I began by describing compound interest, with its difference equation p(t+Delta t)=p(t)+Ip(t)\Delta t. Then I let the compounding period Delta t go to zero, to get the "continuous approximation and the ODE p'(t)=Ip(t). Then I solved dx/dt=ax with careful attention to how the c in x=ce^{at} comes about. I reminded the students that this is a very common equation in nature. I returned to the original problem and inserted an initial value and a value I=.1, and found that after 20 years I have e^2 times as much as I deposited.
I wrote up the general form of a first-order ODE, dy/dx=g(x,y), and gave as examples dx/dt=ax, dy/dx=g(x), dy/dx=y^2/2 (from Wednesday's lecture), dx/dt=x^2-t$, and dy/dx=y^2-x^2-1.
I made the point that in this course we'll study ODEs from three different but mutually reinforcing perspectives:
I proposed to pursue the first approach now. I tried to give meaning to the equation dy/dx=g(x,y): at each point in the plane we are specifying a slope. I sketched the ``direction field'' for dx/dt=x, and then threaded some solutions to see the exponentials appearing. I marked c>0 above the t-axis, c<0 below, and c=0 on it.
Then I proposed to study the Riccati equation dx/dt=x^2=t in the same way. I pointed out that in the earlier case I didn't just plot the slope at random points; rather, I found all the points at which m=0,1,2,-1,-2: the "isoclines." So I did the same here, but it was harder and the solutions weren't so clear. I used this to motivate turning to Matlab.
I fired up Matlab, computed e^2 (using
In the 1:00 class I then returned to the setup box and replaced the
ODE with y'=y^2-x^2-1, plotted some solutions, observed their
behavior, found the separatrices, and discovered the solution y=-x.
This part of the 2:00 class was interrupted by laughter.
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