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According to the main results of experiment, the strength of RAC was higher than the other two factors in the effect of mechanical performance and ultimate bonding stress.
Such a significant difference (from 1.46 to 1.56 times) between the experimental and ab initio values of strength is due to the fact that in the experiment, the strength of contact bond between the chain and the graphene sheet is measured, and ab initio calculations gives the strength of atomic bonds in the chain itself.
In one experiment, the strength of blink reflexes to unexpected noises was measured and correlated with degrees of reactions to external threats.
In a real experiment, the strength of selection might also not be known and often cannot be changed for the trait of interest.
In each experiment the strength of the gradient pulse was incremented, while δ (2 5 ms) and Δ (60 ms) remained constant.
After experiment the strength of quadriceps on the operated side in group A (NMES) increased from 645.9 to 893.4 N (28.7%, P = 0.001) and in group B (control) it increased from 648.6 to only 669.8 N (4.6%, P = 0.04).
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Through the numerical experiments the strength of the solver in effectively/accurately simulating various complex flows past different forms of immersed boundaries is extensively demonstrated, in which the nested Cartesian grid method was suitably combined together with the fractional-step algorithm to speed up the solution procedure.
In all experiments, the strength of the prior λ was set to λ = 10.
Fig. 11 Results of a sensitivity experiment of the strength of numerical diffusion.
We next investigated the effects of the length of the experiment and the strength of selection on the power to detect QTL.
Figure 4A shows the results from a representative experiment testing the strength of attachment of HEK-293 cells to dishes coated with various doses of PEI.
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