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It is also concluded that when the boundary control points of interfacial surface are free to move, maximum system heat flux can be obtained by the present algorithm since it has more degree of freedom in describing the interfacial surface.
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Finally, the results show that for the two different cases considered in this work, the maximum increasing in the system heat flux is obtained as 11.3% and 14.1%, respectively.
The maximum system efficiency based on lower heating value (LHV) is 37% at 120.7 W.
Results reveal that the maximum system efficiency was as high as 81% when combining heat and power.
In this phase cycle efficiency and heat source recovery factor lead to opposite design choices in the achievement of maximum system efficiency and, in turn, maximum power output.
More specifically, the maximum system COP is found to be 0.234 when the system produces refrigeration at 10 °C and rejects heat to the environment at 30 °C.
Maximum heat recovery heat exchanger effectiveness was about 93% with overall system efficiency of 54%.
By integrating system heating, a maximum energy recovery network (MER) and also a relaxed network were developed.
Currently, the system heats a laboratory space.
The irreversible transformation to higher conductivities is also observed in systems heated to maximum temperatures between 50 and 80 °C for which degradation was shown to be negligible.
A combined heat and power (CHP) system using the maximum waste heat recovery and Rankine cycle is illustrated to assess performance in terms of power generation and CO2 utilization.
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