Exercise 7.3 · Q4:
Find the integral of the function
Let .
Using ,
Put . Then .
.
Want the reason behind every step, the basics and the checks?
An odd power of sine has a spare factor. Keep one aside and turn the remaining into . The spare is (up to a constant) the derivative of , so the substitution turns the whole integral into a polynomial in .
- Given
- , defined for every real .
- To find
- .
- Plan
- (1) Write with . (2) Substitute . (3) Integrate the polynomial and return to . (4) Differentiate back to check. (5) Compare with the triple-angle route used in Example 7(iii).
Basics you need
, so for every . Basics: trigonometric identities for integrals
If then , and (Section 7.3.1). Here and . Basics: substitution
, (standard formulae, Section 7.2). Basics: powers and the power rule
is right exactly when is the integrand (Property (I), Section 7.2.1). Basics: integration undoes differentiation
Solution
Keep one sine aside
Write . Then
With an odd power we can split off one factor and still have an even power left, which the Pythagorean identity converts entirely into cosines. Everything is then a function of times , and is what the derivative of supplies. This is the method of Example 6(i) and of the "Alternatively" part of Example 7(iii).Substitute
By the chain rule, , so
Therefore
Two things to watch: the minus sign (the derivative of cosine is minus sine) and the factor 2 (the derivative of the inner angle ). Both end up in the constant . No is left inside the integral, so the substitution is complete. It is valid for all , since is differentiable everywhere.Change of variable, Section 7.3.1; chain rule, Theorem 4, Section 5.3.1. Lesson: integration by substitutionIntegrate and return to
Put back :
The integrand in is a polynomial, so the power formula does everything. Multiplying into the bracket: .Check: differentiate the answer back
Let , so . Then
The answer is correct for every real .
In the last line , which is Step 1 read backwards.Chain rule, Theorem 4, Section 5.3.1. Basics: integration undoes differentiationThe triple-angle route gives the same function
Example 7(iii) also uses , that is . With (so ):
Now use with :
This is exactly our answer: here the two routes agree with no difference in the constant at all.
The book's Remark after Example 7 says the two answers there are equivalent "using trigonometric identities"; this step shows how, for our function. In general two correct answers may differ by a constant; here they happen to be identical.
valid for all real . This is exactly the textbook answer, .
At with : and , so the slope is about . The integrand is . They agree to three significant figures (the gap is the error of the difference quotient).
- Treating like . The half-angle identity alone does not lower a cube; split off one factor first (or use the triple-angle identity).
- Losing the minus sign in .
- Losing the factor 2 from the inner angle .
- Thinking two different-looking answers must be wrong. Step 5 shows that very different-looking answers can be the same function.
- Odd power of sine: keep one , convert the rest with , put . (Odd power of cosine: the mirror image, .)
- For an inner angle , carries the factor .
- Compare answers by rewriting one into the other or by checking that their difference is constant.
Every fact used, and where it comes from
| Fact | Used in | Source |
|---|---|---|
| Steps 1, 4 | Pythagorean identity (Class XI trigonometry) | |
| Substitution | Step 2 | Section 7.3.1; same method as Example 6(i) and Example 7(iii) |
| Step 3 | Standard formulae, Section 7.2 | |
| Chain rule | Steps 2, 4 | Theorem 4, Section 5.3.1 |
| , | Step 5 | Triple-angle formulas (Class XI); Example 7(iii), Section 7.3.2 |
| Differentiation undoes integration | Step 4 | Property (I), Section 7.2.1 |
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