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Universitā degli studi di Roma “Tor Vergata” - ART - TORVERGATA ...

Universitā degli studi di Roma “Tor Vergata” - ART - TORVERGATA ...

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where Ix is the advective flux in x <strong>di</strong>rection [g m -2 s -1 ]; ux is the average longitu<strong>di</strong>nal velocity [m<br />

s -1 ]; c is the tracer concentration [g m -3 ]. The Lagrangian system, which lies at the centre of the<br />

tracer cloud (collection of fluid parcels whose <strong>di</strong>mension are comparable with the smallest length<br />

scale of interest and with velocity and concentration characteristics), is use for advection.<br />

The molecular <strong>di</strong>ffusion is modelled by the Fick’s law:<br />

∂c<br />

J x = −em<br />

∂x<br />

Eq. 2.2-6<br />

where Jx is the molecular <strong>di</strong>ffusive flux in the x <strong>di</strong>rection [g m -2 s -1 ]; em is the molecular <strong>di</strong>ffusion<br />

coefficient whose typical value in water changes between 0.5 – 2.0 x 10 -9 [m 2 s -1 ]; δc/δx is the<br />

tracer concentration gra<strong>di</strong>ent in the x <strong>di</strong>rection [g m -4 ]. The negative sign means that the<br />

molecular <strong>di</strong>ffusion develops in the opposite <strong>di</strong>rection of the concentration gra<strong>di</strong>ent. The<br />

molecular <strong>di</strong>ffusion is defined in a fixed Eulerian coor<strong>di</strong>nates.<br />

The advection/<strong>di</strong>ffusion three <strong>di</strong>mensional equation can be derived from a mass balance<br />

on a rectangular parcel fluid moving at mean velocity is in rectangular Cartesian coor<strong>di</strong>nates 2 :<br />

∂c<br />

+<br />

∂t<br />

3<br />

∑<br />

⎛ ∂c<br />

⎞ ⎡<br />

⎜<br />

⎜u<br />

⎟ i = em<br />

⎢<br />

⎝ ∂x<br />

⎠ ⎣<br />

∑<br />

2 ⎛ ∂ c ⎞⎤<br />

⎜<br />

⎟ 2 ⎥<br />

⎝ ∂x<br />

⎠⎦<br />

i= 1 i<br />

i= 1 i<br />

3<br />

Eq. 2.2-7<br />

where ui is the average velocity along the three orthogonal <strong>di</strong>rections defined by the rectangular<br />

Cartesian coor<strong>di</strong>nates [m s -1 ] where 1=“x”, 2=”y” and 3=”z”.<br />

A solution of this system for:<br />

a. a conservative tracer;<br />

b. known initial con<strong>di</strong>tions;<br />

c. stationary situation;<br />

d. unbounded channel;<br />

allows us seeing that the variance of tracer cloud increase linearly with time.<br />

If the Reynolds number is below 500 the flow is laminar, if it is above about 2000 the<br />

flow is turbulent which is generated by velocity shears where there are velocity gra<strong>di</strong>ents. In a<br />

turbulent flow the tracer spread more rapidly than in the first one.<br />

2 It is considered the right Cartesian coor<strong>di</strong>nate system.<br />

41

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