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BREAKING BAR MIGRATION
INDUCED BY INFRAGRAVITY WAVES
H. Michallet
M.V.L. Rocha and P.A. Silva
With many thanks to: E. Barthélemy, Joël Sommeria, F. Bonnel
XBeachXConference – Delft - 1.11.2017
• LEGI Wave flume
36 m / 0.55 m
• Controlled wave maker
irregular waves
• Hydrodynamics
Froude scaling
length scale 1:10
• Loose bed
Shields / Rouse scaling
• Morphodynamics (Grasso et al. 2009, 2011)
• Boundary layer (Berni et al. 2013, 2017)
• Liquefaction (Scholtès et al. 2015)
• Morpho / long waves (Rocha 2016)
lightweight sediment
d50 = 0.64 mm
r = 1.18
Physical model of
beach morphodynamics
2 conditions
of 2 groups
of bichromatic waves
Tp = 1.7 s Tg = 14 s
differing in LF component
C1
C2
beach profiles
and changes
surface elevation maximum
mean
minimum
wave skewness
asymmetry
Wave height short waves
LF
Net sediment transport
C1 : onshore bar migration
C2 : offshore
same
Tp = 1.7 s Tg = 14 s
less LF amplitude
(less grouping)
C1
C3
C1 : offhore bar migration
C3 : onshore
HSW
HLF
AS
wave propagation
wave gage
Video evidence 200 frames/s
of phase lags in boundary layer flow and sediment transport (here 1/10 frames)
Video analysis
of succesive frames
to get velocity fields (CIV)
and sediment concentration
(pixel brightness)
Need to identify :
air entrainment
sediment concentration
gradients / grey scale
erosion
bed dilation
divergencevorticity
Velocity fields
Normalized pixel brightness
Horizontal velocity
Bed response to breaking waves
Plug flow jet impact increasing erosion, suspension …
Horizontal velocity
Sediment concentration
Maximum erosion and transport of a dense bed layer
at the end of the group
Low-pass filtered horizontal velocity
Sediment concentration
Maximum erosion and transport of a dense bed layer
at the end of the group / LF off-shore flow
Sediment flux / surface elevation
vertically integrated
net transport
average
concentration
undertow
Net transport primarily in the bed layer, with LF trend
net transport over 4 runs
4 runs of same condition C1
for 1 run from video
10 successive runs of same condition C2
bar formation, off-shore migration
• Light-weight sediment
small-scale physical model
+ CIV-UVMAT :
further insight into
sediment transport
mechanisms
(e.g. Roelvink & Stive, 1989,
Sleath, 1999)
• Evidence of leading flow acceleration induced bed motion
(plug flow vs. sheet flow, see Berni et al., 2017, likely to occur in the field,
see large scale experiments by Anderson et al. 2017)
• Moving bed layer increases along the wave group, advected at LF
• For similar short waves, increase / decrease in LF energy
promotes off-shore / onshore bar migration
Conclusions

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DSD-INT 2017 Breaking bar migration induced by infragravity waves - Michallet

  • 1. BREAKING BAR MIGRATION INDUCED BY INFRAGRAVITY WAVES H. Michallet M.V.L. Rocha and P.A. Silva With many thanks to: E. Barthélemy, Joël Sommeria, F. Bonnel XBeachXConference – Delft - 1.11.2017
  • 2. • LEGI Wave flume 36 m / 0.55 m • Controlled wave maker irregular waves • Hydrodynamics Froude scaling length scale 1:10 • Loose bed Shields / Rouse scaling • Morphodynamics (Grasso et al. 2009, 2011) • Boundary layer (Berni et al. 2013, 2017) • Liquefaction (Scholtès et al. 2015) • Morpho / long waves (Rocha 2016) lightweight sediment d50 = 0.64 mm r = 1.18 Physical model of beach morphodynamics
  • 3. 2 conditions of 2 groups of bichromatic waves Tp = 1.7 s Tg = 14 s differing in LF component C1 C2 beach profiles and changes surface elevation maximum mean minimum
  • 4. wave skewness asymmetry Wave height short waves LF Net sediment transport C1 : onshore bar migration C2 : offshore
  • 5. same Tp = 1.7 s Tg = 14 s less LF amplitude (less grouping) C1 C3 C1 : offhore bar migration C3 : onshore HSW HLF AS
  • 6. wave propagation wave gage Video evidence 200 frames/s of phase lags in boundary layer flow and sediment transport (here 1/10 frames)
  • 7. Video analysis of succesive frames to get velocity fields (CIV) and sediment concentration (pixel brightness) Need to identify : air entrainment sediment concentration gradients / grey scale
  • 9. Normalized pixel brightness Horizontal velocity Bed response to breaking waves Plug flow jet impact increasing erosion, suspension …
  • 10. Horizontal velocity Sediment concentration Maximum erosion and transport of a dense bed layer at the end of the group
  • 11. Low-pass filtered horizontal velocity Sediment concentration Maximum erosion and transport of a dense bed layer at the end of the group / LF off-shore flow
  • 12. Sediment flux / surface elevation vertically integrated net transport average concentration undertow Net transport primarily in the bed layer, with LF trend
  • 13. net transport over 4 runs 4 runs of same condition C1 for 1 run from video
  • 14. 10 successive runs of same condition C2 bar formation, off-shore migration
  • 15. • Light-weight sediment small-scale physical model + CIV-UVMAT : further insight into sediment transport mechanisms (e.g. Roelvink & Stive, 1989, Sleath, 1999) • Evidence of leading flow acceleration induced bed motion (plug flow vs. sheet flow, see Berni et al., 2017, likely to occur in the field, see large scale experiments by Anderson et al. 2017) • Moving bed layer increases along the wave group, advected at LF • For similar short waves, increase / decrease in LF energy promotes off-shore / onshore bar migration Conclusions