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    Thermoacoustic Modeling of a Gas Turbine Using Transfer Functions Measured Under Full Engine Pressure

    Source: Journal of Engineering for Gas Turbines and Power:;2010:;volume( 132 ):;issue: 011::page 111503
    Author:
    Bruno Schuermans
    ,
    Daniel Guyot
    ,
    Christian Oliver Paschereit
    ,
    Felix Guethe
    ,
    Douglas Pennell
    DOI: 10.1115/1.4000854
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Thermoacoustic transfer functions of a full-scale gas turbine burner operating under full engine pressure have been measured. The excitation of the high-pressure test facility was done using a siren that modulated a part of the combustion airflow. Pulsation probes have been used to record the acoustic response of the system to this excitation. In addition, the flame’s luminescence response was measured by multiple photomultiplier probes and a light spectrometer. Three techniques to obtain the thermoacoustic transfer function are proposed and employed: two acoustic-optical techniques and a purely acoustic technique. The first acoustical-optical technique uses one single optical signal capturing the chemiluminescence intensity of the flame as a measure for the heat release in the flame. This technique only works if heat release fluctuations in the flame have only one generic source, e.g., equivalence ratio or mass flow fluctuations. The second acoustic-optical technique makes use of the different response of the flame’s luminescence at different optical wavelengths bands to acoustic excitation. It also works, if the heat release fluctuations have two contributions, e.g., equivalence ratio and mass flow fluctuation. For the purely acoustic technique, a new method was developed in order to obtain the flame transfer function, burner transfer function, and flame source term from only three pressure transducer signals. The purely acoustic method could be validated by the results obtained from the acoustic-optical techniques. The acoustic and acoustic-optical methods have been compared and a discussion on the benefits and limitations of each is given. The measured transfer functions have been implemented into a nonlinear, three-dimensional, time domain network model of a gas turbine with an annular combustion chamber. The predicted pulsation behavior shows a good agreement with pulsation measurements on a field gas turbine.
    keyword(s): Acoustics , Transfer functions , Flames , Signals , Modeling , Pressure , Combustion chambers , Engines AND Gas turbines ,
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      Thermoacoustic Modeling of a Gas Turbine Using Transfer Functions Measured Under Full Engine Pressure

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    http://yetl.yabesh.ir/yetl1/handle/yetl/143046
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    contributor authorBruno Schuermans
    contributor authorDaniel Guyot
    contributor authorChristian Oliver Paschereit
    contributor authorFelix Guethe
    contributor authorDouglas Pennell
    date accessioned2017-05-09T00:37:27Z
    date available2017-05-09T00:37:27Z
    date copyrightNovember, 2010
    date issued2010
    identifier issn1528-8919
    identifier otherJETPEZ-27141#111503_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/143046
    description abstractThermoacoustic transfer functions of a full-scale gas turbine burner operating under full engine pressure have been measured. The excitation of the high-pressure test facility was done using a siren that modulated a part of the combustion airflow. Pulsation probes have been used to record the acoustic response of the system to this excitation. In addition, the flame’s luminescence response was measured by multiple photomultiplier probes and a light spectrometer. Three techniques to obtain the thermoacoustic transfer function are proposed and employed: two acoustic-optical techniques and a purely acoustic technique. The first acoustical-optical technique uses one single optical signal capturing the chemiluminescence intensity of the flame as a measure for the heat release in the flame. This technique only works if heat release fluctuations in the flame have only one generic source, e.g., equivalence ratio or mass flow fluctuations. The second acoustic-optical technique makes use of the different response of the flame’s luminescence at different optical wavelengths bands to acoustic excitation. It also works, if the heat release fluctuations have two contributions, e.g., equivalence ratio and mass flow fluctuation. For the purely acoustic technique, a new method was developed in order to obtain the flame transfer function, burner transfer function, and flame source term from only three pressure transducer signals. The purely acoustic method could be validated by the results obtained from the acoustic-optical techniques. The acoustic and acoustic-optical methods have been compared and a discussion on the benefits and limitations of each is given. The measured transfer functions have been implemented into a nonlinear, three-dimensional, time domain network model of a gas turbine with an annular combustion chamber. The predicted pulsation behavior shows a good agreement with pulsation measurements on a field gas turbine.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleThermoacoustic Modeling of a Gas Turbine Using Transfer Functions Measured Under Full Engine Pressure
    typeJournal Paper
    journal volume132
    journal issue11
    journal titleJournal of Engineering for Gas Turbines and Power
    identifier doi10.1115/1.4000854
    journal fristpage111503
    identifier eissn0742-4795
    keywordsAcoustics
    keywordsTransfer functions
    keywordsFlames
    keywordsSignals
    keywordsModeling
    keywordsPressure
    keywordsCombustion chambers
    keywordsEngines AND Gas turbines
    treeJournal of Engineering for Gas Turbines and Power:;2010:;volume( 132 ):;issue: 011
    contenttypeFulltext
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