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Three-dimensional Lagrangian Tracer Modelling in Wadden Sea ...

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CHAPTER 3. IDEALISED TESTCASES 45<br />

z/D<br />

z/D<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

0 1 2 3 4<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

k [m 2 /s 2 ] ⋅ 10 −4<br />

0<br />

0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16<br />

u [m/s]<br />

a)<br />

c)<br />

z/D<br />

z/D<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

0 0.5 1 1.5 2<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

ε [m 2 /s 3 ] ⋅ 10 −5<br />

0<br />

0 0.005 0.01 0.015<br />

ν [m 2 /s]<br />

eddy viscoity ν t<br />

eddy diffusivity ν’ t<br />

Fig. 3.2.1: Vertical profiles of a) the turbulent k<strong>in</strong>etic energy k, b) the energy<br />

dissipation rate ε, c) the zonal velocity component u and d) the eddy diffusivity ν ′ t<br />

and viscosity νt.<br />

Depth z [m] CSed,Euler[kg/m 3 ] CSed,Lagrange[kg/m 3 ] CSed,analytical[kg/m 3 ]<br />

−0.5 1.03 · 10 −3 1.07 · 10 −3 1.04 · 10 −3<br />

−1.5 3.69 · 10 −4 3.59 · 10 −4 3.62 · 10 −4<br />

−2.5 2.65 · 10 −4 2.63 · 10 −4 2.59 · 10 −4<br />

−3.5 2.13 · 10 −4 2.14 · 10 −4 2.09 · 10 −4<br />

−4.5 1.78 · 10 −4 1.72 · 10 −4 1.70 · 10 −4<br />

−5.5 1.51 · 10 −4 1.49 · 10 −4 1.47 · 10 −4<br />

−6.5 1.28 · 10 −4 1.23 · 10 −4 1.25 · 10 −4<br />

−7.5 1.07 · 10 −4 1.05 · 10 −4 1.05 · 10 −4<br />

−8.5 8.64 · 10 −5 8.74 · 10 −5 8.40 · 10 −5<br />

−9.5 6.28 · 10 −5 6.41 · 10 −5 6.10 · 10 −5<br />

Table 3.2.1: Sediment concentrations at ten different depths calculated by the<br />

Eulerian scheme, the correct random walk model and the analytical solution.<br />

b)<br />

d)

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