Miscellaneous · Q12: ,
12. Find a particular solution of the differential equation , given that when .
Here . Separating the variables,
Multiplying the numerator and denominator on the left by ,
Put . Then .
Integrating both sides of (i),
Putting , in (ii),
Putting in (ii),
At the product is , so
The particular solution is .
The answer key writes , ; that form solves the equation only where , and the solution through is defined for .
Want the reason behind every step, the basics and the checks?
The slope is a function of times a function of , so the variables separate. The -side, , becomes easy after multiplying top and bottom by : has the derivative of its denominator (up to sign) on top, so it integrates to a logarithm. The point then fixes the constant and also the signs inside the absolute values, which decides where the solution lives.
- Given
- , and when .
- To find
- The particular solution through .
- Plan
- (1) Read the equation: order, degree, separable. (2) Separate, and look at the constant solution lost by dividing. (3) Integrate, with and one constant. (4) Use the condition. (5) Remove the logarithms and the absolute values, solve for , and find the interval. (6) Compare with the textbook's form. (7) Check by substituting back, and see the curve.
Basics you need
If with , then ; integrate both sides and add one constant (Section 9.4.1). Lesson: variables separable
With , , so (Section 7.3.1; Section 7.2, formula (xii)). Basics: every method ends with an integral
; exactly when ; for every , and needs . Basics: exponentials
Put the given point into the general solution to find the constant (Section 9.3). Lesson: general and particular solutions
Solution
Read the equation: separable
Divide by , which needs . The equation has order 1 and, as a polynomial in , degree 1. The right side is a function of times a function of , the separable form of Section 9.4.1. The given point has , so we work on an interval containing 0 that avoids .Section 9.4.1, equation (2); Sections 9.2.1 and 9.2.2. Lesson: variables separableSeparate the variables
Dividing by needs , that is . Then multiply the top and bottom of the left side by : . The case is a constant solution (both sides of the equation are 0), but it does not pass through , since .Section 9.4.1, equation (3). Basics: dy = y′ dxIntegrate both sides, with one constant
On the left put , so :
So the general solution is
, so the top is . Both integrals are of the form . The two constants of integration are collected into one, .Section 9.4.1, equation (4); Section 7.3.1; Section 7.2, formula (xii). Basics: one constant for order 1Use the condition: when
Putting , in (1):
, so , and on both sides.Section 9.3: a particular solution. Lesson: general and particular solutionsRemove the logarithms and the absolute values
With , (1) gives , that is
The product is continuous along the solution and has absolute value 1, so it cannot change sign; at it equals . Hence
To change sign, a continuous quantity would have to pass through 0, but here its absolute value is always 1. Taking needs . On the interval through we have , so we need , that is . As , the fraction tends to and : the solution cannot be continued further left. As , , the constant solution of Step 2.Compare with the textbook's form
The textbook gives , . For the fraction is positive, so this is our answer there. But on the absolute value form does not solve the equation. Take : the formula gives , so the right side is ; but its slope there is , so the left side is .
Differentiating gives wherever it is defined. Where the fraction is negative, is instead of , and the equation fails. The textbook's form is valid only where , and the solution through is the piece .(Section 7.2, formula (xii)); a particular solution lives on one interval through the given point. Lesson: the Miscellaneous exercise playerCheck by substituting back, and see the curve
From , for :
The two sides agree, and at : .
Slope field of for , with equal scales, and the particular solution through . It plunges towards the dashed line and levels off towards the dashed constant solution . because . Substituting the answer back makes both sides equal to , and the point satisfies it.A solution makes L.H.S. = R.H.S. (Section 9.3). Basics: a rule for slopes
The general solution is , and the particular solution with when is , for . (Textbook answer: , ; the same for , but the absolute value form does not solve the equation on , see Step 6.)
Take : . The equation gives for , so .
The curve itself: and , a difference of , so
- Integrating directly. Multiply top and bottom by first; then it is .
- Losing the minus sign: , so .
- Keeping the absolute values to the end. The point fixes their signs; without that step the answer looks valid where it is not.
- Forgetting the interval. The solution through stops at , not at .
- For , multiply top and bottom by to get the derivative of the denominator on top.
- After using the point, settle the signs inside ; that also tells you the interval of the particular solution.
- Dividing by can lose constant solutions; here , which the curve approaches but never reaches.
Every fact used, and where it comes from
| Fact | Used in | Source |
|---|---|---|
| Separable form; separating and integrating, one constant | Steps 1, 2, 3 | Section 9.4.1, equations (2) to (4) (Lesson) |
| Order and degree | Step 1 | Sections 9.2.1 and 9.2.2 (Lesson) |
| Substitution ; | Step 3 | Section 7.3.1; Section 7.2, formula (xii) (Basics) |
| Particular solution from a point | Step 4 | Section 9.3 (Lesson) |
| Laws of logarithms; for | Steps 5, 6, 7 | Chapter 5, Section 5.4 (Basics) |
| , with the chain rule; substituting back | Steps 6, 7 | Section 7.2, formula (xii); Chapter 5, Section 5.3.1; Section 9.3 (Basics) |
Tell us if something on this page is wrong or unclear, or if you would like a fuller explanation, another method or a new feature. Send feedback on this problem →