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Modern Engineering Thermodynamics

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13.16 Brayton Cycle 497<br />

Equation (7.38) also allows us to write<br />

so that<br />

T 3 /T 4s = ðp 4s /p 3 Þ ð1 − kÞ/k = ðv 3 /v 4s Þ 1 − k<br />

ðη T Þ Brayton<br />

= 1 − T 3 /T 4s = 1 − PR ð1 − kÞ/k = 1 − CR 1 − k (13.23)<br />

cold ASC<br />

where PR is the isentropic pressure ratio p 4s /p 3 , and CR is the isentropic compression ratio v 3 /v 4s . Thus, the thermal<br />

efficiency of the Brayton cold ASC can be written as a function of the isentropic pressure or compression<br />

ratio and the specific heat ratio of the working fluid.<br />

EXAMPLE 13.12<br />

The average power cylinder and compression cylinder pressures for the early 1878 Brayton cycle engine shown in Figure 13.45<br />

were p 1 = p 4s = 0.210 MPa and p 2s = p 3 = 0.190 MPa, respectively. For this engine, determine<br />

a. The isentropic pressure ratio PR.<br />

b. The isentropic compression ratio CR.<br />

c. The Brayton cold ASC thermal efficiency.<br />

Solution<br />

Using the Brayton cycle diagram shown in Figure 13.44, we can carry out<br />

the following analysis.<br />

a. The isentropic pressure ratio of a Brayton cycle engine is given by<br />

PR = p 4s<br />

p 3<br />

=<br />

0:210 MPa<br />

0:190 MPa = 1:11<br />

b. The isentropic compression ratio of a Brayton cycle engine is given by<br />

CR ¼ðPRÞ 1/k = ð1:11Þ 1/1:40 = 1:07<br />

c. Equation (13.23) gives the Brayton cold ASC thermal efficiency as<br />

ðη T Þ Brayton<br />

= 1− T 3<br />

= 1−PR ð1−kÞ/k = 1−ð1:11Þ ð1−1:40Þ/1:40 = 0:0294 = 2:94%<br />

T 4s<br />

cold ASC<br />

Exercises<br />

34. Determine the isentropic pressure ratio for the Brayton cycle engine in<br />

Example 13.12 if the power piston pressure is increased from 0.210 MPa<br />

to 0.300 MPa. Assume all the other variables remain unchanged.<br />

Answer: PR= 1.58.<br />

FIGURE 13.45<br />

Example 13.12.<br />

35. If the compression pressure of the Brayton cycle engine in Example 13.12 is lowered from 0.190 MPa to 0.100 MPa,<br />

determine the corresponding isentropic compression ratio of the engine. Assume all the other variables remain<br />

unchanged. Answer: CR= 1.70.<br />

36. If operating conditions of the Brayton cycle engine in Example 13.12 are altered such that the isentropic temperature at<br />

the exit of the compressor is T 4s = 35.0°C when the inlet air temperature is 22.0°C, determine the Brayton cycle cold<br />

ASC thermal efficiency of this engine under these operating conditions. Answer: (η T ) Brayton cold ASC = 4.22%.<br />

Since T 3 = T L but T 4s < T 1 = T H , the Brayton cold ASC thermal efficiency is less than that of the Carnot cold ASC<br />

working between the same temperature limits (T 1 and T 3 ). However, for fixed values of the temperature limits<br />

T 1 and T 3 , there is an optimum value for the compressor outlet temperature T 4s that maximizes the net output<br />

work. This can be determined as follows for an isentropic turbine and compressor:<br />

ð _W out Þ net<br />

isentropic<br />

= _W pm − j _W c j = _mc p ðT 1 − T 2s − T 4s + T 3 Þ<br />

Now, holding T 1 and T 3 fixed and replacing T 2 with its isentropic equivalent, T 2s = T 1 T 3 /T 4s , we get<br />

ð _W out Þ net<br />

isentropic<br />

= _mc p ðT 1 − T 1 T 3 /T 4s − T 4s + T 3 Þ

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