Postgraduate Science

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Ordinary Differential Equations

First-order, linear systems, and qualitative behavior in phase space.

An ODE relates a function and its derivatives. First-order:

$$\frac{dy}{dx} = f(x, y).$$

Existence and uniqueness (Picard–Lindelöf) hold when $f$ is Lipschitz in $y$. Linear first-order $y' + P(x) y = Q(x)$ solved by integrating factor $e^{\int P}$.

For second-order linear with constant coefficients $ay'' + by' + cy = 0$, the characteristic polynomial $ar^2 + br + c = 0$ has roots $r_{1,2}$, giving solutions $e^{r_1 x}, e^{r_2 x}$ (real distinct), or oscillating exponentials (complex roots).

For autonomous 2D systems $\dot{\mathbf x} = A\mathbf x$, the eigenvalues of $A$ classify the origin: real same sign → node, opposite signs → saddle, complex with real part → spiral, pure imaginary → center.

Interactive: direction field

Quiz

1. Picard–Lindelöf guarantees existence/uniqueness when $f(x,y)$ is:
2. For $\dot{\mathbf x} = A\mathbf x$ with $A$ having pure imaginary eigenvalues, the origin is a:
3. $y' + P(x) y = Q(x)$ is solved by:
4. Two solutions $y_1, y_2$ of a linear 2nd-order ODE are linearly independent iff:
5. The Frobenius method gives series solutions around: