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The peak light intensity at wavelength was 622 nm which corresponds to a red-orange color.
The location of the peak light deflection, and hence of the Schlieren image, depends on whether the flame front curvature is concave or convex toward the hot products.
The peak light intensities of CH∗ and C∗2 emitters are found to be qualitatively correlated with these aforementioned ST data of lean and rich turbulent CH4/diluent/air propagating flames, respectively.
For representative reduced-gravity, spherically propagating cool flames, the flame radius based on the peak light intensity is plotted as a function of time and the flame radius (and speed) is calculated from a polynomial fit to data.
Peak light areas against dark backdrops, meanwhile, could lack a little intensity compared with Samsung's Q9FN 4K models.
The luminescence of hybrid LED is mixed by blue (458.2 and 479.3-nm 479.3-nmnd red (615-nm peaks light.
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These are lower in peak height (lighter in colour) and do not appear in clusters.
Comparing the slopes of the I-V relations indicates that the peak light-evoked conductance is larger during centrifugal stimulation (Figure 2D).
This was evidenced by voltage-clamp recordings of whole-cell ChR2 currents (Figure 5D), which showed that peak light-evoked responses were ∼28 –fold smaller in neurons expressing ChR2-YFP-NavII-III versus those expressing ChR2-YFP (Figure 5E; Xenon lamp stimulation at ∼170 mW/mm2; ChR2-YFP-NavII-III mean ± SEM, 42.1±8.4 pA, n = 8; ChR2-YFP, 1188.5±235.3 pA, n = 8).
To calculate the daily dose (J m−2) of UVBR and UVAR at the 10 fixed positions, spectral irradiance data for peak and non-peak lighting were multiplied by exposure time (4 h for peak lighting and 8 h for non-peak lighting) and added together (Table 1).
To calculate the daily dose (J m−2) of UVRery at the 10 fixed positions, erythemally-weighted spectral irradiance data for peak and non-peak lighting were multiplied by exposure time (4 h for peak lighting and 8 h for non-peak lighting) and added together (Table 1).
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