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As a result, our simulation results suggest the following: for Rician channels with high κ factor, fully interleaved performance is approximately achieved when the interleaver depth N 1≥0.1N coh; while for Rician channels with low κ factor, in particular for a Rayleigh fading channel, fully interleaved performance is approximately achieved when N 1≥0.7N coh.
In [3], simulations were used to demonstrate that fully interleaved performance is approximately achieved for BPSK over exponentially correlated channels when the interleaver depth is chosen to satisfy f D T s N 1>0.1.
The magnitude response requirement is approximately achieved by a constrained optimization procedure, where the objective function and constraints are all expressed in terms of the auxiliary filters of scaling filters rather than the scaling filters directly.
This result is consistent with our conclusion in Subsection 4.1, which illustrates that the maximum gain from the interleaver is approximately achieved when N 1≥0.7N coh in a Rayleigh fading channel.
As mentioned in Subsection 2.3, simulation results in [3] demonstrated that fully interleaved performance is approximately achieved for BPSK over exponentially correlated channels when N 1≥0.1N coh is satisfied, and [4] further extended this result to Rician channels and a variety of channel auto-correlation functions by proposing a simple figure of merit for evaluating interleaver depth.
At this point, the highest biomass productivity is approximately achieved.
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If the disturbance and the reference signal are slowly varying with respect to the sampling frequency, the proposed sliding mode controller can reject the disturbance and output tracking can be approximately achieved.
In the case of non-zero conservative force, the condition of constant density and divergence-free of velocity can be approximately achieved at large values of the repulsion parameter (i.e., weakly compressible flow).
Dynamic equilibrium over the entire specimen needs to be approximately achieved to relate the crack tip loading state to the far-field loading conditions, and the loading rate at the crack tip should be maintained near constant during an experiment to delineate rate effects on the values of dynamic crack initiation toughness.
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