Week 4 Flashcards
2 goal equations of electrostatics
Harmonic functions
Solutions to laplaces equation
(Not only examples)
form integral form of Gauss’s law for a region of zero net charge in terms of φ
where we use E = grad*phi
Greene’s second identity
Apply greens second identity and laplaces equation to a region V which is a ball radius R and for f = 1/r g = φ
Key insight of harmonic functions
They are averaging functions and have no local extrema across V. Any extrema must occur at boundary of V
If φ satisfies Laplace’s equation in a region V and in addition is constant on boundary of V then φ must be equal to the same value across the entire region as the boundary
Dirichlet boundary conditions
Values of a function itself on a boundary (for PDE)
Neumann boundary conditions
Values of normal derivative of function along a boundary (for PDE)
Showing uniqueness of solution to Laplace’s equation in some volume V
1) let there be 2 solutions
2) construct a difference solution
3) on boundary all solutions must be equal
4) therefore both solutions equal
If Φ is specified on the boundary of V, S
Then below:
Integration by parts
Taking inner product for sin(nx)
Requirements for stable equilibrium
- force in a positive test charge Q is zero at the equilibrium point r0 (E(r0) = 0)
- when displaced from the equilibrium point forces act so as to return the test charge Q to r0
(Field lines all point towards r0)
For a charge q located at the origin ρ(r) = ?
q * δ3(r) which of course spikes at origin
In spherical coordinates, how to ‘remove’ laplacians from equation
Also grad(1/r) = 1/r * er
Relate Laplace’s equation to Poisson’s
Laplace’s equation is a special cause of Poisson’s used in regions where ρ = 0