Homework 10

  1. Warming up

a.- Solve

Δu=f, \Delta u = f,

in a rectangle of sides (L1,L2)(L_1,L_2), with the following boundary conditions and sources:

  1. Homogeneous Dirichlet boundary conditions and ff arbitrary in L2L^2.

  2. Homogeneous Neumann boundary conditions and ff arbitrary in L2L^2. What further condition is need to assert a solution exists?

  3. Mixed boundary conditions, look at what means a Robin boundary condition.

b.- From the structure of the solutions check that if fHsf \in H^s then uHs+2u \in H^{s+2}.

c.- Solve for inhomogeneous Dirichlet boundary conditions. Assume you can decompose the boundary data into the boundaries values for the eigenfunctions of the Laplacian at the rectangle. What can you conclude about the smoothness of the solution in the interior?

  1. Clasification

Exercise 1.1 Classify the following PDEs as elliptic, parabolic, or hyperbolic:

  1. Δu+u=0\Delta u + u = 0 (Helmholtz equation)

  2. uxx+2uxy+uyy=0u_{xx} + 2u_{xy} + u_{yy} = 0

  3. uxxuyy+2ux=0u_{xx} - u_{yy} + 2u_x = 0

  4. div(a(x)u)=f(x)\text{div}(a(x)\nabla u) = f(x), where a(x)>0a(x) > 0.

Exercise 1.2 Show that the PDE uxx+cos(x)uxy+sin(x)uyy=0u_{xx} + \cos(x) u_{xy} + \sin(x) u_{yy} = 0 is elliptic in a region of R2\mathbb{R}^2. Find this region.

  1. Maximum Principles

Exercise 3.1 Prove the weak maximum principle for Δu=0\Delta u = 0 in a bounded domain ΩRn\Omega \subset \mathbb{R}^n: If uC2(Ω)C(Ω)u \in C^2(\Omega) \cap C(\overline{\Omega}), then

maxΩu=maxΩu. \max_{\overline{\Omega}} u = \max_{\partial \Omega} u.

Exercise 3.2 Let uu satisfy Δu0\Delta u \geq 0 in Ω\Omega. Show that if uu attains a maximum at an interior point, then uu is constant.

Exercise 3.3 For Δu+c(x)u=0\Delta u + c(x)u = 0 with c(x)0c(x) \leq 0, prove that if uu attains a non-negative maximum inside Ω\Omega, then uu is constant.

  1. Existence and Uniqueness

Exercise 4.1 Use Lax-Milgram to show that the Dirichlet problem

Δu+u=f in Ω,u=0 on Ω -\Delta u + u = f \text{ in } \Omega, \quad u = 0 \text{ on } \partial \Omega

has a unique weak solution in H01(Ω)H^1_0(\Omega) for fL2(Ω)f \in L^2(\Omega).

Exercise 4.2 For the Neumann problem Δu=f-\Delta u = f with un=g\frac{\partial u}{\partial n} = g: (a) Find a necessary condition on f,gf,g for solvability. (b) Show solutions are unique up to additive constants.

  1. Variational Methods

Exercise 5.1 Show that minimizers of

J(u)=Ω(12u2fu)dx J(u) = \int_\Omega \left( \frac{1}{2} |\nabla u|^2 - fu \right) dx

over H01(Ω)H^1_0(\Omega) solve Δu=f-\Delta u = f.

Exercise 5.2 Prove the first Dirichlet eigenvalue λ1\lambda_1 of Δ-\Delta satisfies:

λ1=minuH01(Ω)u0Ωu2dxΩu2dx. \lambda_1 = \min_{\substack{u \in H^1_0(\Omega) \\ u \neq 0}} \frac{\int_\Omega |\nabla u|^2 dx}{\int_\Omega u^2 dx}.

  1. Nonlinear Elliptic Equations

Exercise 7.1 Show that a weak solution exists for

Δu+u3=f in Ω,u=0 on Ω, -\Delta u + u^3 = f \text{ in } \Omega, \quad u = 0 \text{ on } \partial \Omega,

when fL2(Ω)f \in L^2(\Omega).

Exercise 7.2 Prove that for Δu=eu-\Delta u = e^u in ΩRn\Omega \subset \mathbb{R}^n bounded,

supΩusupΩu+C(Ω). \sup_\Omega u \leq \sup_{\partial \Omega} u + C(\Omega).
Last modified: June 14, 2025.
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