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Modern Engineering Thermodynamics

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14.14 Reversed Brayton Cycle Refrigeration 569<br />

14.14 REVERSED BRAYTON CYCLE REFRIGERATION<br />

In 1844, the American physician John Gorrie (1803–1855) designed and built an air cooling apparatus in Florida<br />

to provide air conditioning for his yellow fever patients. His machine had a piston-cylinder apparatus that<br />

compressed air that was cooled back to ambient temperature by circulating water. The cooled compressed air<br />

was then expanded in a second piston-cylinder apparatus that caused the air to drop to a sufficiently low temperature<br />

to produce ice and satisfy other cooling needs. The expanded air was then drawn back into the compressor<br />

and the cycle began again. The two piston-cylinder devices were connected together so that the<br />

expansion work was used to offset the compression work. This was clearly a reversed, closed loop Brayton cycle,<br />

as shown by comparing Figures 13.44 and 14.27.<br />

The COP of an actual reversed Brayton cycle is given by<br />

and<br />

COP reversed<br />

= j _Q H j<br />

=<br />

j _W<br />

Brayton cycle in j net<br />

HP<br />

COP reversed<br />

= j _Q L j<br />

=<br />

j _W<br />

Brayton cycle in j net<br />

R=AC<br />

ðT 2s − T 1<br />

ðT 2s − T 1<br />

T 2 − T 3<br />

(14.22)<br />

Þ/ ðη s Þ c<br />

− ðT 3 − T 4s Þðη s Þ c<br />

T 1 − T 4<br />

(14.23)<br />

Þ/ ðη s Þ c<br />

− ðT 3 − T 4s Þðη s Þ c<br />

where T 2 = T 1 + ðT 2s − T 1 Þ/ ðη s Þ c and T 4 = T 3 − ðT 3 − T 4 Þðη s Þ e : Since the processes 1 to 2s and 3 to 4s are isentropic<br />

and the processes 2s to 3 and 4s to 1 are isobaric,<br />

T 2s = T 1 ðp 2s /p 1<br />

Þ ðk−1<br />

Þ/k = T 1 PR ðk−1<br />

Þ/k<br />

Cooling water<br />

Q H<br />

Q H<br />

3<br />

Expander<br />

Hot air<br />

2<br />

Compressor<br />

3<br />

Hot air<br />

2<br />

W E<br />

W C<br />

Turbine<br />

Compressor<br />

W net<br />

4<br />

Cold air<br />

1<br />

4<br />

Cold air<br />

1<br />

Q L<br />

(a) John Gorrie’s 1844 equipment schematic<br />

Q L<br />

(b) A modern reversed Brayton cycle equipment<br />

schematic<br />

T<br />

W E<br />

Q H 2s<br />

p = c<br />

3<br />

W C<br />

1<br />

p = c<br />

4s Q L<br />

FIGURE 14.27<br />

The reversed Brayton cycle cooling system using air as a working fluid.<br />

s<br />

(c) Reversed Brayton ASC T–s diagram

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