Sentence examples for max as shown from inspiring English sources
Δ2θ R sum starts to deviate at approximately 2θ max as shown by the arrow with increasing 2θ. Figure 3b shows the 2θ max-dependence of R wp's.
Although Δ2θ R sum is closer to Δ2θ m than Δ2θ R cnv, it deviates from Δ2θ m above 2θ max as shown in the inset of Fig. 3e as an example.
The difference in match scores was normalized by the maximum score possible for a given PWM matrix (ψ max), as shown in the following equation.
It is revealed that a certain d can be calculated for a given s, r and v max, as shown in Eq.7.
It can be seen from (20) to (22) that the cyclic variation between T min and T max (as shown in Fig. 1) of the building's indoor temperature can be realized when the chiller units operate with the constant cooling capacity q ch for τ on and stop working for τ off in τ c.
This is attributed to a more rapid increase in strength development for ESC with higher compressive strength at the same T max as shown in Figs. 3 and 6. Figure 7b shows the effects of limiting the maximum value of T (T max) on the E idx value.
This conclusion was supported by comparisons between the variances of the larger optic flow sums obtained at 90° and at 45° (Max(Σω90°) and Max(Σω45°)): as shown by the histograms to the right of Figure 4B,D, the variance-to-the-mean ratio was distinctly lower at 45° than at 90° ( t(36) = 2.99, p<0.01 ).
If a unit missed its deadline, the delay is calculated as deadline minus request time (max. delay) as shown in equation 4. δ max = t deadline - t req (4).
The difference, R wp all − R wp cnv, becomes smaller with decreasing 2θ max and is 0.02% or less below 2θ max = 120° as shown in Fig. 3c.
Furthermore, the top amplitude of the modulation strength is 1 + f(C MAX ) * M, and the bottom is 1 − f(C MAX ) * M as shown in Fig. 5.
The dependences of fNL on V S30 and A max were investigated, as shown in Fig. 10c, d, respectively.
