AIR STANDARD BRAYTON CYCLE
Gas turbines function based on Brayton cycles. Figures 30.4 (a), (b) and (c) explain working of a Brayton cycle.
Figure 30.4 (a) (b) and (c) |
The air-standard Brayton cycle consists of
1-2 Isentropic compression of air
2-3 Constant pressure energy addition
3-4 Isentropic expansion
4-1 Constant pressure energy rejection
![](images/image039.gif)
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(30.10) |
![](images/image041.gif)
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(30.11) |
![](images/image043.gif)
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(30.12) |
![](images/image045.gif)
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(30.13) |
is the pressure ratio
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(30.14) |
![](images/image049.gif) |
(30.15) |
and
or ![](images/image053.gif) |
(30.16) |
or,
![](images/image055.gif) |
(30.17) |
so,
![](images/image057.gif) |
(30.17) |
or
![](images/image059.gif) |
(30.18) |
The variation of as a function of is shown in Figure 30.5
|
(30.19) |
|
(30.20) |
But
& ![](images/image075.gif) |
|
or
![](images/image079.gif) |
(30.21) |
The optimum pressure ratio is obtained by differentiating W wrt rp holding T1 and T3 constant, and setting the expression equal to zero. This gives
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