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Space Grant Consortium - University of Wisconsin - Green Bay

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load total load<br />

( nd ) ( 1 nd 8 nd )<br />

Q� v� = Q� m� v� m� + v� m�<br />

(25)<br />

2 2 2<br />

Optimization Algorithm. The optimization process for the results presented in this paper<br />

identify the optimal mixture composition in the 2 nd stage ( y nd , the vector <strong>of</strong> compositions <strong>of</strong><br />

2<br />

each mixture component) for a particular set <strong>of</strong> operating conditions. The total heat exchanger<br />

compactness figure <strong>of</strong> merit ( QUA �<br />

total ) calculated by the thermodynamic model varies<br />

significantly as the mixture mole fraction vector ( y nd ) changes, so it is necessary to evaluate a<br />

2<br />

wide range <strong>of</strong> mole fraction combinations. It is not computationally efficient to parametrically<br />

evaluate the mole fractions for all possible y nd combinations. Therefore, an optimization<br />

2<br />

algorithm that is able to select the optimal mixture using significantly less computations than a<br />

parametric study is utilized here.<br />

The optimization routine selected is the PIKAIA 1.2 [9] genetic algorithm that finds the<br />

maximum <strong>of</strong> the objective function using an algorithm that mimics biological evolution. A<br />

detailed description and demonstration <strong>of</strong> the routine as it is used to select a best mixture is<br />

found in [0]. As shown by [0], other optimization techniques such as the direct search and<br />

variable metric strategies do not reliably converge because <strong>of</strong> the sharp discontinuities in mixture<br />

properties near phase boundaries as well as other constraints that are placed on the mixture.<br />

Note that the reliability <strong>of</strong> the genetic optimization routine comes at the expense <strong>of</strong> computation<br />

speed; the genetic algorithm should only be used when other, faster, routines have failed.<br />

The optimization routine excludes mixtures based on two practical considerations: 1) A mixture<br />

is excluded from further consideration if the temperature at the exit <strong>of</strong> the 2 nd stage expansion<br />

valve is below the freezing point temperature. 2) Mixtures in a saturated or liquid state leaving<br />

the recuperator (state 1) are excluded to avoid the introduction <strong>of</strong> liquid into the 2 nd stage<br />

compressor. The freezing point is calculated as the weighted average <strong>of</strong> the triple point <strong>of</strong> the<br />

mixture constituents, as described in [0]<br />

Optimization Results<br />

The results <strong>of</strong> the optimization model using a pure refrigerant in the 1 st stage and a hydrocarbon<br />

based mixture in the 2 nd stage are presented in this section. The refrigerant used for analysis in<br />

the 1 st stage is R22. The Q� load UAtotal<br />

figure <strong>of</strong> merit is optimized in order to yield the MGJT<br />

system that provides the most cooling for a given geometric size for load temperatures spanning<br />

100 K to 180 K. The effect <strong>of</strong> the precooling temperature (T4) on Q� load UAtotal<br />

is studied in<br />

order to show the optimal balance between the precooler and the recuperator. The other figure <strong>of</strong><br />

merit, the load specific compressor volumetric flow rate is not explicitly optimized but is<br />

reported as it is important in the design <strong>of</strong> a practical system. The performance <strong>of</strong> the two stage<br />

system is normalized against the performance <strong>of</strong> a single stage system in order to show the<br />

relative benefit and penalty associated with the addition <strong>of</strong> precooling.<br />

The Q� load UAtotal<br />

for a two stage system in which an optimal mixture has been selected for each<br />

precooling and load temperature is shown in FIGURE 3(a). As the precooling temperature is<br />

35

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