Unit 2 - Integration Methods as Structural Rewriting · AP
Trigonometric Integrals
Use parity and Pythagorean identities to rewrite powers of sine and cosine into integrable forms.
By Theory Commons Editors8 min readPublished Sep 1, 2026Updated Sep 1, 2026
Overview
Central question: Which power and parity patterns suggest identities? You will use identities to expose a factor that can become a differential, and you will distinguish the odd-power case from the all-even case. An identity is not inserted to make an expression look more complicated. It is chosen because it changes the integral into a form that has an antiderivative.
Look first at ∫sin3(x)cos2(x)dx. The power of sine is odd. One sine factor can be saved, while the remaining even power sin2(x) can be converted with sin2(x)=1−cos2(x). Predict which substitution will then finish the problem.
Save one factor when a power is odd
Rewrite the integrand as
sin2(x)sin(x)cos2(x)=(1−cos2(x))sin(x)cos2(x).
Now u=cos(x) is justified because du=−sin(x)dx. The remaining integral is polynomial:
∫sin3(x)cos2(x)dx=−∫(1−u2)u2du=−3u3+5u5+C.
Returning to the original variable gives
−3cos3(x)+5cos5(x)+C.L3-V01 - Odd-power decision path. Place it beside the rewrite. It is a static flow diagram: “odd sine power” leads to “save sinx\sin xsinx,” then “rewrite sin2x=1−cos2x\sin^2x=1-\cos^2xsin2x=1−cos2x,” then “u=cosxu=\cos xu=cosx.” Include the derivative du=−sinx dxdu=-\sin x\,dxdu=−sinxdx at the final arrow
The sign in du=−sin(x)dx is easy to lose. Write it immediately when selecting u; do not repair signs by intuition at the end. Differentiate the final answer to verify both the powers and the sign.
Use half-angle identities when both powers are even
For ∫sin2(x)cos2(x)dx, neither sine nor cosine has an odd power to save. The previous strategy cannot create a lone differential factor. Instead, use the double-angle identity
sin(x)cos(x)=21sin(2x).
Squaring gives
sin2(x)cos2(x)=41sin2(2x)=81(1−cos(4x)).
The integral is now direct:
∫sin2(x)cos2(x)dx=8x−32sin(4x)+C.L3-V02 - Even-power identity route. Place it beside the double-angle calculation. It is a static equivalence chain with sin2xcos2x\sin^2x\cos^2xsin2xcos2x, 14sin2(2x)\frac14\sin^2(2x)41sin2(2x), and 18(1−cos4x)\frac18(1-\cos4x)81(1−cos4x) in three linked panels. Use the same font size and do not present the chain as a fraction written with slashes
Contrast: choose the factor that matches the derivative
For ∫sin4(x)cos3(x)dx, cosine has an odd power. Save one cos(x), convert cos2(x) to 1−sin2(x), and choose u=sin(x). Do not save sine simply because it appears first; d(sinx)=cosxdx determines the productive pairing.
L3-V03 - Parity comparison. Place it after the contrast. It is a two-column static chart: odd sine power pairs with u=cosxu=\cos xu=cosx; odd cosine power pairs with u=sinxu=\sin xu=sinx; both even leads to a half-angle identity
Explain the identity choice
The Pythagorean identity is useful here because it changes an even power into an expression involving the other function. In the odd-sine example, saving one sine leaves an even sine power. Replacing sin2x by 1−cos2x produces a polynomial in the same function chosen for u. This is the desired structural outcome: after u=cosx, the remaining expression contains only powers of u and du.
If instead you rewrite cos2x as 1−sin2x in that example, the saved sine factor no longer pairs naturally with the chosen u=cosx. The algebra may remain true, but it does not expose the differential relationship. An identity is selected for compatibility with the factor being saved, not because one identity is universally preferable.
For all-even powers, half-angle identities are needed because neither function supplies a single differential factor. The formulas
sin2x=21−cos(2x),cos2x=21+cos(2x)
lower the powers and replace the original product by sums of directly integrable functions. The argument 2x requires attention when integrating: ∫cos(2x)dx=21sin(2x)+C. The factor 21 comes from the derivative of the inside function, just as it did in substitution.
A definite-integral comparison
Consider ∫0π/2sin3xcos2xdx. The same odd-power strategy applies, but the transformed bounds change when u=cosx. At x=0, u=1; at x=2π, u=0. The negative differential reverses the order, giving a positive integral. This is a useful combined retrieval: parity chooses the rewrite, substitution changes the variable, and the bounds must follow the new variable.
The final value should be positive because the original integrand is nonnegative on the stated interval. Checking sign and scale against the graph is especially useful when a minus sign enters through du=−sinxdx.
Stop and check
A common incorrect start is to substitute u=sin(x) in ∫sin3(x)cos2(x)dx without first creating a lone cos(x)dx. The misconception is choosing a familiar function without checking whether its differential is present. The correction is to inspect parity before choosing u and to show the identity rewrite that creates the required differential.
Retrieval check
Set up, but do not fully simplify, ∫cos5(x)sin4(x)dx. Because cosine has an odd power, save one cos(x), rewrite the remaining cos4(x) as (1−sin2(x))2, and use u=sin(x). Explain why a half-angle identity is unnecessary in this case.
The next lesson uses a different trigonometric rewrite. Instead of powers of sine and cosine, radicals such as a2−x2 are matched to a Pythagorean identity through a trigonometric substitution.