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The rate of an enzymatic reaction increases with increased substrate concentration, reaching maximum velocity when all active sites of the enzyme molecules are engaged.
The droplet was uniformly accelerated by constantly applied positive pressure, and the droplet had maximum velocity when passed through final point of experimentally observed region.
In blast events, auxetic composite panels are found to effectively absorb double the amount of impulsive energy via plastic deformation, and reduce up to 70% of the back facet's maximum velocity when compared with monolithic ones.
We observe a similar maximum velocity when laterally translating identical beads without attachment to a nanomembrane, suggesting that the hydrodynamic drag resulting from the unique shape of the nanomembranes is minimal.
Experimental results show that flame reaches the maximum velocity when mixtures are near the stoichiometric concentration without obstacles while deflagration to detonation transition (DDT) may occur when obstacles are arranged in the duct.
It is found from this figure that for each selected value of ϕ, there is a critical value of η c corresponding to the maximum velocity, when η < η c, the velocity profile f ′ increases dramatically as η enlarges, while, when η ≥ η c, f ′ decreases gradually as η evolves.
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From Figs. 8, 9, we see that there is a value of the gait parameter (delta) which gives the maximum forward velocity when the gait parameters (alpha) and (omega) are kept constant.
From Figs. 13e, f and 14e, f, it is clear that there exists a value of the gait parameter (delta) which gives the maximum forward velocity, when the gait parameters (alpha) and (omega) are kept constant, which is in accordance with the simulation results presented in previous section.
The maximum detectable velocity, when multiple aliasing rings are visible, is affected by a combination of factors including SNR, spatial resolution, and the performance of the phase unwrapping techniques.
Applied to directional solidification experiments carried out with aluminium silicon alloys, the model shows that this maximum velocity was reached when the top position of the mushy zone (i.e. the dendritic interface) reached about two-thirds the length of the ingots.
Thus, the damping coefficient in LED is varied according to the average variation of maximum relative velocities when structures are unconnected and the corresponding calculations to arrive at the variation of damping of LEDs are shown in Table 2.
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