The Behavior of the Free Boundary for Reaction-Diffusion Equations with Convection in an Exterior Domain with Neumann or Dirichlet Boundary Condition
Abstract
Let equation* L=Σi,j=1dai,j∂2∂ xi∂ xj-Σi=1dbi∂∂ xi equation* be a second order elliptic operator and consider the reaction-diffusion equation with Neumann boundary condition, equation* aligned &Lu= up\ in\ Rd-D;\\ &∇ u· n=-h\ on\ ∂ D;\\ &u0 \ is minimal, aligned equation* where p∈(0,1), d2, h and are continuous positive functions, D⊂ Rd is bounded, and n is the unit inward normal to the domain Rd- D. Consider also the same equations with the Neumann boundary condition replaced by the Dirichlet boundary condition; namely, u=h on ∂ D. The solutions to the above equations may possess a free boundary. When D=\|x|<R\ and L and are radially symmetric, we write the solution as u(r) with r=|x| and define the radius of the free boundary by r*(h)=∈f\r>R:u(r)=0\. We normalize the diffusion coefficient to be on unit order, consider the convection vector field to be on order rm, m∈ R, pointing either inward (-) or outward (+), and consider the reaction coefficient to be on order r-j, j∈ R. For both the Neumann boundary case and the Dirichlet boundary case, we show for which choices of m, () and j a free boundary exists, and when it exists, we obtain its growth rate in h as a function of m, () and j. These results are then used to study the free boundary in the non-radially symmetric case.
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