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Syllabus:
Differential Equations&Mathematica
Authors: Bill Davis and Jerry Uhl ©1999
Producer: Bruce Carpenter
Publisher:
Distributor: ![]()
These lessons are used in Math 385, 286 and 351.
![[Graphics:Images/285syl_gr_4.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_4.gif)
![[Graphics:Images/285syl_gr_5.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_5.gif)
How to write down formulas for solutions of
.
How to use integrating factors to get formulas for solutions of
.
If
, then all solutions of
go into the same steady state.
Exponential models.
The jump function
and the impulse function ![]()
Impulse forcing the exponential diffeq with a Dirac Delta function; The physical meaning of the impulse force.
The superpositio n principle.
![[Graphics:Images/285syl_gr_13.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_13.gif)
The undamped unforced oscillator
< br>The damped unforced oscillator
The damped forced oscillator
< br>Steady state and transients for forced damped oscillators
Resonance and beating
Euler Identity
The characteristic equation
Using convolution i ntegrals to try to get formulas solutions of the forced
oscillator diffeq
Resonance
Forcing an oscillator with a Dirac Delt a function;
the physical meaning of the impulse hit
Amplitude and frequency of unforced oscillators
Underdamped,critically damped,and overdamped oscillatorsBoundary value problems
![[Graphics:Images/285syl_gr_17.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_17.gif)
The Laplace transform of a function ![]()
How to write down the Laplace tranform of the solution of a forced oscillator
diffeq
Solving forced oscillator diffeqs by inverting Laplace tran sforms
Fast Fourier point fit and Fourier integral fit
Combining Fourier fit and the Laplace transform to come up with good
approximate formulas for periodically forced oscillators
Fourier analysis for detecting resonance
![[Graphics:Images/285syl_gr_19.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_19.gif)
Euler's method of faking the plot of the solution of a differential equation
and how it highlights the fundamental issue of diffeq
Reading a diffeq t hrough flow plots
Solving diffeq's numerically with Mathematica
Systems of interacting differential equations: The predator-prey model
Sensitive dep endence on starter data
The drinking versus driving model
Population models and control; Logistic harvesting
Lanchester war model
![[Graphics:Images/285syl_gr_20.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_20.gif)
Reading an autonomous diffeq through phase lines
Automomous diffeqs with parameters. Bifurcations and bifurcation points
Hand symbol manipulation: Separating the variables
Population models and control
Using bifurcation plots to study E. Coli growing in a chemostat
Automatically controlled air conditioning
Getting t here in infinite time versus getting there in finite time
![[Graphics:Images/285syl_gr_21.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_21.gif)
Flows and their trajectories as pairs of solutions of a system of differential equations
Flow analysis of the unforced linear oscillator differential equa tion by converting it to a system of two first order differential equations
Equilibrium points
Damped oscillators, undamped oscillators and van der Pol's nonlinea r oscillator
Linear systems and graphical meaning of eigenvectors of the coefficient matrix
Pursuit models
Boundary value problems: Shooting for a specified outcome
![[Graphics:Images/285syl_gr_22.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_22.gif)
Eigenvectors of the coefficient matrix point in the directions of strongest inward and/or outward flow
Eigenvalues of the coefficient matrix indicate realtive streng hs of inward and/or outward flow
Eigenvalue-trajectory analysis to predict swirl in,swirl out or no swirl at all
Stability and instability
Reservoir Models for drug metabolization
Linear systems in life science, chemistry and electrical engineering
Higher dimensional linear systems
![[Graphics:Images/285syl_gr_28.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_28.gif)
Using the Jacobian to approximate a nonlinear diffeq system by linearizing at equilibrium points
Attractors and repellers:Lyapunov's rules for detecting them via ana lysis of the eigenvalues of the Jacobian
The pendulum oscillator: Damped and undamped
When linearizations can be trusted and when they shouldn't be trusted & nbsp;
Linearization of pendulum oscillators: Using linearzation to estimate the amplitude and frequency of a pendulum oscillator
Energy and the undamped pendulum oscillator
The Van der Pol oscillator
Gradient and Hamiltonian systems
Lorenz's chaotic oscillator
![[Graphics:Images/285syl_gr_29.gif]](http://cm.math.uiuc.edu/385syl_files/285syl_gr_29.gif)
Rigging
on
to get a pure sine fast Fourier fit of
on
Fourier Sine fit for solving the heat equation.
Fourier Sine fit for solving the wave equation.
Solving the heat and the wave equations in the case that initial data are given by a data list.
As the years go by and I look back on my undergraduate experience, I realize more and more that Calculus&Mathemeatica was the most important thing I did at the University of Illinois. It was an excellent experience. Beyond Calculus, I learned computer programming, problem solving, and the value of teamwork. I am still realizing the positive impact it has made on my career ... including being an big asset when applying to MIT! Last, but not least, C&M has created many lasting friendships that I truly value! C&M develops a very unique ability to help students realize their potential by allowing them to create their own experience!
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