Probable Maximum Flood estimation using upper bounded...

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Probable Maximum Flood estimation using upper bounded statistical models and its upper bounded statistical models and its effect on high return period quantiles By: By: Félix Francés and Blanca Botero 3 rd International Week on Risk Analysis, Dam Safety, Dam Security and Critical Infrastructure Management Dam Security , and Critical Infrastructure Management Valencia, Spain, October 18-19, 2011

Transcript of Probable Maximum Flood estimation using upper bounded...

Page 1: Probable Maximum Flood estimation using upper bounded ...lluvia.dihma.upv.es/ES/publi/congres/058_PMFenValencia2011_FF.pdfIntroduction The PMF is the biggest flood physically possible

Probable Maximum Flood estimation using upper bounded statistical models and itsupper bounded statistical models and its

effect on high return period quantiles

By:By:Félix Francés and Blanca Botero

3rd International Week on Risk Analysis, Dam Safety, Dam Security and Critical Infrastructure ManagementDam Security, and Critical Infrastructure Management Valencia, Spain, October 18-19, 2011

Page 2: Probable Maximum Flood estimation using upper bounded ...lluvia.dihma.upv.es/ES/publi/congres/058_PMFenValencia2011_FF.pdfIntroduction The PMF is the biggest flood physically possible

IntroductionIntroduction

The PMF is the biggest flood physically possible at aThe PMF is the biggest flood physically possible at a specific catchment (Smith and Ward, 1998)

It has a physical meaningIt has a physical meaningand provides an upper limit for the decision makerfor the decision maker

It will change the cdf T rIt will change the cdfbehaviour at medium and high return periods

Thigh return periods

xmin ∞X g

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IntroductionIntroduction

High return period quantile estimation main drawback:High return period quantile estimation main drawback: lack of available information about large events in a relatively short data series => increase amount of yinformation

One possibility is to included palaeoflood and/or historic information. From now, Non-Systematic information:Information different to the systematic record at the flow gauge stationN diff f th t ti ti l i t f i !No differences from the statistical point of view!

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Page 4: Probable Maximum Flood estimation using upper bounded ...lluvia.dihma.upv.es/ES/publi/congres/058_PMFenValencia2011_FF.pdfIntroduction The PMF is the biggest flood physically possible

IntroductionIntroduction

High return period quantile estimation main drawback:High return period quantile estimation main drawback: lack of available information about large events in a relatively short data series => increase amount of yinformation

Obj ti i d t i i ti k l d dObjective: merging deterministic knowledge and statistical analysis to better estimate high return period quantiles in a framework of enough informationquantiles in a framework of enough information

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LN4 - Slade transformationLN4 - Slade transformation

Applied by Takara and Loebis (1996)Applied by Takara and Loebis (1996)Basic distribution function Y ~ LN2

⎞⎛ axSlade-type transformation: ⎟⎟

⎞⎜⎜⎝

⎛−−=

xgaxy ln

⎤⎡ 2

Resulting pdf: ( )( )⎥⎥⎥

⎢⎢⎢

⎪⎭

⎪⎬⎫

⎪⎩

⎪⎨⎧ −

−−−−

=2

21exp

2)(

y

y

y

yxgaxagxf

σμ

πσ

Parameters:g = upper bound (PMF)

⎥⎦⎢⎣

g pp ( )a = lower bound, set to 0 to reduce the # of parametersμy, σy = LN parameters

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TDF - Elíasson transformationTDF - Elíasson transformation

Developed by Elíasson (1997)Developed by Elíasson (1997)Basic distribution function: Y ~ EV1 (or Gumbel)

2Transformation:

⎤⎡ ⎞⎛( )XgakXY−

−=2*

Resulting cdf:Parameters:

( ) ⎥⎥⎦

⎢⎢⎣

⎟⎟⎠

⎞⎜⎜⎝

⎛−

−+

−−= b

xgak

axxF *expexp)(

Parameters:g = upper bound (PMF)k* = transformation parameter = –0.5 for better resultspa = scale and transformation parameterb = location parameter

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EV4 modelEV4 model

It was derived from a GEV (Takara and Tosa 1999)It was derived from a GEV (Takara and Tosa, 1999)

⎤⎡ 'k

The resulting cdf is:⎥⎥⎦

⎢⎢⎣

⎭⎬⎫

⎩⎨⎧

−−

−='

)(exp)(

k

axxgxF

ν

P t

⎦⎣ ⎭⎩

Parameters:a = lower bound (set to 0 to reduce # of parameters)g = upper bound (PMF)g = upper bound (PMF)v = scale parameterk’ = shape parameter

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k = shape parameter

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The Jucar River case studyThe Jucar River case study

Relative large basin: 22 000 km2Relative large basin: 22,000 km

Mediterranean torrential regimegMean flow = 36 m3/sMean flood = 713 m3/s

3Q20= 2,000 m3/sCoefficient of variation = 2.74Skewness coefficient = 5 26Skewness coefficient = 5.26

Very strong Convective Mesoscale Systems in Fall (Rigo y g y ( gand Llasat, 2007)

Mixed flood population (Rossi et al., 1984)

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Sources of Non-Systematic InformationSources of Non-Systematic Information

Hi t i l i f tiHistorical informationArchives: municipality records notary notesrecords, notary notes, engineering damage reportsreports Newspapers, books, chroniclesMaps, photographs, plansBuilding marksgOral communications

Plan of the two biggest floods in XIX century floods at Pont

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gg yd’Arc (Ardèche River in France)

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Sources of Non-Systematic InformationSources of Non-Systematic Information

Palaeoflood informationBotanical evidencesPalaeolevel indicators

Slackwater depositsSlackwater depositsSilt marks

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Sources of Non-Systematic InformationSources of Non-Systematic Information

Palaeoflood informationBotanical evidencesPalaeolevel indicators

Slackwater depositsSlackwater depositsSilt marks

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Sources of Non-Systematic InformationSources of Non-Systematic Information

J t d ith hi t i lJucar case study with historical information (building marks): flooding of an ancient convent located

Year Peak Q (m3/s)

1805 8,400

1814 6 400flooding of an ancient convent located in the floodplain

Threshold of inundation XH =

1814 6,400

1864 13,000

Threshold of inundation XH 6,200 m3/sHistorical period: 1792 to 1945p

Stationarity was tested and provedy pusing the Lang Test (Lang et al., 1999)

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)

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Upper limit estimationUpper limit estimation

ML PG: g is fixed at the value previously calculated (G)ML-PG: g is fixed at the value previously calculated (G) as the best approximation for the true unknown PMF, and the other parameters are estimated by ML method:p y

⎭⎬⎫

Θ=

)'(max LGg

⎭Θ )(max L

ML-C: the whole parameters set of the distribution function is estimated by the ML method, including g as another free parameter in the maximization process:another free parameter in the maximization process:

)(max ΘL

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)(

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Upper limit estimationUpper limit estimation

In some combinations of distribution + type ofIn some combinations of distribution + type ofinformation, ML-C estimates g as the maximumobservation =>

ML-GE: This method consists on the use of the GenericML GE: This method consists on the use of the Generic Equation to estimate g (Kijko, 2004) and the ML method for the rest of parameters:

⎪⎬⎫

Θ+= ∫ )],';([max dxgxFxgg

nX

⎪⎭⎬

Θ

∫∞−

)'(max

)],;([max

L

gg X

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ML-PG (prefixed g)ML-PG (prefixed g)

PMF i ifiPMF using specific discharge from upstream PMF study = 33 900 m3/sPMF study 33,900 m /s => possible overestimation

“D l ” ff t d t“Dog leg” effect due to mixed populations

TDFClear different approach to the upper limit

TDFLN4EV4

Slower for TDFFaster for EV4

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ML-C (complete ML)ML-C (complete ML)

PMF ith EV4 d TDFPMF with EV4 and TDF ML-C = 13,000 m3/s (maximum observation)(maximum observation)

PMF with LN4 ML-C =PMF with LN4 ML C 93,300 m3/s

TDFTDFLN4EV4

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ML-GE (mixed with generic equation)ML-GE (mixed with generic equation)

N i l bl ithNumerical problems with LN4

PMF with EV4 ML-GE = 18 100 m3/s18,100 m /s

PMF with TDF ML-GE =TDF PMF with TDF ML-GE = 93,100 m3/s

TDFLN4EV4

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Models comparisonModels comparison

EV4 better performance with high skewnees coefficientEV4 better performance with high skewnees coefficient, as it was pointed out by Takara and Tosa (1999)

Llobregat SegreLlobregat Segre

TuriaOnyar

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EV4 uncertainty analysisEV4 uncertainty analysis

Monte CarloMonte Carlo simulations with:

N= 50 yearsN 50 yearsM = 400 yearsH = 50 yearsH = 50 years return periodγ = 5.77γx 5.77

Errors in G withErrors in G withCV = 0.3bias = +10%

( )100

ˆ1

(%)1

2

θ

θθ∑ =−

=

N

i iNE

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bias 10%

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EV4 uncertainty analysisEV4 uncertainty analysis

γ = 5 77γx = 5.77

γx = 2.39

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ConclusionsConclusions

Why not explore and use upper bounded distributionWhy not explore and use upper bounded distribution functions?

There is an upper limitThere is an upper limit Upper bounded and unbounded distributions behave different at medium and high return periodsdifferent at medium and high return periods

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ConclusionsConclusions

Why not explore and use upper bounded distributionWhy not explore and use upper bounded distribution functions?

The upper limit represents the PMF and either can be:Causal information expansion (Merz and Blöschl,Causal information expansion (Merz and Blöschl, 2008), if it is fixed a priori

Within a temporal information expansionframework (Merz and Blöschl, 2008), considered as

t t b ti t d i th t ti ti lone more parameter to be estimated in the statistical model fitting

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RemarksRemarks

Program AFINS available at http://lluvia dihma upv esProgram AFINS available at http://lluvia.dihma.upv.es

Poster: High return period annual maximum reservoirPoster: High return period annual maximum reservoir water level quantiles estimation using synthetic generated flood eventsgenerated flood events

Many thanks for your attention!Many thanks for your attention!

Prof. Félix Francés ([email protected])( @ p )Research Group in Hydrological and Environmental Modelling (GIMHA)

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