At every point of the ray with , the equation gives the same slope , because the slope depends only on the ratio . Such an equation is usually not separable as written, but taking the ratio as the new unknown makes it separable. This lesson explains the scaling property behind the method, the substitution and its derivative, and the line solutions and half-planes that have to be checked separately.
Key terms
Homogeneous first-order equation
Definition Let be the independent variable, with . A first-order equation is homogeneous, in the sense used for this method, if on the half-plane , or on the half-plane , it can be written as
for a function of one variable. The same structure comes from a differential form whose coefficients are homogeneous functions of the same degree , meaning
for every . Where and , the choice gives , and on the choice works the same way. This use of the word is different from a homogeneous linear equation, which means an equation with zero forcing, and a homogeneous equation in the present sense is often nonlinear.
In plain words The slope at a point depends on the direction of the point from the origin, not on its distance. Here homogeneous describes how the equation behaves under scaling, not whether it has a forcing term.
Example The equation
has coefficients that are homogeneous of degree . Where it reads , and dividing the numerator and the denominator by gives
By contrast, the linear equation is homogeneous in the linear sense, since it has no forcing term, but not in this sense. Along the ray its slope is at and at .
Scale invariance
Definition A slope function is scale invariant on the half-plane if
for every and every point with . This holds exactly when there, with , since the choice gives . The same definition applies on . For an equation the scaling sends solutions to solutions. If is a solution on an interval of positive , then for every so is
because .
In plain words Stretch the plane away from the origin by any positive factor and the direction field looks exactly the same. So a solution curve stretched in this way is again a solution curve.
Example For the slope is at each of the points , and , the same along the whole ray. For the slopes at those points are , and , so that equation is not scale invariant. One solution of the first equation is on , since . Stretching it by a factor gives , which is again a solution, because the same check gives .
Ratio substitution
Definition For on an interval of that does not contain , the ratio substitution introduces the new unknown
By the product rule , so the equation becomes
A differentiable function solves the original equation on the interval exactly when solves this one. The quotient rule gives the same relation in the form .
In plain words Write as times the ratio. Both factors change with , so the derivative of has two terms. Dropping the term , or writing , is a common error.
Example For we have . Substituting gives , and the terms cancel, leaving . Writing instead would give , a different equation, and none of its solutions gives a solution of the original equation.
Reduction to a separable equation
Definition Let be continuous on an open interval. The equation is separable, of the form with and . On an interval of that does not contain , a solution whose values stay where satisfies
After solving for , the solution of the original equation is , the whole expression for multiplied by . Its interval must avoid , where the original slope is undefined, and every point where the formula breaks down.
In plain words After the substitution, the dependence on and the dependence on come apart, so the method for separable equations applies. Then multiply by to return to .
Example Solve with on . The substitution gave , so and . Then , and , so
The check is direct, since and . The maximal interval is . As the solution tends to while its slope tends to , and because the equation itself is undefined at , no solution passes through that line.
Excluded solution branches
Definition An excluded solution branch is a solution of the original equation that the separated formula does not produce. Each root of gives the constant ratio and hence the line solution on each half-plane, because then . Separating divides by , so these roots must be found before dividing, and their lines added to the answer when the formula does not contain them. In addition, the line is excluded from the start, the half-planes and are handled separately, with in place of , and the explicit formula for holds only on intervals that avoid its own singular points.
In plain words Before dividing by , ask which constant ratios make it zero. Each one gives a straight-line solution that the final formula may leave out.
Example For
we have and . The root gives , which clearly solves the equation. For , separating gives
No value of gives , so the zero solution has to be added separately. Each nonzero branch lives on an interval that avoids both and the pole where . With , for instance, the branch through is on .
Check yourself
- Decide which of the equations , and have the form .
Show the answer
The first one does. Dividing the numerator and the denominator by gives with , valid where . The second does not, since along the ray its slope is at but at . The third does not either. It is a homogeneous linear equation, because it has no forcing term, but its slope is at and at , so it is not scale invariant. The two meanings of homogeneous are different properties.
- Find all solutions of
on the half-plane .
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With the right side is , so the substitution gives . The root gives the line , and indeed its slope equals . For , separating gives
so and
No value of gives , so the complete answer is this family together with the line . Each curve of the family lives on an interval of that avoids , that is on or on .
- Solve the initial-value problem below and find the maximal interval of its solution.
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Here , so the substitution gives . Since is never zero, no line solution is lost. Separating gives , so on
At the ratio is , so and . Since , the positive root is the right one, and
The equation divides by , so the solution must stay positive, which requires , that is . The maximal interval is , where . As from the right, and the slope grows without bound.