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A stochastic model for the analysis of the temporal change of dry spells

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Abstract

In the present paper a stochastic approach which considers the arrival of rainfall events as a Poisson process is proposed to analyse the sequences of no rainy days. Particularly, among the different Poisson models, a non-homogeneous Poisson model was selected and then applied to the daily rainfall series registered at the Cosenza rain gauge (Calabria, southern Italy), as test series. The aim was to evaluate the different behaviour of the dry spells observed in two different 30-year periods, i.e. 1951–1980 and 1981–2010. The analyses performed through Monte Carlo simulations assessed the statistical significance of the variation of the mean expected values of dry spells observed at annual scale in the second period with respect to those observed in the first. The model has then been verified by comparing the results of the test series with the ones obtained from other three rain gauges of the same region. Moreover, greater occurrence probabilities for long dry spells in 1981–2010 than in 1951–1980 were detected for the test series. Analogously, the return periods evaluated for fixed long dry spells through the synthetic data of the period 1981–2010 resulted less than half of the corresponding ones evaluated with the data generated for the previous 30-year period.

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Abbreviations

a mod(n):

Remainder of the Euclidean division of a by n

a 0, a j , b j :

Coefficients of the truncated Fourier series, with j = 1, 2,…,n h (days−1)

α 0, α j , β j :

Coefficients of the truncated Fourier series for the Monte Carlo simulations, with j = 1, 2,…,n h (days−1)

c :

Integration constant

D :

Period (in this case, average length of the year, days)

\( H_{0}^{{(n_{h} )}} \) :

Null hypothesis about the truncated Fourier series with n h harmonics

\( H_{0}^{{(\bar{m})}} \) :

Null hypothesis about the mean expected annual value \( \bar{m} \)

\( i_{n}^{'} \) :

First day of the nth sequence of no rainy days

int[u]:

Greatest integer number lower than u

inv f(x):

Inverse function of f(x)

K′ :

Number of consecutive time intervals with no rainfall (k′ = 0, 1, 2,…,)

\( k_{\hbox{max} }^{'} \) :

Maximum value of k′ over a time interval of length 1 year

\( k_{n}^{'} \) :

Number of no rainy days of the nth sequence of K′

\( k_{*}^{'} \) :

Threshold value of K′

λ(t):

Arrival intensity function (parameter of the Poisson process)

Λ(t):

Integral of the arrival intensity function λ(t)

L :

Number of rainy consecutive time intervals Δt belonging to a rainfall event started before the instant iΔt (l = 0, 1, 2,…,)

Lf :

Likelihood function

M :

Number of consecutive time intervals of equal length Δt (=1 day) with no rainfall, followed by at least one rainy day (m = 0, 1, 2,…,)

\( m_{*} \) :

Threshold value of M

M′:

Number of consecutive time intervals of length Δt (=1 day) without any arrival of rainfall events, followed by at least one rainy day (m′ = 0, 1, 2,…,)

\( \bar{m}_{X}^{(j)} \) :

Mean of the sample values of the variable X for the jth class

\( \bar{m}_{X}^{{({\text{year}}1 {-} {\text{year}}2)}} \) :

Mean of the sample annual values of the variable X for the period (year1–year2)

µ X :

Theoretical mean of the generic variable X

\( \bar{\mu }_{X,p}^{(j)} \) :

p-percentile of the mean value of the simulated series for the jth class of the variable X

\( \bar{\mu }_{X}^{{({\text{year}}1 {-} {\text{year}}2)}} \) :

Mean of the simulated annual values of the variable X for the period (year1–year2)

\( \bar{\mu }_{X,p}^{{({\text{year}}1 {-} {\text{year}}2)}} \) :

p-percentile of the mean value of the simulated series of the variable X in the period (year1–year2)

N c :

Number of sample data classes

N d :

Sample size of dry spells

N G :

Number of series generated through an embedded Monte Carlo procedure

n h :

Number of harmonics

\( \sigma_{X}^{2} \) :

Theoretical variance of the generic variable X

\( t_{R}^{{(n_{R} )}} \) :

Series of temporal arrival of sequences of consecutive no rainy days longer than 5 days with n R  = 1, 2,…,

T :

Return period

\( U^{{(n_{R} )}} \) :

Synthetic generation of uniformly distributed random values in the interval (0, 1) with n R  = 1, 2,…,

ω(t):

Arrival intensity function of the Monte Carlo simulation

Ω(t):

Integral of the arrival intensity function ω(t)

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Acknowledgments

The authors are grateful to the anonymous reviewers for the precious remarks and comments which led to improve the initial version of this paper.

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Sirangelo, B., Caloiero, T., Coscarelli, R. et al. A stochastic model for the analysis of the temporal change of dry spells. Stoch Environ Res Risk Assess 29, 143–155 (2015). https://doi.org/10.1007/s00477-014-0904-5

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