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Instantaneous Point-source Solution - IfH

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Section 5: <strong>Point</strong>-<strong>source</strong> solution with advection 19<br />

5. <strong>Point</strong>-<strong>source</strong> solution with advection<br />

The final step is to substitute the coordinate transformation for the<br />

moving reference frame into the point <strong>source</strong> solution (35). In the<br />

moving coordinate system, this solution is<br />

( )<br />

M<br />

C(ξ, τ) =<br />

A √ 4πDτ exp − ξ2<br />

. (37)<br />

4Dτ<br />

Our coordinate transformation was ξ = x − (x 0 + ut) and τ = t.<br />

Substituting into (37) gives:<br />

(<br />

M<br />

C(x, t) =<br />

A √ 4πDt exp − (x − (x 0 + ut) 2 )<br />

. (38)<br />

4Dt<br />

Figure 5 shows the schematic behavior of this solution for three different<br />

times, t 1 , t 2 , and t 3 . A second animation shows this solution<br />

in action.<br />

[PgUp] [PgDn] [Back]

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