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Stress distribution across the depth becomes nonlinear when d/l = 0.25 and d/l = 0.5.
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In [12], the approach to robust beamforming, with null widening, imparts robustness into adaptive pattern by judicious choice of null placement and width through introducing the concept of a covariance matrix taper (CMT), while the performance degradation of the method is evident because the relative high sidelobe and the depth become somewhat shallower when the null width is broadened.
The nsplit and the depth become the hyperparameters of the model.
The length of this depth becomes more and more pronounced as the electromagnetic frequency approaches the so-called plasma frequency, which varies according to the material properties.
The results show that, the larger the optimum diameter, the larger the corresponding optimum depth becomes; the optimum area ratio is not bound up with the texture parameters and operating parameters; the optimum depth increased while the optimum diameter decreased as the velocity became larger and the load became smaller.
As the temperature approaches the critical temperature, the penetration depth becomes extremely large.
When the flame is propagated downward, the spacing between cells is almost constant and the cell depth becomes smaller as the acceleration increases.
First, as the tree depth becomes shallower the implied rate of speciation increases because all trees contain 50 species.
When the screen effect is taken into account, the trap depth becomes even smaller than the stimulated values (Fig. 1b) in vacuum, because the screen effect remarkably reduces the effective surface charge density at the trap electrodes.
We can recognize that δt tends to be large as the focal depth becomes deep, although the scatter is large.
The water depth becomes very thin at the wave front.
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