2010
DOI: 10.1088/1742-5468/2010/11/p11030
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Universality of rain event size distributions

Abstract: Abstract. We compare rain event size distributions derived from measurements in climatically different regions, which we find to be well approximated by power laws of similar exponents over broad ranges. Differences can be seen in the large-scale cutoffs of the distributions. Event duration distributions suggest that the scale-free aspects are related to the absence of characteristic scales in the meteorological mesoscale.

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Cited by 79 publications
(151 citation statements)
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“…Indeed, while all of the explicit convection runs have probability densities similar to a power-law distribution across most of their range before decreasing exponentially at very high rain rates (similar to recent observational studies; DeMott et al, 2007;Field and Shutts, 2009;Peters et al, 2010), the 12 km param model with parametrized convection has a positive deviation from this type of power-law distribution, suggesting a 'preferred' scale of rainfall centred around 0.4 mm h −1 (10 mm day −1 ). Rainfall rates around this value contribute more to the total rainfall in this model than higher or lower rates, unlike observations and explicit convection runs.…”
Section: Discussionsupporting
confidence: 77%
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“…Indeed, while all of the explicit convection runs have probability densities similar to a power-law distribution across most of their range before decreasing exponentially at very high rain rates (similar to recent observational studies; DeMott et al, 2007;Field and Shutts, 2009;Peters et al, 2010), the 12 km param model with parametrized convection has a positive deviation from this type of power-law distribution, suggesting a 'preferred' scale of rainfall centred around 0.4 mm h −1 (10 mm day −1 ). Rainfall rates around this value contribute more to the total rainfall in this model than higher or lower rates, unlike observations and explicit convection runs.…”
Section: Discussionsupporting
confidence: 77%
“…These numbers are consistent with the discussion above regarding model differences, with more occurrences of rainfall at a fairly low average rain rate (near the apparent preferred scale) for the 12 km param model and fewer occurrences with higher average rain rates for the observations and the explicit convection models (with especially infrequent, heavy rain for the 4 km 3Dsmag and 12 km 3Dsmag models). The rough power-law relationship of −1 for lower values of precipitation for both the 4 km runs and TRMM (Figure 2(a)) compares well with rain-rate distributions from several tropical observation sites (Peters et al, 2010, their figure 1). This value of the power law implies an equal contribution at all scales, which is evident in Figure 2(b).…”
Section: Precipitation Distributionssupporting
confidence: 62%
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“…For Case 1, one has a simple Fokker-Planck equation (30) with τ = 3/2 and sL = 2D for Case 1, for s above a small-event cutoff (Eq. S3) that is too small to see in gauge observations (18,19) or in the climate model. Features of this solution are seen in the top pair of curves of Fig.…”
Section: Significancementioning
confidence: 95%
“…Here, we derive a stochastic prototype from a fundamental climate model equation. This leads to an explanation of key properties of the probability density function (pdf) of accumulations noted in station observations (18)(19)(20)-why the pdf of accumulation size drops slowly with increasing size over many orders of magnitude before reaching a cutoff scale, after which the pdf drops rapidly for very large accumulations. From the theory, we show that physical balances creating this behavior regime imply extremely high sensitivity for the very largest events under climate change.…”
mentioning
confidence: 98%