Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M....
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![Page 1: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/1.jpg)
Potential mechanism for the initial formation of rhythmic coastline features
M.van der Vegt, H.M. Schuttelaars and H.E. de SwartInstitute for Marine and Atmospheric research Utrecht, Utrecht University, The
Netherlands
“ Tidal motion can cause coastline variations with wave lengths of a couple of kilometers “
![Page 2: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/2.jpg)
Mesoscale rhythmic coastlines
Shoreline sand waves: planimetric variations of coastline
1-10 km
C 100m/yr
A10-100 m
Red colors: protrudingBlue colors: retreating
(adapted from Ruessink&Jeuken,2002)
Protruding or retreating coast
![Page 3: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/3.jpg)
Motivation
• Waves and tides are potentially important
• Tides not considered so far
• Can tidal motion cause initial formation of rhythmic coastline features?
• What are the underlying physical mechanisms?
Research questions
![Page 4: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/4.jpg)
Physical model
• Geometry:
• Assumptions: - Near shore zone has constant width- Sediment transport q only in near shore zone- Sediment transport determined by velocities at transition line
20 m
5 m
10 km
500 m
q
Side view
Top view
CoastlineTransition line
Inner shelfTideNear shore
zone
![Page 5: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/5.jpg)
Physical model
• 2-DH Shallow water equations, no diffusion, rigid lid approximation. Only on inner shelf.
• Boundary conditions: at x=xt and at x
• Width-integrated sediment transport for the near shore zone:
• Tm>>T Coastline evolution is slow and tidally averaging is allowed
• Alongshore variations of sediment transport causes changes of shoreline position. No change of bathymetry.
0nu
0u
txxuq
//
![Page 6: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/6.jpg)
Basic state and perturbations
• The model allows for a basic state with uniform alongshore conditions
• Note that basic state velocity has vorticity: • Basic state is perturbed by perturbation of coastline• Solutions cyclic in y and t. Model calculates initial
complex growth rate
xV
imre iC
oastV(x,t)
Sea 1 m/s
NearShorezone
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Results: Growth rate curve
)1(155)( / foldingexexH
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Residual flow on inner shelf
• Tidal residual circulations cells Vorticity dynamics?• Growth determined by depth dependent friction• Coriolis force migration
Without Coriolis effects With Coriolis effects
![Page 9: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/9.jpg)
Mechanism behind model results: vorticity dynamics
vdx
dH
H
rω
H
r
y
Ωv
y
ωV
x
Ωu2
Basic state velocity:V
Basic state vorticity:
xV
Perturbed velocity: u,v
Perturbed vorticity:
yx uv
UnstableStable
![Page 10: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/10.jpg)
Battle between the fluxes
• Stabilizing fluxes in cross-shore, destabilizing in alongshore direction
• Convergence cross-shore flux ~ width of inner shelf
• Convergence alongshore flux ~ wave length
Positive growth rate for < width inner shelf
![Page 11: Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M. Schuttelaars and H.E. de Swart Institute for Marine and.](https://reader030.fdocuments.us/reader030/viewer/2022032600/56649db55503460f94aa62d6/html5/thumbnails/11.jpg)
Conclusions
• Tidal motion can initially form rhythmic coastlines• Length scale in the range of shoreline sand waves • Steeper profile Critical wave length shorter • Mechanism can be understood in terms of vorticity
fluxes. Cross-shore Alongshore fluxes• No damping mechanism• With diffusion a preferred mode will occur
• Inclusion of wave action diffusion• Model parameterization
Future work