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Impact of fuel supply impedance and fuel staging on gas turbine ...

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Introducti<strong>on</strong><br />

perfect premixed combusti<strong>on</strong><br />

Air + Fuel<br />

Fuel<br />

n<strong>on</strong>- premixed combusti<strong>on</strong><br />

Air<br />

practical premixed combusti<strong>on</strong><br />

Fuel Fuel<br />

Air<br />

Figure 1.3: Sketch <str<strong>on</strong>g>of</str<strong>on</strong>g> premixed, n<strong>on</strong>-premixed <str<strong>on</strong>g>and</str<strong>on</strong>g> practical premixed combusti<strong>on</strong><br />

systems<br />

A general ”c<strong>on</strong>diti<strong>on</strong>” arises from the geometric extensi<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> the c<strong>on</strong>sidered<br />

combusti<strong>on</strong> system in relati<strong>on</strong> to the wavelength <str<strong>on</strong>g>of</str<strong>on</strong>g> interest. The flame resp<strong>on</strong>se<br />

exhibits low pass filter behavior in the frequency domain with a cut-<str<strong>on</strong>g>of</str<strong>on</strong>g>f<br />

frequency. For the combusti<strong>on</strong> system analyzed, this frequency lies between<br />

400 Hz <str<strong>on</strong>g>and</str<strong>on</strong>g> 800 Hz. The maximum frequency can then be restricted to 1000 Hz<br />

in the present work. In additi<strong>on</strong>, the burner c<strong>on</strong>figurati<strong>on</strong> examined exhibits<br />

small radial <str<strong>on</strong>g>and</str<strong>on</strong>g> circumferential extensi<strong>on</strong>s compared to the wavelength. The<br />

problem can therefore be reduced to <strong>on</strong>e-dimensi<strong>on</strong>al acoustics.<br />

14

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