1.3 & 1.4 Flashcards
Bernoulli Equation has the form:
x’ + p(t)x = q(t) * x^b
How do you solve Bernoulli Equation (i.e. x’ + p(t)x = q(t) * x^b)?
It is linear in the variable y = x^ 1-b
1. Take derivative of that to get dy/dt = (1-b) * x^-b * dx/dt
2. Sub in dx/dt from the initial question
3. When possible, substitute y in for any x^1-b
4. Then you have a linear ODE, so solve using integrating factor method
An autonomous equation is one which:
does not depend on t, so that x’ = f(x).
An equilibrium point is an x* such that given x’ = f(x)
f(x*) = 0
Thm: Assume x* is an equilibrium and x(t) is any solution of the equation. If x( t* ) = x* for any t*, then:
x(t) = x* for all t. AKA, you cannot cross an equilibrium point.
Suppose x(t) is a solution and x* is an equilibrium point. If x(t) > x* for any t, then:
x(t) > x* for all t. AKA, if you’re above an equilibrium point, you cannot touch it or cross it.
Suppose x(t) is a solution which is not a constant. Then:
then x(t) is either strictly increasing or strictly decreasing
Suppose x(t) is a solution to x’ = f(x) and x(t.0) = x.0. Then one of the following is true as t gets large
- x(t) is unbounded for t > t.0
- x(t) exists for all t > t.0 and lim( x(t) ) = x* for some equilibrium point
How to tell if x* equilibrium point is stable or unstable given x’ = f(x)
if f ‘ (x) < 0, stable
if f ‘ (x) > 0, unstable
How to find the linearized version of a solution around a equilibrium point x* = x* given x’ = f(x)
x’ = f ‘ (x* ) * (x - x*)
such that x(0) = x.0
so also solve for x.0
Phase diagram equivalence
When 2 phase diagrams have the same number and arrows all point in the same direction, doesn’t matter what the points are exactly
A bifurcation point is when:
The point p in the parameters when the phase diagram changes (not equivalent). AKA, the phase diagram is unstable at point p because it looks different in the immediate area around it.
A bifurcation diagram is a plot of
a plot of equilibrium points as a function of the parameters
How to draw a bifurcation diagram.
- Solve for x* in terms of p, then see how p affects the x* in each case
- Plug in each x* into f ‘ (x) to find stability of each line
Saddle node bifurcation
No x* on one side, and has one x* at bifurcation point, then splits into 2 x*, one stable and one unstable