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Integration using trigonometric identities (WACE Year 12 Mathematics Specialist Unit 4)

Syllabus dot point

“Integrate trigonometric functions by first applying double-angle, Pythagorean and product identities”

7 min read

Quick answer

Powers of sine and cosine are not directly integrable, so rewrite them first. For even powers use the double-angle identities cos⁡2x=1+cos⁡2x2\cos^2 x = \tfrac{1 + \cos 2x}{2} and sin⁡2x=1−cos⁡2x2\sin^2 x = \tfrac{1 - \cos 2x}{2}; for odd powers split off one factor and use sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1 with a substitution.

Jump to a section
  1. What this dot point is asking
  2. Even powers: the double-angle identities
  3. Where the power-reduction identities come from
  4. Odd powers: split and substitute
  5. Higher even powers
  6. Products of different angles
  7. Choosing the route from the integrand
  8. Exam-style questions

What this dot point is asking

SCSA wants you to choose the right identity to transform a trigonometric integrand into a sum of standard integrals.

Even powers: the double-angle identities

The integrals of sin⁡2x\sin^2 x and cos⁡2x\cos^2 x rely on lowering the power. From the double-angle formula for cosine,

Power-reduction identities

cos⁡2x=1+cos⁡2x2,sin⁡2x=1−cos⁡2x2.\cos^2 x = \frac{1 + \cos 2x}{2}, \qquad \sin^2 x = \frac{1 - \cos 2x}{2}.

Each right-hand side integrates termwise to a sum of a linear term and a sin⁡2x\sin 2x term. Higher even powers are reduced by applying these identities repeatedly.

Where the power-reduction identities come from

The power-reduction identities are rearrangements of the double-angle formula for cosine, cos⁡2x=1−2sin⁡2x=2cos⁡2x−1\cos 2x = 1 - 2\sin^2 x = 2\cos^2 x - 1. Solving the first form for sin⁡2x\sin^2 x gives sin⁡2x=1−cos⁡2x2\sin^2 x = \dfrac{1 - \cos 2x}{2}, and solving the second for cos⁡2x\cos^2 x gives cos⁡2x=1+cos⁡2x2\cos^2 x = \dfrac{1 + \cos 2x}{2}. Knowing the derivation means you can reconstruct the identities under exam pressure rather than relying on memory, and it links this dot point back to the double-angle work of Methods. The same double-angle relation, read in the other direction, also reverses the process when you need to express a cos⁡2x\cos 2x answer back in terms of cos⁡2x\cos^2 x.

Odd powers: split and substitute

For an odd power such as sin⁡3x\sin^3 x, peel off one factor of sin⁡x\sin x and convert the remaining even power using sin⁡2x=1−cos⁡2x\sin^2 x = 1 - \cos^2 x. Then substitute u=cos⁡xu = \cos x, since du=−sin⁡x dxdu = -\sin x\,dx supplies the leftover factor. The same idea handles odd powers of cosine with u=sin⁡xu = \sin x.

Higher even powers

A fourth power such as cos⁡4x\cos^4 x is reduced by applying the power-reduction identity twice. First, cos⁡4x=(cos⁡2x)2=(1+cos⁡2x2)2=14(1+2cos⁡2x+cos⁡22x)\cos^4 x = (\cos^2 x)^2 = \left(\dfrac{1 + \cos 2x}{2}\right)^2 = \dfrac{1}{4}(1 + 2\cos 2x + \cos^2 2x). The remaining cos⁡22x\cos^2 2x is itself reduced by cos⁡22x=1+cos⁡4x2\cos^2 2x = \dfrac{1 + \cos 4x}{2}, leaving only constants and single cosine terms in 2x2x and 4x4x, all of which integrate directly. The pattern is that each application of the identity halves the highest power, so any even power of sine or cosine eventually flattens into a sum of cosines of multiple angles.

Products of different angles

For products like sin⁡mxcos⁡nx\sin mx \cos nx, use the product-to-sum identities to rewrite as a sum of single trigonometric terms, each of which integrates directly. The relevant identities are sin⁡Acos⁡B=12[sin⁡(A+B)+sin⁡(A−B)]\sin A\cos B = \dfrac{1}{2}\big[\sin(A + B) + \sin(A - B)\big], cos⁡Acos⁡B=12[cos⁡(A+B)+cos⁡(A−B)]\cos A\cos B = \dfrac{1}{2}\big[\cos(A + B) + \cos(A - B)\big] and sin⁡Asin⁡B=12[cos⁡(A−B)−cos⁡(A+B)]\sin A\sin B = \dfrac{1}{2}\big[\cos(A - B) - \cos(A + B)\big]. After rewriting, each term is a single sine or cosine of a multiple angle and integrates with the usual 1k\dfrac{1}{k} factor.

Choosing the route from the integrand

Diagnosing the integrand quickly is the key skill. Scan the powers of sine and cosine present. If the highest power is even and there is no convenient derivative pairing, reach for power reduction. If there is an odd power, split off one factor of that function and substitute, letting the leftover factor become dudu. If the integrand is a product of trig functions of different angles, use the product-to-sum identities. A mixed integrand such as sin⁡2xcos⁡3x\sin^2 x\cos^3 x combines methods: peel off one cos⁡x\cos x for the substitution u=sin⁡xu = \sin x and convert the remaining cos⁡2x=1−sin⁡2x\cos^2 x = 1 - \sin^2 x, turning the whole thing into a polynomial in uu. Identifying the route before integrating avoids the dead ends that cost time in the exam.

Match the identity to the parity

Even power, use power reduction (double angle). Odd power, split one factor and substitute. Mixed angles, use product-to-sum. Choosing the right route first avoids dead ends.

Worked example

Evaluate ∫cos⁡2x dx\displaystyle\int \cos^2 x\,dx.

Step 1: Apply the power-reduction identity

The integrand cos⁡2x\cos^2 x is an even power of cosine, and there is no paired derivative present to use a substitution. The power-reduction identity converts the squared cosine into a linear expression in cos⁡2x\cos 2x, which can be integrated term by term.

cos⁡2x=1+cos⁡2x2\cos^2 x = \frac{1 + \cos 2x}{2}

Step 2: Split and integrate each term

Substituting the identity rewrites the integral as two standard integrals. The constant 12\tfrac{1}{2} is distributed across each, and each term is then integrated separately using the rule ∫cos⁡(ax) dx=1asin⁡(ax)\int \cos(ax)\,dx = \tfrac{1}{a}\sin(ax).

∫cos⁡2x dx=∫1+cos⁡2x2 dx=12∫1 dx+12∫cos⁡2x dx\int \cos^2 x\,dx = \int \frac{1 + \cos 2x}{2}\,dx = \frac{1}{2}\int 1\,dx + \frac{1}{2}\int \cos 2x\,dx

The first integral gives 12x\tfrac{1}{2}x. For the second, ∫cos⁡2x dx=12sin⁡2x\int \cos 2x\,dx = \tfrac{1}{2}\sin 2x, so 12×12sin⁡2x=14sin⁡2x\tfrac{1}{2} \times \tfrac{1}{2}\sin 2x = \tfrac{1}{4}\sin 2x.

Step 3: Combine and write the final answer

Adding the two results and including the constant of integration gives the complete antiderivative. The factor of 12\tfrac{1}{2} on cos⁡2x\cos 2x compensates for the inner derivative of 2x2x.

∫cos⁡2x dx=x2+sin⁡2x4+C\int \cos^2 x\,dx = \frac{x}{2} + \frac{\sin 2x}{4} + C

Final answer: x2+sin⁡2x4+C\dfrac{x}{2} + \dfrac{\sin 2x}{4} + C.

Common traps
Integrating cos⁡2x\cos^2 x as cos⁡3x3\tfrac{\cos^3 x}{3}
There is no chain-rule factor present; you must use the power-reduction identity first.
Forgetting the inner-derivative factor
∫cos⁡2x dx=12sin⁡2x\int \cos 2x\,dx = \tfrac{1}{2}\sin 2x, not sin⁡2x\sin 2x.
Choosing the wrong substitution for odd powers
Split off the factor whose function you are substituting, so the derivative matches.

Exam-style questions

Questions in the style of SCSA exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

WACE 2022-style5 marks
Calculator-free. Evaluate ∫0π/2sin⁡2x dx\displaystyle\int_0^{\pi/2} \sin^2 x\,dx exactly.
Show worked answer →

An even-power integral by power reduction.

Use sin⁡2x=1−cos⁡2x2\sin^2 x = \dfrac{1 - \cos 2x}{2}. Then ∫0π/2sin⁡2x dx=12∫0π/2(1−cos⁡2x) dx=12[x−sin⁡2x2]0π/2\displaystyle\int_0^{\pi/2} \sin^2 x\,dx = \dfrac{1}{2}\displaystyle\int_0^{\pi/2} (1 - \cos 2x)\,dx = \dfrac{1}{2}\left[x - \dfrac{\sin 2x}{2}\right]_0^{\pi/2}.

At x=π2x = \dfrac{\pi}{2}: π2−sin⁡π2=π2−0\dfrac{\pi}{2} - \dfrac{\sin\pi}{2} = \dfrac{\pi}{2} - 0. At x=0x = 0: 0−0=00 - 0 = 0. So the value is 12×π2=π4\dfrac{1}{2} \times \dfrac{\pi}{2} = \dfrac{\pi}{4}.

Markers reward the power-reduction identity, integrating cos⁡2x\cos 2x to 12sin⁡2x\dfrac{1}{2}\sin 2x, and the exact answer π4\dfrac{\pi}{4}.

WACE 2024-style6 marks
Calculator-assumed. Find ∫sin⁡3x dx\displaystyle\int \sin^3 x\,dx.
Show worked answer →

An odd-power integral by split-and-substitute.

Write sin⁡3x=sin⁡x⋅sin⁡2x=sin⁡x(1−cos⁡2x)\sin^3 x = \sin x \cdot \sin^2 x = \sin x (1 - \cos^2 x). Let u=cos⁡xu = \cos x, so du=−sin⁡x dxdu = -\sin x\,dx, that is sin⁡x dx=−du\sin x\,dx = -du.

The integral becomes ∫(1−u2)(−du)=∫(u2−1) du=u33−u+C=cos⁡3x3−cos⁡x+C\displaystyle\int (1 - u^2)(-du) = \displaystyle\int (u^2 - 1)\,du = \dfrac{u^3}{3} - u + C = \dfrac{\cos^3 x}{3} - \cos x + C.

Markers reward peeling off one sin⁡x\sin x, converting the rest with sin⁡2x=1−cos⁡2x\sin^2 x = 1 - \cos^2 x, the substitution u=cos⁡xu = \cos x, and substituting back.

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Sources & how we know this

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