Start with y′ = y·(1 − y). The right side is a product, and a product is zero when either factor is. So the slope is 0 exactly where y = 0 or y = 1, at every t: both lines are horizontal solutions, and the lab lists them in the tile named Horizontal solutions.
Between the lines and outside them the sign of the slope is fixed. For y between 0 and 1 both factors y and 1 − y are positive, so the slope is positive and the segments rise. For y above 1 the factor 1 − y is negative and the slope is negative. For y below 0 the factor y is negative and 1 − y is positive, so the slope is negative again.
y′ = y·(1 − y)
range of y sign of y sign of 1 − y slope
y < 0 − + falling
y = 0 0 + 0
0 < y < 1 + + rising
y = 1 + 0 0
y > 1 + − falling
Why curves do not cross, and what that gives
A solution that starts at y = 1/2 rises, because the slope there is positive. Could it reach y = 1? Not by crossing at an angle: the field gives one slope at each point, and two curves through one point with two slopes cannot both be solutions. But a curve that reached y = 1 would arrive flat, since the slope there is 0 by the equation, and the one-slope argument has nothing to say against that. What rules it out is the uniqueness claim: through a given point there is exactly one solution, and the horizontal line is already it. For a polynomial right side the claim holds, and with it a solution that starts below 1 stays below it for ever, and the same argument keeps it above 0.
Theorem · The no-crossing claimTwo different solutions of y′ = f(t, y) never cross at an angle, because they would need two slopes at one point. For the equations of this course they never touch either: through each point there is exactly one solution, which is the uniqueness statement of “Blow-Up and the Interval of Existence”.
The first sentence is settled by the arithmetic of the slope, and the lab demonstrates it. The second is a claim this course states, uses and does not prove; it is what makes a horizontal solution a wall and not merely a line of flat segments. For the rest of this course, take both as the working rule.
A field where the curve approaches a line
In the second preset the equation is y′ = t − y and the drawn solution starts at (0, 2). The line y = t − 1 is itself a solution: its derivative is 1, and t − (t − 1) = 1, so the residual is zero, by the test of “What a Differential Equation Is”. The drawn curve bends towards that line. That is what the picture suggests; First-Order Linear Equations is where the claim is established.
Example · A curve that leaves the windowTake y′ = y² with the solution through (0, 1), and look at the third preset. The drawn curve climbs, steeper and steeper, and leaves the window before t = 1.
What the field supports: the slope y² is never negative, so the curve never falls, and it grows steeper as y grows. What it does not settle is whether the curve is merely large at the window's edge or has stopped existing there. “Blow-Up and the Interval of Existence” answers that.
Hold that distinction in the examples that follow. The arithmetic of the slope settles the horizontal solutions, the sign on each side and the no-crossing rule. The look of the picture suggests the far future, and the drawn curve is a floating-point drawing that says so in the legend.