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Finally, three optimum schemes were recommended for practical application according to their outdoor cooling effect and impact on driving glare.
First, the optimum schemes with noncausal CSI (offline schemes) provide a benchmark for all the other schemes that guarantee the required delay.
We outline some key points: (i) the great difficulty to obtain accurate numerical results for large values of α (ii) the possibility of virtually optimum schemes is essentially theoretical and requires, in practice, careful experiments; (iii) for strongly convective problems, some second-order explicit schemes are almost as efficient (and less costly) than implicit fourth-order schemes.
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Nevertheless, the CAF scheme has losses of 10% compared to the centralized global optimum scheme.
In an AWGN environment, MRT can be seen as an optimum scheme.
Some properties are proved and used to determine the optimum scheme which maximizes utilization.
Then, power consumed in driving reciprocator is considered to derive a multi-objective optimum scheme.
The results show that the proposed optimum scheme outperforms MSE-MSE and ZF-ZF schemes by a good margin.
It can be easily observed that the proposed optimum scheme outperforms both MMSE-MMSE and ZF-ZF methods.
In these cases too, the simulation results reveal that the optimum scheme outperforms the other two methods.
Particle size of 1 2 mm was selected as the optimum scheme considering the adsorption kinetic parameters and technical specifications.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com