Autonomous Differential Equations
Differential equations of the form
are called autonomous.
or an autonomous equation, the solutions y(t) = yi, where yi’s are the
roots of f (t), are called equilibrium.
- If an equilibrium repels neighboring solutions as t → ∞ then it is called a source, repeller, or unstable equilibrium,
- If an equilibrium attracts neighboring solutions as t → ∞ then it is called a sink, attractor, or stable equilibrium,
- If an equilibrium is neither a source nor a sink, then it is called a node, or semi-stable.
Equilibrium solution
Occurs at the points where
Equilibrium solutions:
when
is a source/repeller/unstable
when
is a node/semi-stable
when
is a sink/attractor/stable
when
when
when
when
when
when
when
when
when
Chapter 2: First-Order ODEs
Three main types of First-Order Equations
Separable ODE
Linear (1st order) ODE
Exact ODE
where
Separable ODEs
Assume that
is inseparable, so this is NOT a separable ODE
Solving Separable ODEs
“Separate then integrate”
- Convert the given equation into the form
- Integrate both sides
to obtain . This gives the implicit solution to the given equation. (General solution in implicit form) - Convert the solution obtained in step 2 to explicit form and use the initial condition to solve for the constant C, if required/able.
Solve the following IVP:
- Separate
- Integrate
- Use initial condition
to solve for C:
Thus, the particular soln in implicit form is
To convert this into explicit form:
There can only be 0, 1, or infinitely many solutions. Not 2, so we have to figure out if we are using the + or - sign.
Under the inital condition when, which is if the sign is +, or if the sign is -
So the correct sign is -
is the particular solution in explicit form.
- Separate
- Integrate