Equilibrium solutions mark the places where a system comes to rest. But not all equilibrium solutions are alike; some attract nearby solutions, others repel them, and some do a bit of both. In this section, weβll learn how to classify these points by examining the slope field, the sign of \(f(y)\text{,}\) and a tool called a phase line.
Suppose \(y = c\) is an equilibrium solution of an autonomous equation\(y' = f(y)\text{.}\) If you nudge a solution slightly above or below \(c\text{,}\) it might drift back, move away, or react differently on each side. What it does determines the type of equilibrium it is.
In a slope field, a sink looks like segments converging toward a horizontal line, a source shows segments diverging away, and a semi-stable equilibrium is a mix: converging on one side, diverging on the other. Next, weβll look at different ways to determine these behaviors.
Slope fields convey a great deal of information at once, but for autonomous equations, we can simplify them. Since the slope depends only on \(y\text{,}\) we can βcompressβ the slope field into a simple vertical diagram of just \(y\)-values. This is called a phase line.
The arrows summarize how \(y(t)\) changes: whether solutions are rising or falling. Follow the arrows up or down, and youβll see where solutions eventually settleβor whether theyβre pushed away.
A single vertical y-axis marks equilibria at y = -1 and y = 1 as solid dots. Flow arrows point up between the two equilibria and down above y = 1 and below y = -1, so solutions converge on y = 1 (a sink) and diverge from y = -1 (a source).
Three solid dots sit on a vertical line. Arrows point toward the top dot from both sides (a sink), away from the middle dot on both sides (a source), and toward the bottom dot from above but away below (semi-stable). No numeric labels are shown; the points are referred to as A, B, and C in the exercise.
The important observation is that \(f(y)\) increases through sources and decreases through sinks. This is true in general, so we can classify equilibrium solutions by looking at the sign of \(f'(y)\) at the equilibrium points.
A two-panel perspective figure. The vertical panel is the slope field for y-prime equals 1 minus y squared, with the equilibrium at y = 1 labeled a sink and y = -1 labeled a source. The horizontal panel plots f of y equals 1 minus y squared as a downward-opening parabola, drawn solid where f is positive and dashed where negative, showing f increasing through the source and decreasing through the sink.