\[ \frac{\partial\vec{C}}{dt}=\vec{V}.\nabla_{\{x,y\}} \vec{C} + 0.1\Delta_{\{x,y\}} \vec{C} \]
in 2d domain [-1,-1]*[1,1] with the boundary conditions on the walls as no-slip for velocity \(\vec{V}=0\) and sink for the chemicals \(\vec{C}=0\) for all time \(t\). Further, we start with the initial condition for the concentration as
\[\vec{C}=\begin{cases} (1,0)\text{ for } x=0,-0.5<y<0\\ (0,1)\text{ for } x=0, 0<y<0.5\\ (0,0) \text{ for the rest of the domain}\\ \end{cases} \]
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