Lecture Recordings
If the latest recording is not yet here, it almost certainly will be on Blackboard, so if you’re desperate you might want to look there.
Lecture 13
Summary.
Uniquess of wave equation solutions - the proof
The heat equation
The maximum principle
Lecture 12
Summary.
The wave equation on a finite-length string continued
The problem for \(T(t)\)
Finding the Fourier coefficients
Uniquess of wave equation solutions
Lecture 11
Summary.
The wave equation on a finite-length string
Seeking a separable solution
The Sturm-Liouville problem for \(X(x)\)
Seeking non-trivial solutions
Eigenvalues and eigenfunctions
Lecture 10
Summary.
Derivation of Duhamel’s formula (continued)
Example of its application
Solving the inhomogeneous wave equation with inhomogeneous initial conditions
Lecture 09
Summary.
Finalising the solution to the wave equation Cauchy problem on a semi-infinite string
The inhomogeneous wave equation
Starting to derive Duhamel’s formula
Lecture 08
Summary.
Causality (domains of dependence and influence)
The wave equation on a semi-infinite string
Solving this using odd reflection
Lecture 07
Summary.
The wave equation
Derivation of the one-dimensional wave equation’s general solution
The Cauchy problem for the wave equation
Derivation of d’Alembert’s formula (solution to aforementioned Cauchy problem)
Lecture 06
Summary.
Proving the canonical forms theorem
Well-posed problems
Hadamard’s example of an ill-posed problem
Dirichlet and Neumann boundary conditions
Examples of well-posed problems for elliptic, hyperbolic, and parabolic PDEs
Lecture 05
Summary.
Case 3: \(a(x,y) u_x + b(x,y) u_y + c(x,y)u = f(x,y)\) (solution reduces to ODE along characteristic curves). Another example.
Classification of second order linear PDEs: elliptic, hyperbolic, parabolic.
A theorem on canonical forms (proof next time).
Lecture 04
Summary.
Parameterising curves
First order linear PDEs - the method of characteristics
Case 3: \(a(x,y) u_x + b(x,y) u_y + c(x,y)u = f(x,y)\) (solution reduces to ODE along characteristic curves)
Lecture 03
Summary.
Vector calculus refresher
First order linear PDEs - the method of characteristics
Case 1: \(a u_x + b u_y = 0\) (solution is constant along characteristic lines)
Case 2: \(a(x,y) u_x + b(x,y) u_y = 0\) (solution is constant along characteristic curves)
Lecture 02
Summary.
Linearity
Order
Homogeneous and inhomogeneous
The Superposition Principle
Some simple PDEs: ODEs dressed up as PDEs
Directional derivative
Lecture 01
Summary.
How the module works
Why study PDEs?
Notation
Introducing classification: linearity