1926
DOI: 10.1088/0959-5309/39/1/316
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The present state of atomic physics

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Cited by 14 publications
(29 citation statements)
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“…It is convinced that this theoretical relation corresponds to the empirical one, K=02 L4/3 cm2.sec-1, which was found for the wide range of horizontal diffusion phenomena in the atmosphere by Richardson (1926) (9). Thus, to some extent, we might be able to consider safely that the atmosphere has such the structure as assumed above.…”
supporting
confidence: 66%
“…It is convinced that this theoretical relation corresponds to the empirical one, K=02 L4/3 cm2.sec-1, which was found for the wide range of horizontal diffusion phenomena in the atmosphere by Richardson (1926) (9). Thus, to some extent, we might be able to consider safely that the atmosphere has such the structure as assumed above.…”
supporting
confidence: 66%
“…∼t 1/2 . For intermediate time scales the dispersion follows the Richardson law, ∼t 3/2 (Richardson 1926). Figure 12 shows the evolution between z = 30 and z = 0.5 of the pair dispersion statistics derived with N = 10 6 couples of tracers in the same cluster run.…”
Section: Tracers Dispersion Statisticsmentioning
confidence: 99%
“…where X 1 (t) is the position of the first particle and X 2 (t) the position of the second particle at time t. The first quantity of interest is the mean-square separation between the two particles ∆ 2 (t) as a function of time which has received much research attention since the pioneering work of [1] (see for example [2][3][4][5][6][7][8][9][10][11][12][13][14]). …”
mentioning
confidence: 99%