Semilinear elliptic problems involving a parameter

dc.contributor.authorYasmin, Lubana
dc.contributor.examiningcommitteeLui, Shaun (Mathematics) Slevinsky, Richard (Mathematics)en_US
dc.contributor.supervisorCowan,Craig (Mathematics)en_US
dc.date.accessioned2020-09-09T00:18:10Z
dc.date.available2020-09-09T00:18:10Z
dc.date.copyright2020-08-22
dc.date.issued2020-06-29en_US
dc.date.submitted2020-08-22T05:15:39Zen_US
dc.degree.disciplineMathematicsen_US
dc.degree.levelMaster of Science (M.Sc.)en_US
dc.description.abstractWe consider \begin{equation}\label{hum} \left\{ \begin{array}{rrl} -Δ u &=& λ f(u) \quad \mbox{ in } Ω \\ u&=& 0 \qquad \mbox{ on } ∂Ω, \end{array} \right. \end{equation} in a bounded domain $Ω⊂ \IR^N$. The nonlinear term $f$ is smooth, positive, increasing, convex, superlinear at ∞, and $λ>0$ a parameter. We also consider (\ref{hum}) in case of nonlinearity $\frac{1}{(1-u)^2}$ (MEMS nonlinearity), and with a divergence free advection term, a(x) ($-Δ u+a(x)⋅ ∇ u=λ f(u)$ in $Ω$ and $u=0$ on $∂Ω$). In this thesis, we are interested in talking about the existence of stable minimal solutions to these partial differential equations (pde's). We show, when $λ<λ^*$ (a critical parameter), there is a minimal stable solution and when $λ>λ^*$, there exists no solution. Here, stability of solution means nonnegativeness of the first eigenvalue of the linearized operator associated with the pde. This nonnegative inequality can also be viewed as the second variation of energy functional associated with the pde at $u$. At $λ^*$, we obtain a unique weak solution which is the limit of minimal solutions ($\lim_{λ↗ λ^*} u_λ↗ u^*$), we call it extremal solution. Properties of extremal solution depend strongly on $Ω, f, N$. For (\ref{hum}), the extremal solution is smooth in $N≤ 9$ with $f(u)=e^u$ while it is singular for $N≥10$, $Ω=B_1$. The best result is by Nedev, which says $u^*$ is bounded for any $f$ and $Ω$ when $N≤ 3$. We discuss the radial case which shows the optimal regularity result for $u^*$ in $N≤ 9$. For the MEMS model, all stable solutions are smooth iff the dimension is $N≤ 7$. For the pde with advection, there is no suitable variational characterization for the stability assumption. To overcome this difficulty, we use a general version of Hardy's inequality to show smoothness of extremal solution in dimension $N≤ 9$ with exponential nonlinearity.en_US
dc.description.noteOctober 2020en_US
dc.identifier.urihttp://hdl.handle.net/1993/35007
dc.language.isoengen_US
dc.rightsopen accessen_US
dc.subjectSemilinear elliptic partial differential equationen_US
dc.subjectSobolev spaceen_US
dc.subjectRegularityen_US
dc.subjectExtremal solutionen_US
dc.subjectGelfand problemen_US
dc.subjectMEMS modelen_US
dc.subjectRadial solutionen_US
dc.subjectLinearized operatoren_US
dc.titleSemilinear elliptic problems involving a parameteren_US
dc.typemaster thesisen_US
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