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Modern Engineering Thermodynamics

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14.9 Cascade and Multistage Vapor-Compression Systems 555<br />

HOW DO YOU LIQUEFY A GAS LIKE OXYGEN?<br />

Though French engineer Charles Tellier (1828–1913) first suggested the concept of cascade refrigeration in 1867, the Swiss<br />

scientist Raoul Pictet (1846–1929) first developed a dual-cascade refrigeration system and used it to produce liquid oxygen<br />

in 1877. He used SO 2 in the high-temperature cycle and CO 2 in the low-temperature cycle. He was able to produce only a<br />

liquid oxygen mist, but it was the beginning of cryogenic refrigeration. Hydrogen gas was first liquefied in 1898 and<br />

helium gas was finally liquefied in 1908.<br />

system using the same refrigerant in each cycle. However, adifferentrefrigerantisoftenusedineachcycleto<br />

optimize overall system performance. When different refrigerants are used in the cascaded cycles, separate (or<br />

combined) T–s diagrams must be used in the analysis. Some industrial systems require three or four cascaded<br />

cycles to reach the desired low temperature.<br />

The cascaded cycles are interconnected through insulated closed loop heat exchangers that function as evaporators<br />

in the higher temperature cycle (A) and as condensers in the lower temperature cycle (B). An energy balance on an<br />

interconnecting heat exchanger provides a relation between the mass flow rates of refrigerant in the two cycles as<br />

Where h 2b is determined from<br />

_m A<br />

_m B<br />

= h 2B − h 3B<br />

h 1A − h 4hA<br />

(14.9)<br />

And the coefficient of performance for the entire cascaded system is<br />

COP cascade =<br />

For a dual-cascade system, Eq. (14.11) becomes<br />

COP dual<br />

=<br />

cascade<br />

_Q L<br />

_W c−A + _W c−B<br />

=<br />

h 2B = ðh 2sB − h 1B Þ/ðη s Þ c−B + h 1B (14.10)<br />

_Q L<br />

_W c−A + _W c−B + … =<br />

_Q L<br />

∑ _W compressors<br />

(14.11)<br />

_m B ðh 1B − h 4hB Þ<br />

_m A ðh 2sA − h 1A Þ/ðη s Þ c−A + _m B ðh 2sB − h 1B Þ/ðη s Þ c−B<br />

(14.12)<br />

The following example illustrates that cascading can be used to decrease the individual compressor pressure<br />

ratios and increase the coefficient of performance of a system. However, understand that this increase in system<br />

COP also requires an increased capital investment and increased maintenance costs.<br />

EXAMPLE 14.6<br />

A food-processing refrigeration unit is required to produce 40.0 tons of refrigeration at an evaporator temperature of −50.0°C<br />

and a condenser temperature of 25.0°C. Since this temperature difference is quite large, it was decided to design a dual-cascade<br />

unit using. R-22 in both of the cascaded loops. The intermediate heat exchanger connecting the two loops is to operate<br />

at −20.0°C, and the isentropic efficiencies of both compressors is 80.0%. The following design specifications were then<br />

established for the refrigeration loops shown in Figure 14.17:<br />

Loop A<br />

Loop B<br />

Station 1A Station 2sA Station 3A Station 4hA<br />

Compressor A inlet Compressor A outlet Condenser A outlet Expansion valve A outlet<br />

x 1A = 1:00 p 2sA = 1500: kPa x 3A = 0:00 h 4hA = h 3A<br />

T 1A = −20:0°C s 2sA = s 1A T 3A = 25:0°C<br />

Station 1B Station 2sB Station 3B Station 4hB<br />

Compressor B inlet Compressor B outlet Condenser B outlet Expansion valve B outlet<br />

x 1B = 1:00 p 2sB = 300: kPa x 3B = 0:00 h 4hB = h 3B<br />

T 1B = −50:0°C s 2sA = s 1B T 3B = −25:0°C<br />

(Continued )

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