We use to represent the time derivative of that is,
We can interpret a @differential-equation of this form as a as a vector field. tells us in which direction and at what magnitude we move at any point on the real line (where is defined.) We can do this by plotting vs
You can see that when is to the right of the flow is to the right, and when is to the left of 0 the flow is to the left.
At some points, there is no flow.
A point at which the change in position of a system is is called a fixed point. We denote a fixed point at as
Referenced by (23 direct, 2 transitive)
Direct references:
- Introductory PDE Stuff
- Bifurcations
- Transcritical
- intuition-6
- intuition-7
- Discrete Time Dynamical Systems
- Flows on the Line
- Stable
- Unstable
- Globally stable
- linear-stability-analysis
- Half-stable
- Limit Cycles
- proof-of-conservative-systems-have-no-attracting-fixed-points
- Homoclinic orbit
- Liapunov Function
- theorem-17
- Planar Bifurcations
- Planar Systems
- Homoclinic Orbit
- Heteroclinc Trajectory
- Hyperbolic Fixed Point
- Weakly Nonlinear Oscillators
Transitive (depth 1):
A fixed point where nearby points flow towards it is said to be stable.
Referenced by (5 direct)
A fixed point where nearby points flow away from it is said to be unstable.
Referenced by (4 direct)
The convention, when drawing a dynamical system as a vector field is to draw filled in circles for stable fixed points and empty circles for unstable fixed points.
The starting point, where we place a particle is called a phase point.
Referenced by (1 direct, 9 transitive)
Direct references:
Transitive (depth 1):
Transitive (depth 2):
Transitive (depth 3):
The function describing the path taken by a particle starting at a phase point is called a trajectory and represents a solution to a @differential-equation with @initial-conditions
Referenced by (5 direct, 5 transitive)
Direct references:
Transitive (depth 1):
Transitive (depth 2):
A drawing that shows the different trajectories taken from different phase points in a system is called a phase portrait.
We can also visualize trajectories by plotting vs
Here's both views together.
A fixed point that is approached from any starting position on the real line (other than that at itself) is said to be globally stable.
Application: Population Growth
A very simple model of population growth is just exponential growth. You can model this as
where You can see by modeling this on the demo's above that population just goes to infinity with this. This is not realistic. A better model assumes there is a certain carrying capacity , where if the population exceeds , growth actually becomes negative. This is modeled using the logistic equation
Linear Stability Analysis
While it's nice to have a visual intuition for whether a fixed point is stable or not, sometimes it's also nice to know analytically.
Let be a fixed point of Then, if if is negative, then is a stable fixed point . If is positive, then is an unstable fixed point.
This comes from letting be a small perturbation away from differentiating it, writing its taylor series, then noticing that and terms greater than the linear term matter less than the linear term and writing
This is called the linearization about
It also only works if If that's not the case, the best bet is to fall back to graphical analysis or to solve explicitly if possible.
A fixed point where and the stability depends on which side of lies on is called half-stable. It is denoted with a half-filled circle.
Referenced by (1 direct)
Direct references:
Existence and Uniqueness
Consider the @initial-value-problem
Suppose that and are continuous on an open interval of the -axis, and suppose that is a point in Then, the initial value problem has a solution on some time interval about and the solution is unique.