneous inlet flow field

    Turbines with non-homogeneous inlet flow field

    Fig. Turbines with homogeneous and non-homogeneousinlet flow field

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    GAS TURBINE TYPES

    TYPES BY NUMER OF STAGES

    Single stage

    Dual stage

    Triple stage

    Multi stage

    TYPES BY NUMBER OF SPOOLS

    Single spool turbines

    Dual spool turbines

    Triple spool turbines

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    GAS TURBINE TYPES

    Fig. Single stage axial gas turbine

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    GAS TURBINE TYPES

    Fig. Dual stage axial gas turbine

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    GAS TURBINE TYPES

    Fig. Triple stage axial gas turbine

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    GAS TURBINE TYPES

    Fig. Multi (4) stage axial gas turbine2 stages for compressor drive

    2 stages for propeller drive

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    GAS TURBINE TYPES

    Fig. Multi (8) stage axial gas turbine

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    GAS TURBINE TYPES

    TYPES BY REACTION OF STAGE

    Impulse stage

    Impulse/Reaction (Reaction) stage

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    GAS TURBINE TYPES

    Fig. Impulse and reaction stage

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    BASIC PARAMETERS

    Flow rate

    Depends on construciton 0,5-300kg.s -1

    Thermal gradient

    Max. 30kJ.kg-1on one stage

    Temperature before turbine

    Non-cooled turbines max. 1000C Cooled turbines 1200C and more

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    BASIC PARAMETERS

    Fig. Evolution of temperature parameters

    years

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    BASIC PARAMETERS

    RPM (Revolutions per minute)

    Depends on construction 5-90.103 min-1

    Reliability

    Means reliability of blades. At present days in modern enginesits approximately 10000 hours.

    Efficiency

    Single stage turbines 0,82-0,90

    Multi stage turbines 0,88-0,94Cooling air

    Depend on intensity of cooling (approximately 5% from flowrate)

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    BASIC PARAMETERS

    Fig. Dependence of efficiency on flow rate

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    TURBINE STAGE

    Fig. Elementary turbine stage

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    TURBINE STAGE

    Fig. Impulse turbine stage

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    TURBINE STAGE

    Fig. Reaction turbine stage

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    TURBINE STAGE

    Forces on rotor blade are created by:

    Aerodynamic forces created by fluid aroundblades (impulse action of gases)

    Reaction action of gases in convergent rotorblades canal where are gases accelerated

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    TURBINE STAGE

    Fig. Reaction turbine stage

    c3

    ,c

    3

    c3150m.s

    1

    c4= u4 w4

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    TURBINE STAGE

    Work transferred to blades of elementary stagefrom 1kg of gas

    From Euler equation:

    We , st=u '3 . c3' uu4 . c4u[J.kg1

    ]

    since c4u

    0

    We , st=u '3 . c3' uu4 . c4u[J.kg1

    ]

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    TURBINE STAGE

    Fig. Velocity triangles on elementary turbine reaction stage

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    TURBINE STAGE

    Fig. Ideal and real expansion on turbine stage in T-s diagram

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    TURBINE STAGE

    Fig. Real expansion on turbine stage in p-V and T-s diagramshows static and total parameters

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    TURBINE STAGE

    Work on turbine stage

    Efficiency of turbine stage

    We ,st=cp. T3tT4t [J.kg1

    ]

    Wad ,st=c p. T3tT4t , ad [J.kg1]

    st=We ,st

    Wad , st

    [1] st=T

    3tT

    4t

    T3tT4t, ad

    [1]

    st=0.830.89

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    TURBINE STAGE

    Efficiency of multistage turbines is higher thanefficiency of every single stage (in compressorthat's NOT true)

    Efficiency of multistage turbines is 0.88-094 Efficiency increasing by number of turbine

    stages WHY?

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    TURBINE STAGE

    Efficiency of multistage turbines is higher thanefficiency of every single stage (in compressorthat's NOT true)

    Efficiency of multistage turbines is 0.88-094 Efficiency increasing by number of turbine

    stages WHY?

    Lower velocity of gases as in single stage Losses from stage before are exploited in the next

    one

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    TURBINE STAGE

    Reaction of elementary stage

    Is ratio of adiabatic static work of rotor andadiabatic static work of elementary stage

    =hR

    H[1]

    01

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    TURBINE STAGE

    Fig. Impulse and reaction turbine in T-s diagrams

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    LOSSES IN GAS TURBINE

    Profile losses

    in stator and rotor as well

    These losses are generated as soon as gas

    fluid around vanes/blades. Friction losses (boundary layer)

    Shock phenomenas

    Wakes (high angle of atack) Profile losses are higher in rotor

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    LOSSES IN GAS TURBINE

    Secondary losses

    Generated by pair-wakes (induced drag)

    Losses in redial spaces between rotor blade

    and turbine case

    Other losses

    Losses in bearings

    Friction of disks

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    LOSSES IN GAS TURBINE

    Fig. Losses in rotor blade

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    BLADE GEOMETRY

    Characteristic shape of rotor blade is the longitudinalshape

    In elementary stage is determined in the middle diameter( by flow equation )

    The real flow is spatial. The peripheral speed is increasefrom rotor root to rotor tip. Absolute velocity and pressurechanged as well. All of these parameters are connected

    The real flow is spatial, compressible, viscous and

    non-stationary

    GEOMETRY of blade must accepted these facts

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    BLADE GEOMETRY

    Fig. Geometric solution of rotor blade construction

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    BLADE GEOMETRY

    Fig. Reaction rotor blade construction

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    BLADE GEOMETRY

    Fig. Creating rotor back with lemniscate

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    BLADE GEOMETRY

    Fig. Creating a impulse rotor blade

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    MULTISTAGE GAS TURBINE

    Created by compiling of turbine stages in a row

    Modern engines used 6 and more stageturbines because:

    There are high thermal gradients Higher efficiency

    Better collaboration with compressor ( biggerdiameter lower RPM )

    Smooth shape of engine

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    MULTISTAGE GAS TURBINE

    Fig. Shape of overflow canal

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    MULTISTAGE GAS TURBINE

    Fig. Parameters through the multistage impulse turbine

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    MULTISTAGE GAS TURBINE

    Fig. Thermal gradient distribution on multistage turbine

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    TURBINE CHARACTERISTIC

    Fig. Gas turbine characteristic

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    TURBINE CHARACTERISTIC

    Fig. Gas turbine characteristic

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    STATOR VANES

    Fig. Tubular stator vanes

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    STATOR VANES

    Fig. Stator vanes

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    ROTOR BLADES

    Fig. Turbine rotor blades

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    ROTOR BLADES

    Fig. Turbine double-rotor blades

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    ROTOR BLADES

    Fig. Turbine double-floor rotor blades

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    MULTISTAGE GAS TURBINE

    Fig. Double-stage gas turbine

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    MULTISTAGE GAS TURBINE

    Fig. Scheme of double-stage gas turbine

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    MULTISTAGE GAS TURBINE

    Fig. Double-stage gas turbine

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    MULTISTAGE GAS TURBINE

    Fig. 'Free' gas turbine

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    MULTISTAGE GAS TURBINE

    Fig. Triple-stage gas turbine

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    MULTISTAGE GAS TURBINE

    Fig. Four-stage gas turbine

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    GAS TURBINE COOLING

    Fig. Thermal and mechanical load blades

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    GAS TURBINE COOLING

    Fig. Rotor blade damaged by thermal load

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    GAS TURBINE COOLING

    Fig. Stator vanes damaged by thermal load

    Thermal damage of pressure sideof stator blade

    Cracks on cooledstator blade

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    GAS TURBINE COOLING

    Fig. Evolution of temperature increasingin depends on used material

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    GAS TURBINE COOLING

    Sources of cooling

    Air from fan

    Air from low pressure compressor

    Air from secondary flow on CC

    Air from secondary flow ( turbofan engines )

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    GAS TURBINE COOLING

    Fig. Turbine cooling

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    GAS TURBINE COOLING

    Fig. Multi-stage turbine cooling

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    GAS TURBINE COOLING

    Fig. Distribution of cooling air in turbine stage

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    BLADES COOLING

    Methods of blade cooling Convective ( Internal cooling )

    Film cooling

    Transpiration cooling

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    BLADES COOLING

    Film cooling Cooling is provided

    with cooling air, which

    is delivered throughthe holes on the bladesurface.

    Cooling with air film is

    more efficient asconvective cooling

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    BLADES COOLING

    Transpiration cooling Transpiration cooling is similar technique of

    cooling as cooling with air film.

    In this case is generated a homogeneoussurface of cooling air on surface of blade

    Transpirationally cooled blades have no holes.

    Air flow through the porous surface of blade.

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    BLADES LOAD

    Fig. Turbine rotor blades load

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    REFERENCES

    Otis, Vosbury: Aircraft gas turbine powerplants Jeppesen: 2002

    Rolls royce The jet engine, 1996

    Hanus D., Marlek J, : Studijn modul 15,Turbnov motor, CERM, s.r.o. Brno 2004

    Kadrnoka J.: Tepeln turbny a

    turbokompresory, CERM, s.r.o. Brno 2004

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    DISCUSSION...

    ...QUESTIONS