Ordinary Differential Equations

Schedule

Lectures. Wednesday 4-6 pm; Thursday 2-3 pm. To be delivered online. Link will be sent through moodle or posted on this page!

Recitation instructor: Emanuel Sygal

Recitations. Thursday 3-4 pm and 6-7 pm.
Emanuel's office hours. Sunday 12-1 pm.

Course grader: Ariel Rom

About this course

Topics include: Existence and uniqueness of ODEs. Exponentiating matrices and linear ODEs. Bases of solutions and Wronskians. Method of variation of parameters. Power series expansions. Qualitative theory of non-linear systems. Boundary value problems. Sturm-Liouville theory.

Prerequisites

I expect familiarity with linear algebra and multi-variable calculus (chain rule, equality of mixed partials).

References

There are many books on differential equations. The two books that I found most helpful are:

Differential Equations, Dynamical Systems, and an Introduction to Chaos by Morris W. Hirsch, Stepen Smale, Robert L. Devaney

Ordinary Differential Equations by Garrett Birkhoff and Gian-Carlo Rota

At times, I will follow the beautiful notes by Shiri Artstein (in Hebrew).

Homework

Assignment 1
Assignment 2
Assignment 3
Assignment 4
Assignment 5
Assignment 6
Assignment 7
Assignment 8
Assignment 9
Assignment 10
Assignment 11
Practice Slides
Practice Exam

Marking scheme

It is university policy that homework is to be submitted as if it were a regular semester. You can submit it via Moodle to Ariel Rom. I am told that there are many apps that allow you to make quality scans on a modern smartphone. If you don't have a modern smartphone, you can latex your solutions.


Week 1 in review

This week we discussed we studied several simple differential equations: y' = y, y' = \sqrt{y}, y' = y^2, y' = y(L-y). We noticed that in the first, third and fourth examples, the integral curves (solutions of the equation) foliate the plane, that is, through every single point in the plane, passes a unique integral curve. In particular, no two integral curves intersect. This is a consequence of the Picard-Lindelof theorem (the existence and uniqueness theorem for first-order ODEs) -- it is enough that the function f in y' = f(x,y) is C^1. We will prove this theorem in a week or two. We also saw that this property fails in the second example.

We discussed the concept on an equilibrium point (where y' = 0) and saw some examples of stable and unstable equilibrium points.

We also discussed two second order systems: the harmonic oscillator x'' = -x and x'' = -sin x. The idea was to convert them into first-order systems by introducing a dummy variable y = x'. In both examples, we defined an energy function E(x,y) and proved that the energy is conserved under the dynamics, so that (x,y) travels along the level sets of E.

Finally, we discussed the inhomogeneous problem y' = y + f(x) and saw that it could be solved by the method of variation of parameters: one examines the homogenous equation y' = y, which has the solution Ce^x and made the constant a function of x: C(x)e^x. Notes



Week 2 in review

This week, we have discussed the theorems of Peano and Picard-Lindelof concerning the existence and uniqueness of ODEs. I expect that you understand the statements of the theorems and have some idea how the proofs work, but if you don't follow the proofs 100%, it is perfectly fine, since we will not need the ``details of the proofs'' in this course. I apologize if the lectures were somewhat technical. Notes 2 (updated)

Slides (Wed) Slides (Th)


Week 3 in review

This week, we discussed the principle of continuation of solutions, the concept of maximal/minimal solutions (when one does not have uniqueness) and Osgood's uniqueness criterion (generalizing Picard-Lindelof). We also discussed exponentiation of matrices. Notes 3 (draft)


Week 4-5 plans

Notes (updated) and Slides


Week 6 plans

This week we will discuss the concept of distributions or generalized functions and what it means for a differential equation to hold in the sense of distributions. For the purposes of this course, the only non-trivial distribution is the Dirac delta mass and one only needs to know that the presence of the delta mass indicates a jump discontinuity. The notions of Greens functions and delta masses will not appear on the exam, but may appear on the homework. Notes (draft)


Further notes

Notes on higher-order equations

Laplace Transform and Slides

Notes on Power Series Solutions (not on the exam)

Fourier Series and the Heat Equation

Wave Equation, Sturm-Liouville Theorem

Exact Equations, Kepler's Laws