As goes to zero, the unique solution of the scalar advection-diffusion equation $y^{\varepsilon}t-\varepsilon y^{\varepsilon}{xx} + M y^{\varepsilon}x=0(x,t)\in (0,1)\times (0,T)(\varepsilon)(\sqrt{\varepsilon})T$ is large enough, these thin layers where the solution displays rapid variations intersect and interact each other. Using the method of matched asymptotic expansions, we show how we can construct an explicit approximation of the solution satisfying $\Vert y^{\varepsilon}-\widetilde{P}^\varepsilon\Vert{L^\infty(0,T; L^2(0,1))}=(\varepsilon^{3/2})\Vert y^{\varepsilon}-\widetilde{P}^\varepsilon\Vert_{L^2(0,T; H^1(0,1))}=(\varepsilon)\varepsilon$ small enough.

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