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investigation of a prototype industrial gas turbine combustor using ...

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2. Gas Turbine Combustor<br />

Figure 2.1: The SIT <strong>gas</strong> <strong>turbine</strong>, SGT-750, in which the full-scale version<br />

<strong>of</strong> the <strong>combustor</strong> investigated in this thesis operates. (Courtesy <strong>of</strong><br />

Siemens Industrial Turbomachinery [SIT].)<br />

(Figure 2.2).<br />

In the ideal Brayton cycle diagram, Figure 2.2, it can be seen that<br />

the temperature is increased from position 1 to position 2 because <strong>of</strong> the<br />

isentropic compression <strong>of</strong> the <strong>gas</strong> by the ideal compressor. Heat is then<br />

added via combustion at constant pressure, thereby further increasing<br />

the temperature. The expander then reduces the pressure from P 2 to P 1<br />

and the temperature drops. The area inside the cycle in the T-S diagram<br />

equals the work output <strong>of</strong> the cycle. The efficiency <strong>of</strong> the cycle equals<br />

the work done divided by the heat input (2.1).<br />

η GT = W out<br />

Q in<br />

, (2.1)<br />

Maximizing work output can be achieved by maximizing the area <strong>of</strong> the<br />

Brayton cycle (Figure 2.2). This can be done by maximizing the difference<br />

8

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