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Higher irradiation power and frequencies result in more severe graphitization due to higher temperature and accumulative heating respectively.
Due to the randomness of the formation of closed loop paths, their respective resonance frequencies result in discrete sharp random peaks in the emission spectrum.
The low pulse frequency such as 10 Hz yields a wavy mixing interface, but the high pulse frequencies result in a set of mixing clouds in the mixing channel.
Light from 50/60 Hz fluorescent lamps produces a photocurrent with a total bandwidth of 20 kHz [122], while higher modulation frequencies result in photocurrents that have a considerable part of their power spectrum in the MHz range [121].
The 2.3 and 1.63 ppm signals may be assigned to protons bound to C2 and C3 carbons in acyl chains, whose NMR frequencies result from progressively longer distance from the deshielding carboxyl group (C1).
The IR intensity weighted-averages of the two sets of frequencies result in calculated values 1338 and 1503 cm-1 that are as close as can be expected to the observed frequencies for modeling aqueous phase complexes at this level of theory [90].
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Modelled event durations and eruption frequencies resulted in similar total erupted masses in each event bin.
Many visually impaired individuals experience a loss of visual perception to high spatial frequencies resulting in blurred vision [2].
However, when using omnidirectional microphones, the signals are highly correlated at low frequencies, resulting in a high estimation variance.
Such a choice is due to low attenuation at these frequencies, resulting in higher precision of input data.
According to classical physics the intensity of this continuous radiation would grow unlimitedly with growing frequencies, resulting in what was called the ultraviolet catastrophe.
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