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Potential mechanism for the initial formation of rhythmic coastline features M.van der Vegt, H.M....

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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 Atmospheric research Utrecht, Utrecht University, The Netherlands “ Tidal motion can cause coastline variations with wave lengths of a couple of kilometers “
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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.

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.

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.

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.

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.

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.

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

Page 7: 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.

Results: Growth rate curve

)1(155)( / foldingexexH

Page 8: 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.

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.

Mechanism behind model results: vorticity dynamics

vdx

dH

H

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.

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.

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


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