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Assessment and Future Directions of Nonlinear Model Predictive ...

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A Minimum-Time Optimal Recharging Controller 4452.1 Equation <strong>of</strong> StateThe following two-coefficient virial equation <strong>of</strong> state for a binary mixture [1]Z =PRT ρ =1+B mixρ + C mix ρ 2 (1)B mix = b 1 (T )x 2 1 +2b 12 (T )x 1 x 2 + b 2 (T )x 2 2 (2)C mix = c 1 (T )x 3 1 +3c 112(T )x 2 1 x 2 +3c 122 (T )x 1 x 2 2 + c 2(T )x 3 2 (3)is used in this work where x 1 ,x 2 are the component mole fractions <strong>and</strong> B mix <strong>and</strong>C mix are, in general, functions <strong>of</strong> temperature. Because the composition <strong>of</strong> theinlet gas mixture is maintained at the desired target composition, x 1 <strong>and</strong> x 2 areconstant at this composition in stages C <strong>and</strong> D. The equation <strong>of</strong> state for thesingle component streams in stages A 1 <strong>and</strong> B 1 is obtained by setting x 1 =1<strong>and</strong>x 2 = 0 in Eqs. 2 <strong>and</strong> 3. The equation <strong>of</strong> state for stages A 2 <strong>and</strong> B 2 is h<strong>and</strong>ledin a similar manner by setting x 1 =0<strong>and</strong>x 2 =1.PressureP (initial)initial stageP (final)P (ideal gas)HRi∆HIGfinal stageH RfT (initial)TemperatureT (final)Fig. 2. Isoenthalpic stage transition model2.2 Isoenthalpic TransitionThe first two transitions are described by the path shown in Figure 2 for boththe individual pure components <strong>and</strong> the gas mixture. The resulting equation forthe transition from an initial stage i to the next stage f becomes∆H i→f =0=−H R i + ∆H IG + H R f (4)where HiR is the residual enthalpy between the gas at the initial stage <strong>and</strong> thegas at ideal conditions at the initial temperature, ∆H IG is the change in enthalpy<strong>of</strong> the gas at ideal conditions between the final <strong>and</strong> initial temperatures, <strong>and</strong> HfRis the residual enthalpy between the gas at the next stage <strong>and</strong> the gas at idealconditions at the final temperature. The residual enthalpy is

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