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The experimental and simulated efficiency values agreed well.
The simulated efficiency of the single stage depressed collector is 63%.
Timing precision calculations were then used to determine the timing response for each configuration based on its simulated efficiency.
The expression for theoretical efficiency, ηT is also applicable to experimental efficiency (ηP), empirical efficiency (ηE), and simulated efficiency for oceanic wave (ηc).
In the graphical analysis in Fig. 5, the simulated efficiency (ηc) of the machine is greatly hampered by the oceanic waves.
Using the simulated efficiency of the array, cross sections for radiative capture can be calculated from the measured γ ray yields, for the individual reactions.
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However, the simulated efficiencies are ranging between 8 and 15, while experimental instantaneous efficiencies were within the range of 3.5 15.5%%. .
An informed decision based on the simulated efficiencies and timing precision calculations allowed the optimum configuration for the array to be determined.
A short-cut equation based on statistical fit of all simulated efficiencies as a function of Reynolds numbers and inertial impaction parameter is also presented to compute the inertial collection efficiency of an isolated cylindrical collector.
This is confirmed from simulation results obtained by Qu et al [ 3] comparing the simulated relative efficiency (SRE) of parameter estimators from GEE and QIF: SRE = mean squared error of GEE estimator mean squared error of QIF estimator.
Under these conditions the simulated power efficiency is more than 80%.
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