linear and non linear persistence in climate and its effect on the extremes
DESCRIPTION
Linear and non linear persistence in climate and its effect on the extremes. Armin Bunde, Sabine Lennartz, Mikhail Bogachev Justus-Liebig Universität Giessen. In cooperation with: E. Koscielny-Bunde (Giessen), H.J. Schellnhuber (PIK), - PowerPoint PPT PresentationTRANSCRIPT
Linear and non linear persistence in climate and its effect on the extremes
Armin Bunde, Sabine Lennartz, Mikhail Bogachev Justus-Liebig Universität Giessen
In cooperation with:
E. Koscielny-Bunde (Giessen), H.J. Schellnhuber (PIK), S. Havlin (Tel Aviv), D. Rybski (Giessen, PIK) H. v. Storch (GKSS), J. Eichner (Giessen, Re Munich)
)(S
I. Linear long-term correlations in climate
i
Climate records: Analysis problems: Finite Size Effects, Trends
i i
1,
2
)2)(1()( ssC sii
:0
:1
:1 white noise 1/f noise
non stationary
i
iii
xx
Seasonal mean
Seasonal standard deviation
Alternative: Fluctuation analysis
)2(
1~
22/1
)(2
h
ii ssF
s
2/)1(
2/1)2(
h
Advantage: Modifications (DFA1, DFA2, ...Wavelet Methods) allow to detect long-term correlations in the presence of trends, with reduced finite size effects
For the inverse problem of trend detection in the presence of long-term memory, with application to anthropogenic global warming, see talk by Sabine Lennartz on Thursday
Summary of the fluctuation exponents: (a) Observational data
J.Eichner et al, 2003, D. Rybski et al, 2004, 2006, E. Koscielny-Bunde et al, 1996, 1998, 2004
2/12/)1(,~)( ssF
(b) Model temperature data (1 000y): Erik the Red (Hamburg),
D. Rybski, A. Bunde, H. v. Storch, 2008, see also Fraedrich + Blender, 2006
Result for long-term correlated records with correlation exponent :
The return intervals are (a) long-term correlated with the same (b) and their probability density scales as
II Extreme events
threshold Q
return intervals ri
QQQ
ix~
QQQ RrRr
RrRrrP
,)/(ln)1(
,)/(~))(ln(
A. Bunde, J. Eichner, S. Havlin, J. Kantelhardt, 2005
Comparison with paleo-climate data
A. Bunde, J. Eichner, S. Havlin, J. Kantelhardt, 2005
III Risk estimation: Hazard function
t
Q
tt
t
Q
Q
drrP
drrP
ttW ;
Q
Q R
tWe
RrP QRr
1
Assume: Last Q-exceeding event occured t time units ago. We are interested in the probability that within the next time units at least one event occurs:
t
t ∆t
???
t
tQWrrP QQ
Q 1~
trivial prediction
strong nonlinear correlations
1
Q R
t
R
tWe
dr
drP
Rr linear long-term correlations
A. B., J. Eichner, J.Kantelhardt, S. Havlin, 2005; M. Bogachev, A.B., 2007, 2010
IV Precipitation and river run-offs
daysdays
i
i
Precipitation
River run-offs
To obtain the proper α-value, we shift
the multifractal spectrum by H´
Cascade model:
V Non linear correlations: Multifractality
Generalized fluctuation function depends on q: Multifractality
)2(h qhssqFs
ii
~1
/1
)(
See also: Schertzer, Lovejoy et al, Kantelhardt et al, Koscielny- Bunde et al, 2000-2006
VI PDF of the return intervals
Weak deviations from exponential: result of weak
linear and nonlinear memory .
Pronounced power law behavior independent of α, result of strong nonlinear
memory
End of the talk
Instrumental record
Historical run
Instrumental recordHistorical runControl runHistorical run (biannual)
Reconstructed record (Kaplan)Historical runControl runHistorical run (biannual)
Historical run
(b) Temperature, precipitation and run-off records
22,~)(~)( ssCssF