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

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2. Gas Turbine Combustor<br />

ratio can be optimized to maximize the efficiency for a specific <strong>combustor</strong><br />

temperature [12]. Besides optimization <strong>of</strong> the efficiency, the <strong>gas</strong> <strong>turbine</strong><br />

should be optimized for the power output (Figure 2.3). The optimization<br />

sets the conditions for the <strong>combustor</strong>. For the <strong>gas</strong> <strong>turbine</strong> cycle in Figure<br />

2.3 at a <strong>combustor</strong> outlet temperature (COT) at 1743 K, the optimal<br />

pressure ratio for specific power is 14.3 bar and the optimal pressure ratio<br />

for efficiency is 25.1 bar. These values are engine-specific but show the<br />

tendency for optimization.<br />

Today, single-cycle efficiency above 40 % for smaller engines are common<br />

and, for heavy frame engines, efficiencies above 60 % are available<br />

[1]. Modern <strong>gas</strong> <strong>turbine</strong>s have a COT <strong>of</strong> 1800 K for the heavy frame engine<br />

(up to ∼300 MW), and 1700 K for the midrange engines (∼100 MW)<br />

[1]. The COT temperature is being pushed towards 1900 K [13]; this will<br />

be a challenge for DLE <strong>combustor</strong>s as the thermal NO X will increase significantly<br />

above around 1850 K [14]. Consequently, maintaining low NO X<br />

emission while having high efficiency is contradictory.<br />

In order to minimize NO X emissions, the combustion temperatures<br />

are being pushed towards lower temperatures. This means that achieving<br />

ultra-low NO X emissions will have a negative influence on cycle efficiency.<br />

In this thesis, the experimental work is largely limited to atmospheric<br />

condition and maximum temperatures around 1750 K.<br />

2.1 The <strong>combustor</strong><br />

2.1.1 General <strong>combustor</strong>s<br />

The purpose <strong>of</strong> a <strong>combustor</strong> is to transform chemically bound energy<br />

to heat, in order to increase the temperature before the <strong>turbine</strong>. The<br />

arrangement for a <strong>combustor</strong> section varies for different <strong>gas</strong> <strong>turbine</strong>s. For<br />

example, many <strong>combustor</strong>s may be placed in an annular arrangement<br />

surrounding the <strong>gas</strong> <strong>turbine</strong>, or just a single larger <strong>combustor</strong> on the<br />

side <strong>of</strong> the <strong>gas</strong> <strong>turbine</strong> [12,14]. The annular arrangement could consist <strong>of</strong><br />

separate cans or could be placed in an open chamber. The combustion<br />

zone (Figure 2.4) is similar for all the <strong>combustor</strong>s mentioned previously.<br />

First, there is a primary zone where combustion is initiated. Here the<br />

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