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

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A.2 Estimati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the optimum number <str<strong>on</strong>g>of</str<strong>on</strong>g> circumferential injecti<strong>on</strong> holes<br />

A.2 Estimati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the optimum number <str<strong>on</strong>g>of</str<strong>on</strong>g> circumferential injecti<strong>on</strong><br />

holes<br />

The optimum number <str<strong>on</strong>g>of</str<strong>on</strong>g> circumferential holes was estimated according to<br />

Holdeman et al. [45] using the relati<strong>on</strong><br />

C = S H<br />

√<br />

J, (A.6)<br />

where S denotes the spacing <str<strong>on</strong>g>of</str<strong>on</strong>g> the holes <str<strong>on</strong>g>and</str<strong>on</strong>g> H corresp<strong>on</strong>ds to the height <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

rectangular duct. C represents a c<strong>on</strong>stant with an optimum value <str<strong>on</strong>g>of</str<strong>on</strong>g> 2.5. For a<br />

cylindrical duct the spacing amounts to S = 2πR/n with n being the number<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> holes. Therefore the number <str<strong>on</strong>g>of</str<strong>on</strong>g> holes can be calculated by the following<br />

equati<strong>on</strong>:<br />

n= 2πR √<br />

J.<br />

H<br />

(A.7)<br />

In case <str<strong>on</strong>g>of</str<strong>on</strong>g> a cylindrical duct the height can be substituted by the radius using<br />

the relati<strong>on</strong> R = H/ 2. For the analyzed case the radius can be determined<br />

by the outer radius or the difference between the outer radius <str<strong>on</strong>g>and</str<strong>on</strong>g> the inner<br />

radius <str<strong>on</strong>g>of</str<strong>on</strong>g> the mixing secti<strong>on</strong>. The optimum number <str<strong>on</strong>g>of</str<strong>on</strong>g> injecti<strong>on</strong> holes can then<br />

be calculated <str<strong>on</strong>g>and</str<strong>on</strong>g> lies in the range between 6.1 <str<strong>on</strong>g>and</str<strong>on</strong>g> 10.2.<br />

A.3 Main flow parameters <str<strong>on</strong>g>and</str<strong>on</strong>g> structure <str<strong>on</strong>g>of</str<strong>on</strong>g> the acoustic network<br />

models<br />

The following tables represent the basic flow parameters which are required<br />

as an input for the acoustic network models used in the present work. In additi<strong>on</strong><br />

Fig. A.1 shows the network structure <str<strong>on</strong>g>of</str<strong>on</strong>g> the combusti<strong>on</strong> c<strong>on</strong>figurati<strong>on</strong><br />

with three <str<strong>on</strong>g>fuel</str<strong>on</strong>g> injecti<strong>on</strong> systems (c<strong>on</strong>figurati<strong>on</strong> B).<br />

187

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