Sentence examples for peak light intensity from inspiring English sources

The peak light intensity at wavelength was 622 nm which corresponds to a red-orange color.

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 intensity was observed at 490 540 nm, with slow reduction from 540 to 700 nm, remaining flat from 700 nm onwards (Fig. 1C).

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.

The minimal length of the tracks lagged behind the peaks in light intensity by ~300 ms. Interestingly, when the light was turned off after the periodical light pulses, the relative length of the bead tracks persisted at the maximal level.

The relative length of the tracks of polystyrene beads decreased sharply within ~300 ms after the dark-light switch, and this period of minimal bead movement persisted for ~2.5 s, even though two peaks in light intensity occurred during this time.

They then performed either a 40 min nonexercise control session of seated rest; or a 30 min cycle bout on an upright ergometer at light (40% VO2 peak, LIGHT) or moderate intensity (60% VO2 peak, MODERATE) with a 5 min warm up and cool down of free wheeling to total 40 min of exercise.

It turned out that, starting from an unpolarized white light source, through a light extraction mechanism based on the diffraction of light, the high quality structure, combined with a uniformly aligned Photo-responsive Liquid Crystal PLCC), is able to give rise to an extremely narrow (FWHM ≈5 nm) and linearly polarized single mode peak of the extracted light intensity.

Peak wavelength verification and light intensity measurements were done with a SPEC-UV/PAR spectroradiometer (Apogee Instruments, Logan, UT).

In white-noise experiments not presented in this work, we used a significantly stronger red light intensity (peak 3 mW/cm) to activate CsChrimson and found that reverse correlation still produces beautiful kernels and nonlinear rate functions, indicating that saturation is not a problem over the majority of the range of these experiments either.

The DH of the sample was obtained from the peak with the highest scattered light intensity (i.e., the mode) in light scattering intensity distributions.