Differential-Equations ยท Unit 1 ยท Video 3 ยท Interactive Practice
| Formula | Name | What you need |
|---|---|---|
| Isocline of slope โ a ray through the origin | A slope value ; the unsolved form reaches | |
| Isocline slope times element slope | Negative reciprocals, so the two are perpendicular | |
| Integral curves, by separation | Integrate both sides; because the left side is | |
| Explicit solution and its domain | One point on the curve, to fix |
Key Insight: Because every isocline carries elements perpendicular to itself, an integral curve must cross every ray through the origin at a right angle โ and only circles centred at the origin do that. The circles arrive before any integration; the domain arrives only after it.
The isocline of slope is the ray , and the two slopes multiply to .
๐ก The solved form can never produce โ it divides by it. Written unsolved as , the value gives : the -axis is a genuine isocline, carrying horizontal elements.
A curve that follows the elements crosses every ray through the origin at a right angle.
Separation confirms the circles, then hands you a domain the equation itself never mentions.
1 ยท separate the variables
๐ก Here the domain can be read off the explicit solution. For most equations it cannot: how far a solution extends is discovered by computing it, never by inspecting the equation.
Problem 1 ยท Finding an Isocline
Given: โ find the isocline along which every line element has slope .
An isocline is the set of points where the equation prescribes one fixed slope, so set the right-hand side equal to that slope and solve for :
Check a point. lies on this line, and there .
Check the geometry. The isocline's own slope is and the elements it carries have slope ; the product is , which is the general fact for this equation.
Problem 2 ยท The Isocline's Slope Is Not the Slope It Carries
Given: the line is an isocline of โ find the constant slope carried by the line elements along it.
Directly. Every point of has the form with , so the equation gives
The same value at every point โ which is what makes the line an isocline.
From the general form. The isocline of slope is , so its own slope is . Here that must equal :
And , so the elements meet this isocline at a right angle, exactly as they do on every other one.
Problem 3 ยท The Solution Through a Point, and How Far It Goes
Given: the solution of passing through โ find it explicitly, and find its domain.
Which explicit solution?
What is its domain?
Step 1 โ separate and integrate.
Step 2 โ fix the constant with the point. Substituting :
Step 3 โ pick the branch. The point has , so the solution is the upper semicircle:
Step 4 โ the domain. The square root requires , that is :
The interval is open at both ends. At the solution would have , where is undefined and the circle is vertical, so the solution cannot be extended past those points. Verify the equation itself:
The equation is identical for every solution of this family; only the constant โ supplied by the point, not by the equation โ decides how wide the interval is.
Problem 4 ยท When the Isoclines Are Not Perpendicular
Given: a different equation, , whose isocline of slope is the line โ find the product of the isocline's slope with the slope it carries, and find the integral curves.
Isocline slope ร element slope
So the integral curves are
The two slopes. The line has slope . At any point on it the equation gives
so the elements have slope as well and the product is . Since , it is never : these isoclines are never perpendicular to their elements. They are parallel to them.
What that forces. An integral curve follows the elements. If the elements along a line point straight down that line, the line already follows them, so each isocline is an integral curve. Separating confirms it:
The contrast. For the slopes multiply to : elements perpendicular to the rays, integral curves circular. For they multiply to : elements along the rays, integral curves the rays. In both cases the isocline geometry alone settles the answer โ and in both cases the -axis or -axis has to be excluded where the right-hand side blows up.
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