Most real systems are nonlinear: $x' = f(x, y)$, $y' = g(x, y)$. We cannot usually solve them, but near an equilibrium they behave like a linear system, and phase portraits tell us what that linear system does. The tool is the Jacobian matrix of partial derivatives.
🔑 Key idea
At an equilibrium $(x^{*}, y^{*})$ (where $f = g = 0$), the linearization is $\mathbf{u}' = J\mathbf{u}$ with $$J = \begin{bmatrix} f_x & f_y \\ g_x & g_y \end{bmatrix}_{(x^{*}, y^{*})}.$$ If $J$ gives a saddle, node or spiral, the nonlinear system has the same type near the equilibrium. If $J$ gives a center, the test is inconclusive.
💡 Why it works
Let $u = x - x^{*}$, $v = y - y^{*}$. The tangent plane approximation gives $f(x, y) \approx f(x^{*}, y^{*}) + f_xu + f_yv$ $= f_xu + f_yv$, since $f = 0$ at the equilibrium; similarly for $g$. So $(u, v)' \approx J(u, v)$, with errors of second order in the small displacements. When the eigenvalues have nonzero real parts, those small errors cannot change the qualitative picture (the Hartman–Grobman theorem). For a center, the real part is 0, and the tiny nonlinear terms can tip the orbits into spirals either way.
✏️ Worked example: Find the equilibria
Find the equilibria of $x' = x - y$, $y' = x^{2} - 4$.
Answer: a saddle: coexistence is unstable, and one species eventually wins
⚠️ Common mistake
Evaluating the Jacobian at the origin, or forgetting to plug in the equilibrium at all, and classifying a matrix that still contains $x$ and $y$. Each equilibrium has its own Jacobian. And a center of the linearization does not prove the nonlinear system has closed orbits.
The nonlinear system $x' = x - y$, $y' = x^{2} - 4$. Near $(2, 2)$ trajectories spiral outward; near $(-2, -2)$ they come in along one direction and leave along another, just as the two Jacobians predict.
Practice
Pass with 3 right answers, the last 2 in a row. Each right answer earns 3 XP.