Exercise 9.4 · Q15: Particular solution of ,
For each of the differential equations in Exercises from 11 to 15, find the particular solution satisfying the given condition:
15. ; when
The equation can be written as
Replacing by and by ,
So is homogeneous of degree zero, and the equation is homogeneous.
Put . Then .
Separating the variables,
Integrating both sides,
Putting ,
Putting , in (i),
The particular solution is ().
Want the reason behind every step, the basics and the checks?
The terms , and all have degree 2, so the slope depends only on : homogeneous, put . After the terms cancel, what is left is , whose -integral is a power, not a log. The condition then fixes the constant, and the answer can be solved for .
- Given
- , and when .
- To find
- The particular solution: no arbitrary constant, passing through .
- Plan
- (1) Write it as . (2) Show . (3) Put . (4) Simplify to . (5) Separate. (6) Integrate. (7) Put back. (8) Use the condition and solve for . (9) Check, and see where it lives.
Basics you need
is homogeneous when for every nonzero (Section 9.4.2). Basics: scale x and y together
; the equation becomes (Section 9.4.2). Lesson: homogeneous equations, put y = vx
and (Section 7.2, formulas (i) and (xii)). Basics: every method ends with an integral
One arbitrary constant in the general solution of a first order equation (chapter Summary); the condition fixes it and gives the particular solution (Section 9.3). Lesson: general and particular solutions
Solution
Write the equation as
Move across and divide by :
This needs , which the substitution needs anyway, so dividing by loses no solution with .Section 9.4.2: a homogeneous equation has the form . Lesson: homogeneous equationsShow that it is homogeneous:
So is a homogeneous function of degree zero, and (1) is a homogeneous differential equation.
Top and bottom both have degree 2, so cancels, for any .Section 9.4.2: homogeneous function of degree . Basics: scale x and y togetherSubstitute
Put ; then , and (1) becomes
Dividing top and bottom by leaves a function of only.Section 9.4.2, equations (2) and (3). Lesson: put y = vxSimplify to
, so subtracting leaves .Section 9.4.2, equation (4). Lesson: homogeneous equationsSeparate and
Multiply by and by . This divides by , which is 0 for . The constant makes both sides of Step 4 zero, so is a solution (the given equation reads ). It is set aside here, but at it gives , not 2, so the particular solution loses nothing.Section 9.4.2, equation (5); separating as in Section 9.4.1. Basics: dy = y′ dxIntegrate both sides
By the power rule, ; it is not a log, because the power is , not . The equation has order 1 (degree 1), so one arbitrary constant. Check: .Section 7.2, formulas (i) and (xii). Basics: every method ends with an integralPut back: the general solution
Since ,
The answer in the original variables, valid for and . So the solution of Step 5 is not given by any : it is an extra solution, set aside by the division by .Section 9.4.2: replace to get the general solution. Lesson: Examples 10 to 13Use the condition: when
Putting , in (2):
So . Multiply by : , and the particular solution is
Solving for needs , that is . This is the book's form.Section 9.3: a particular solution from the general one. Lesson: general and particular solutionsCheck by substituting back, and see where it lives
Check (for , where ): by the quotient rule,
Then , and
So . And at , .
Where it lives. The formula breaks down at and where . The solution through is the piece containing : . On it , so , as Step 5 needed. As from the left, grows without bound; as , .
Slope field of for , with equal scales, and the particular solution through , for . It rises without bound as approaches (dashed line), and runs into the origin (hollow dot: is excluded) as . Getting the equation back proves the answer. The textbook adds the conditions , : these say where the formula is defined on the side of the given point. (For the formula would also need , but that side is not part of the solution through .)The quotient rule; (Chapter 5). Basics: a rule for slopes
The equation is homogeneous, since . Its general solution is , and the particular solution with when is , on . (Textbook answer: (, ).)
Take : , so . Then , and .
The equation gives the slope there. The curve itself: and , a difference of , so
- Integrating as a log. .
- Sign slips when solving for . From , multiply by : .
- Forgetting where the answer holds. The curve through stops at , where .
- Same degree everywhere means homogeneous: .
- Not every -integral is a log: gives .
- Put the given values in on their own line, find , and then say on which interval the particular solution lives.
Every fact used, and where it comes from
| Fact | Used in | Source |
|---|---|---|
| Homogeneous function of degree zero; homogeneous equation | Steps 1, 2 | Section 9.4.2 (Basics) |
| , ; | Steps 3, 4 | Section 9.4.2, equations (2) to (4) (Lesson) |
| Separating the variables; a solution set aside by the division is checked separately | Steps 5, 7 | Section 9.4.1 (separating needs ) (Basics) |
| (); | Step 6 | Section 7.2, formulas (i) and (xii) (Basics) |
| Particular solution from a given point; | Step 8 | Section 9.3 (Lesson) |
| The quotient rule; | Step 9 | Chapter 5, Sections 5.3 and 5.4 (Basics) |
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