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EXPERIMENTS ON EXTREME WAVE GENERATION BASED ON SOLITON ON FINITE BACKGROUND René Huijsmans(MARIN) Gert Klopman (AFR) Natanael Karjanto,Brenny van Groesen.

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Presentation on theme: "EXPERIMENTS ON EXTREME WAVE GENERATION BASED ON SOLITON ON FINITE BACKGROUND René Huijsmans(MARIN) Gert Klopman (AFR) Natanael Karjanto,Brenny van Groesen."— Presentation transcript:

1 EXPERIMENTS ON EXTREME WAVE GENERATION BASED ON SOLITON ON FINITE BACKGROUND René Huijsmans(MARIN) Gert Klopman (AFR) Natanael Karjanto,Brenny van Groesen (U Twente) Aan Andonowatti (ITB)

2 OUTLINE Introduction Soliton on finite Background Results of Experiments Analysis with 2-D non-linear potential code and sNLS Conclusions

3 Spatial NLS equation Free-surface elevation with: Spatial NLS equation: Where and are the carrier wave number and frequency

4 Spatial NLS coefficients: with and and are the bound long-wave amplitude coefficients

5 SOLITON ON FINITE BACKGROUND (SBF) as a solution of (spatial) NLS Physics of SFB van Groesen, A, N. Karyanto Amplitude amplification 1 3 Phase singularity t Parameters of SBF + cc

6 typical wave tank, 250m long 0 L LARGE AMPLITUDE A snapshot of wave elevation under Maximum Temporal Amplitude (MTA) curve Location of wave maker MTA

7 EXPERIMENTS A: DEPTH H0 = 3.55m, various EXPERIMENTS B: DEPTH H0 = 3.55m, various EXPERIMENTAL CASES C2M0C2M2 EXPERIMENTS C: DEPTH H0=3.55m, various Main Characteristics CASES TO BE PRESENTED

8 Overview of Experimental Test Set-Up

9 10m 40m C2M2 100m Prediction of focus point: 150m from the wave maker

10 10m 150m C2M2 160m Prediction of focus point: 150m from the wave maker

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13 160m 150m In between 2 peaks: 11 waves C2M2

14 150m 160m 150m

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18 ANALYSIS With HUBRIS/sNLS

19 ANALYSIS With HUBRIS

20 ANALYSIS With HUBRIS/sNLS

21 ANALYSIS With HUBRIS

22 ANALYSIS With HUBRIS/sNLS

23 ANALYSIS With HUBRIS

24 Conclusions MTA approach good basis for predicting Focus point Phase singularity clearly present at one side of the wave group Non-linear potential flow code and sNLS partly predicts the evolution of the SFB soliton


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