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Advanced delta change method for time series transformation Jules Beersma Adri Buishand & Saskia van Pelt Workshop “Non-stationary extreme value modelling in climatology” Technical University of Liberec February 15-17, 2012
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Page 1: Jules Beersma: Advanced delta change method for time series transformation

Advanced delta change method for time series transformation

Jules BeersmaAdri Buishand & Saskia van Pelt

Workshop “Non-stationary extreme value modelling in climatology”

Technical University of LiberecFebruary 15-17, 2012

Page 2: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 2

Outline

• Introduction

• Delta methods

• Study area: Rhine basin

• Results

• Conclusions

• Future work

• Natural variability…

Page 3: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 3

Introduction

Climate model

Impact modele.g. change in river discharge

Direct methodDelta method

or

Time series transformation

?

Page 4: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 4

Delta method

Temperature: additive change

T* = T + (TF –TC)

Precipitation: factorial change

P* = PF / PC × P

Page 5: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 5

Delta method

● Linear: P* = aP (classical delta method)

Relative change in std. deviation and all quantiles is the same as that in the mean

● Non-linear: P* = aPb

Changes in the quantiles different from the change in the mean if b ≠ 1

May however give unrealistic changes in the extremes if b > 1

Page 6: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 6

Advanced delta method

P* = aPb for P ≤ Q

P* = aQb + EF/EC (P - Q) for P > Q

where:

Q is a large quantile

EC is the mean excess over the quantile Q in the Control climate

EF the same for the Future climate

Coefficients a and b follow from future changes in e.g. P0.60 and P0.90

Page 7: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 7

P* = aPb for P ≤ Q

P* = aQb + EF/EC (P - Q) for P > Q

Advanced delta method

b11

bC0.60

F0.60 g(PPa )

)}P/(gP{g

)}P/(gP{gb

C0.601

C0.902

F0.601

F0.902

log

log

C0.60

O0.601 PPg C

0.90O

0.902 PPg

Page 8: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 8

Advanced delta method

P* = aPb for P ≤ Q

P* = aQb + EF/EC (P - Q) for P > Q

This transformation is obtained if:

● Excesses follow a Generalized Pareto Distribution (GPD)

● The shape parameter of the GPD does not change

May be robust against the GPD, but it is essential that the shape of the upper tail does not change

difficult to check

Page 9: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 9

Advanced delta method

0 ,)/1(1)( /1 xxxG

11

GxG

Generalized Pareto Distribution:

F

CCFCFx

x 1/1 /

Quantile function (inverse):

Assume GC and GF are the distributions of the excesses in the Current and the Future climate with respectively σC , κC and σF , κF then:

xGGx CF1

Page 10: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 10

Advanced delta method

If then:

And the mean of the excesses:

Similarly for the Weibull distribution:

CF

11 E

1

E

xx CF )/(

xx CF )/( and

and thus xEEx CF )/(

F

CCFCFx

x 1/1 /

Page 11: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 11

Points of attention (1)

Q =Default

(SPLUS, R)Median

unbiased

P0.90 1.25 1.23

P0.95 1.29 1.12

P0.95, overlapping 5d 1.25 1.21

Choice of QChange in mean excess EF / EC

(Empirical estimates based on order statistics)

Page 12: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 12

Points of attention (2a)

Bias correction factors

are needed to correct coefficients a and b because of systematic climate model biases in PC

0.60 and PC0.90:

g1 = PO0.60 / PC

0.60

g2 = PO0.90 / PC

0.90

Page 13: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 13

Points of attention (2b)

Effect of bias correction factors

Relative change in the mean annual maxima of 10-day basin-average precipitation

Page 14: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 14

Points of attention (3)

Smoothing

Smoothing of coefficients and quantiles in space and/or time

P0.60 and P0.90: varies over the year (3-month moving average)

EF / EC and b: varies over the year but smoothed spatially

a: varies over the year and over space

Page 15: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 15

Study area:Rhine basin

13 GCMs & 5 RCMs(A1B)

134 sub catchments (for hydrological modelling)

Extreme river discharges Extreme multi-day precipitation amounts

5 RCMs; bias corrected, direct method

Page 16: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 16

Study area:Rhine basin

● P ≡ 5-day precipitation sums at the grid cell scale

● Quantiles P0.60 and P0.90 , coefficients a and b and excesses E are calculated for each grid cell and each calendar month:

● a calendar month is six 5-day periods (= 30 days) or

● zeven 5-day periods (= 35 days) for December

● Temporal smoothing (3-month moving averages) of quantiles and excesses

● Spatial smoothing (median of grid cells) of b and EF / EC similar effect as regional frequency analysis

Page 17: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 17

Schematicrepresentation of the procedure

Page 18: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 18

Schematicrepresentation of the procedure

Page 19: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 19

Schematicrepresentation of the procedure

Page 20: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 20

Schematicrepresentation of the procedure

● Each sub basin gets the same R as the corresponding grid cell

● Daily amounts get the same R as the 5-day amounts

Page 21: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 21

Results (1a)

● 13 GCMs (A1B)

● 5 RCMs (A1B)

● 5 RCMs (bias corrected; direct method)

Page 22: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 22

Results (1b)

GCM RCM GCM References RCM References

CGCM3.1T63 CNRM-CM3

(Flato, 2005)(Salas-Mélia et al., 2005)

CSIRO-Mk (Gordon et al., 2002)

ECHAM5r1 REMO_10 (Roeckner et al., 2003) (Jacob, 2001)

ECHAM5r3 RACMOREMO

(Lenderink, 2003)(Jacob, 2001)

GFDL-CM2.0 (Delworth et al., 2006)

GFDL-CM2.1

HADCM3Q0 CLM (Gordon et al., 2000) (Steppeler et al., 2003)

HADCM3Q3 HADRM3Q3 (Jones, 2004)

IPSL-CM4 (Marti et al., 2005)

MIROC3.2 hires (Hasumi and Emori, 2004)

MIUB (Min et al., 2005)

MRI-CGCM2.3.2 (Yukimoto et al., 2006)

Page 23: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 23

Results (1c)

● 13 GCMs (A1B)

● 5 RCMs (A1B)

● 5 RCMs (bias corrected; direct method)

Quantiles of 10-day precipitation

● Future (2081 – 2100) w.r.t. Current (1961-1995) climate

● basin-average

● winter half year (Oct – Mar)

Page 24: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 24

Results (2)

13 GCMs 5 RCMs

10-

da

y p

rec

ipit

ati

on

(m

m)

Page 25: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 25

Results (3)

10-

da

y p

rec

ipit

ati

on

(m

m)

Deltamethod

Biascorrection

Page 26: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 26

Conclusions

● Extreme quantiles of 10-day basin-average precipitation in winter increase in the future climate in all (18) climate model simulations

● 13 GCMs and 5 RCMs have similar spread in extreme quantiles of 10-day basin-average precipitation

● Similar changes and spread of changes between the 5 RCMs based on the (advanced) delta method and on a (non-linear) bias correction method.

Page 27: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 27

Future work

● Large ensemble of GCMs ~50 from CMIP5

● Coupling to hydrological model (HBV) of the Rhine

● Test performance under dry conditions (left tail)

● Application to different river basins / areas?

● Advanced delta change method for daily precipitation rather than 5-day amounts problem of changing wet/dry day frequency

● Use of a similar transformation to remove the precipitation bias in RCM output (bias correction method)

Page 28: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 28

Natural variability…

13 GCMsEssence

10-

da

y p

rec

ipit

ati

on

(m

m)

Natural variability dominates uncertainty range

Page 29: Jules Beersma: Advanced delta change method for time series transformation

TU of Liberec, 15-17 February 2012 29

Natural variability…

How good can we determine the real climate

change signal in extremes?


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