Integral Representations for Harmonic Problems
- Some Wave Equations
- Introduction
- Physical Background
- The acoustic equation
- The Maxwell equations**
- Elastic waves
- The Helmholtz Equation
- Introduction
- Harmonic Solutions
- Fundamental Solutions
- The Case of the Sphere in R3 **
- Spherical harmonics
- Legendre polynomials
- Associated Legendre functions
- Vectorial spherical harmonics
- The Laplace Equation in R3
- The sphere
- Surfaces and Sobolev spaces
- Interior problems: Variational formulations
- Exterior problems
- Regularity properties of solutions in lRn
- Elementary differential geometry
- Regularity properties
- The Helmholtz Equation in 1R3
- The spherical Bessel functions
- Dirichlet and Neumann problems for a sphere
- The capacity operator T
- The case of a plane wave
- The exterior problem for the Helmholtz equation
- Integral Representations and Integral Equations
- Integral Representations
- Integral Equations for Helmholtz Problems
- Equations for the single layer potential .
- Equations for the double layer potential
- The spherical case
- The far field
- The physical optics approximation for the sphere
- Integral Equations for the Laplace Problem
- Variational Formulations for the Helmholtz Problems
- The operator S
- Fredholm operators
- The operator N
- Formulation with the far field
- Singular Integral Operators
- Maxwell Equations and Electromagnetic Waves
- Introduction
- Fundamental Solution and Radiation Conditions.
- Multipole Solutions
- Multipoles
- The capacity operator
- Exterior Problems
- Trace and lifting associated with the space H(curl) .. .
- Variational formulations for the perfect conductor problem
- Coupled variational formulations for impedance conditions
- Integral Representations
- Integral Equations
- The perfect conductor .
- The zero frequency limit
- The dielectric case
- The infinite conductivity limit: The perfect conductor
- The Far Field
- Far field and scattering amplitude.
- Integral equations and far field