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Integration of trigonometric functions: QCE Maths Methods Unit 4

Syllabus dot point

“Integrate trigonometric functions including sin⁡(kx)\sin(kx), cos⁡(kx)\cos(kx) and sec⁡2(kx)\sec^2(kx), and apply the linear reverse-chain rule for integrals of the form f(ax+b)f(ax+b)”

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Quick answer

Integration of trigonometric functions in QCE Methods Unit 4 follows the standard antiderivative rules (∫sin⁡(kx) dx=−1kcos⁡(kx)+C\int \sin(kx) \, dx = -\frac{1}{k} \cos(kx) + C, ∫cos⁡(kx) dx=1ksin⁡(kx)+C\int \cos(kx) \, dx = \frac{1}{k} \sin(kx) + C, ∫sec⁡2(kx) dx=1ktan⁡(kx)+C\int \sec^2(kx) \, dx = \frac{1}{k} \tan(kx) + C) with the linear reverse-chain 1a\frac{1}{a} factor; Paper 1 evaluations require exact values at standard angles (π/6,π/4,π/3,π/2,π\pi/6, \pi/4, \pi/3, \pi/2, \pi) and the most-tested detail is including the 1k\frac{1}{k} factor in non-unit coefficient integrals.

Jump to a section
  1. What this dot point is asking
  2. Standard trigonometric antiderivatives
  3. The linear reverse chain rule
  4. Definite integrals with exact values
  5. Area between trig curves
  6. Applications in PSMT and EA
  7. Exam-style questions

What this dot point is asking

QCAA wants you to integrate trigonometric functions of the form sin⁡(kx)\sin(kx), cos⁡(kx)\cos(kx) and sec⁡2(kx)\sec^2(kx), evaluate definite integrals with exact values at standard angles, and apply trig integration in kinematics and area contexts. The dot point feeds the IA3 PSMT and the EA Paper 1 short response.

Standard trigonometric antiderivatives

The reverse of the Unit 3 trig derivatives, with the 1k\frac{1}{k} reverse-chain factor for non-unit coefficients.

Integrand Antiderivative
sin⁡x\sin x −cos⁡x+C-\cos x + C
cos⁡x\cos x sin⁡x+C\sin x + C
sec⁡2x\sec^2 x tan⁡x+C\tan x + C
sin⁡(kx)\sin(kx) −1kcos⁡(kx)+C-\frac{1}{k} \cos(kx) + C
cos⁡(kx)\cos(kx) 1ksin⁡(kx)+C\frac{1}{k} \sin(kx) + C
sec⁡2(kx)\sec^2(kx) 1ktan⁡(kx)+C\frac{1}{k} \tan(kx) + C

The 1k\frac{1}{k} factor is the reverse of the chain-rule factor that appears when differentiating sin⁡(kx)\sin(kx) to get kcos⁡(kx)k \cos(kx). Forgetting this factor is the single most common Paper 1 error in trig integration.

Sign check

The pattern for derivatives is:

  • ddxsin⁡x=+cos⁡x\frac{d}{dx} \sin x = +\cos x (no sign change).
  • ddxcos⁡x=−sin⁡x\frac{d}{dx} \cos x = -\sin x (sign change).

Reversing:

  • ∫cos⁡x dx=+sin⁡x\int \cos x \, dx = +\sin x (no sign change).
  • ∫sin⁡x dx=−cos⁡x\int \sin x \, dx = -\cos x (sign change).

The antiderivative of sin⁡\sin is −cos⁡-\cos. The antiderivative of cos⁡\cos is +sin⁡+\sin. These two patterns generate every trig sign error you'll see.

The linear reverse chain rule

For an integrand of the form f(ax+b)f(ax + b) where a,ba, b are constants:

∫f(ax+b) dx=1aF(ax+b)+C\int f(ax + b) \, dx = \frac{1}{a} F(ax + b) + C

where FF is an antiderivative of ff.

Examples:

  • ∫sin⁡(3x+1) dx=−13cos⁡(3x+1)+C\int \sin(3x + 1) \, dx = -\frac{1}{3} \cos(3x + 1) + C.
  • ∫cos⁡(2x−5) dx=12sin⁡(2x−5)+C\int \cos(2x - 5) \, dx = \frac{1}{2} \sin(2x - 5) + C.
  • ∫e4x+2 dx=14e4x+2+C\int e^{4x + 2} \, dx = \frac{1}{4} e^{4x + 2} + C.

The 1a\frac{1}{a} corrects for the chain rule factor that would appear when differentiating the antiderivative.

Definite integrals with exact values

For definite integrals of trig functions evaluated at standard angles, the QCAA Paper 1 expects exact-value answers (in terms of π\pi, fractions, surds).

Standard exact values:

θ\theta sin⁡θ\sin \theta cos⁡θ\cos \theta tan⁡θ\tan \theta
00 00 11 00
π/6\pi/6 1/21/2 3/2\sqrt{3}/2 1/31/\sqrt{3}
π/4\pi/4 2/2\sqrt{2}/2 2/2\sqrt{2}/2 11
π/3\pi/3 3/2\sqrt{3}/2 1/21/2 3\sqrt{3}
π/2\pi/2 11 00 undefined
π\pi 00 −1-1 00
3π/23\pi/2 −1-1 00 undefined
2π2\pi 00 11 00

The Paper 1 expects fluency with these. Substituting π=3.14159\pi = 3.14159 and computing decimals loses marks on a Paper 1 exact-value question.

Worked example

Three definite integrals of trigonometric functions, each requiring exact-value evaluation at standard angles.

Step 1: Integrate sec⁡2x\sec^2 x on [0,π/4][0, \pi/4]

The antiderivative of sec⁡2x\sec^2 x is tan⁡x\tan x (this is the reverse of the differentiation rule). There is no chain rule factor needed here because the argument is simply xx.

∫0π/4sec⁡2(x) dx=[tan⁡x]0π/4=tan⁡ ⁣(π4)−tan⁡(0)=1−0=1\int_{0}^{\pi/4} \sec^2(x) \, dx = [\tan x]_{0}^{\pi/4} = \tan\!\left(\frac{\pi}{4}\right) - \tan(0) = 1 - 0 = 1

Step 2: Integrate cos⁡(3x)\cos(3x) on [0,π/6][0, \pi/6], including the reverse-chain factor

The antiderivative of cos⁡(kx)\cos(kx) is 1ksin⁡(kx)\frac{1}{k}\sin(kx). Here k=3k = 3, so the factor 13\frac{1}{3} appears in front. This corrects for the factor of 33 that the chain rule would produce on differentiation.

∫0π/6cos⁡(3x) dx=[13sin⁡(3x)]0π/6=13sin⁡ ⁣(π2)−13sin⁡(0)=13(1)−0=13\int_{0}^{\pi/6} \cos(3x) \, dx = \left[\frac{1}{3}\sin(3x)\right]_{0}^{\pi/6} = \frac{1}{3}\sin\!\left(\frac{\pi}{2}\right) - \frac{1}{3}\sin(0) = \frac{1}{3}(1) - 0 = \frac{1}{3}

Step 3: Integrate a mixed integrand on [0,π/2][0, \pi/2]

For ∫0π/2[2sin⁡x+cos⁡(2x)] dx\int_{0}^{\pi/2} [2\sin x + \cos(2x)] \, dx, we antidifferentiate each term. The antiderivative of 2sin⁡x2\sin x is −2cos⁡x-2\cos x (the sign changes), and the antiderivative of cos⁡(2x)\cos(2x) includes the 12\frac{1}{2} reverse-chain factor.

Antiderivative:−2cos⁡x+12sin⁡(2x)\text{Antiderivative:} \quad -2\cos x + \frac{1}{2}\sin(2x)

Evaluate at the upper limit x=π/2x = \pi/2, using cos⁡(π/2)=0\cos(\pi/2) = 0 and sin⁡(π)=0\sin(\pi) = 0:

−2cos⁡ ⁣(π2)+12sin⁡(π)=−2(0)+12(0)=0-2\cos\!\left(\frac{\pi}{2}\right) + \frac{1}{2}\sin(\pi) = -2(0) + \frac{1}{2}(0) = 0

Evaluate at the lower limit x=0x = 0, using cos⁡(0)=1\cos(0) = 1 and sin⁡(0)=0\sin(0) = 0:

−2cos⁡(0)+12sin⁡(0)=−2(1)+0=−2-2\cos(0) + \frac{1}{2}\sin(0) = -2(1) + 0 = -2

Subtract lower from upper to get the definite integral.

Final answer: 0−(−2)=20 - (-2) = 2.

Area between trig curves

Trig curves often appear in area problems. The general procedure (top minus bottom on the interval between intersection points) is the same as in the area-between-curves dot point.

Example. Area enclosed between y=sin⁡xy = \sin x and y=cos⁡xy = \cos x on [0,π/4][0, \pi/4].

At x=0x = 0: sin⁡0=0\sin 0 = 0, cos⁡0=1\cos 0 = 1. So cos⁡x>sin⁡x\cos x > \sin x on [0,π/4)[0, \pi/4).

Area =∫0π/4(cos⁡x−sin⁡x) dx=[sin⁡x+cos⁡x]0π/4=(sin⁡(π/4)+cos⁡(π/4))−(0+1)=(2/2+2/2)−1=2−1= \int_{0}^{\pi/4} (\cos x - \sin x) \, dx = [\sin x + \cos x]_{0}^{\pi/4} = (\sin(\pi/4) + \cos(\pi/4)) - (0 + 1) = (\sqrt{2}/2 + \sqrt{2}/2) - 1 = \sqrt{2} - 1.

Applications in PSMT and EA

The QCAA Methods PSMT often involves modelling periodic phenomena (tides, biological cycles, oscillating systems). Integration of the model gives accumulated quantities (total flow, energy, average values).

The EA Paper 1 short response routinely includes trig integration questions involving the 1k\frac{1}{k} factor.

Common errors
Missing the 1k\frac{1}{k} factor
∫sin⁡(2x) dx=−12cos⁡(2x)+C\int \sin(2x) \, dx = -\frac{1}{2} \cos(2x) + C, not −cos⁡(2x)+C-\cos(2x) + C. This is the single most common error.
Wrong sign on cos⁡\cos antiderivative
∫sin⁡x=−cos⁡x\int \sin x = -\cos x (sign change); ∫cos⁡x=+sin⁡x\int \cos x = +\sin x (no sign change).
Using degrees instead of radians
QCAA Methods Paper 1 uses radians. sin⁡(π/2)=1\sin(\pi/2) = 1; sin⁡(90)\sin(90) in calculator mode-degrees is the same value, but the formula expects radians.
Substituting π\pi as 3.14 in Paper 1
Paper 1 expects exact values.
Forgetting the constant of integration
Indefinite integrals always include CC. Definite integrals do not (it cancels in the subtraction).
Sign-cancellation forgotten when integrand changes sign on the interval
For total area, split at zeros and take absolute values; for signed integral, do not.

Exam-style questions

Questions in the style of QCAA 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.

Practice3 marks
Evaluate ∫0π/2(3cos⁡(2x)−2sin⁡(x)) dx\int_{0}^{\pi/2} (3 \cos(2x) - 2 \sin(x)) \, dx exactly.
Show worked answer →

Antidifferentiate term by term using the reverse-chain factor for sin⁡(2x)\sin(2x).

∫3cos⁡(2x) dx=3⋅12sin⁡(2x)=32sin⁡(2x)\int 3 \cos(2x) \, dx = 3 \cdot \frac{1}{2} \sin(2x) = \frac{3}{2} \sin(2x).

∫−2sin⁡(x) dx=2cos⁡(x)\int -2 \sin(x) \, dx = 2 \cos(x).

Combined antiderivative: F(x)=32sin⁡(2x)+2cos⁡(x)F(x) = \frac{3}{2} \sin(2x) + 2 \cos(x).

Apply the fundamental theorem.

F(π/2)−F(0)=[32sin⁡(π)+2cos⁡(π/2)]−[32sin⁡(0)+2cos⁡(0)]=(0+0)−(0+2)=−2F(\pi/2) - F(0) = \left[ \frac{3}{2} \sin(\pi) + 2 \cos(\pi/2) \right] - \left[ \frac{3}{2} \sin(0) + 2 \cos(0) \right] = (0 + 0) - (0 + 2) = -2.

Markers reward the 1/21/2 factor inside sin⁡(2x)\sin(2x), the correct sign on cos⁡\cos antiderivative (the antiderivative of −2sin⁡x-2\sin x is +2cos⁡x+2\cos x, because the sign flips twice), exact-value evaluation at π\pi and π/2\pi/2, and the boxed final answer.

Practice4 marks
A particle moves with velocity v(t)=5sin⁡(2t)v(t) = 5 \sin(2t) m/s, where tt is in seconds. (a) Find the position function x(t)x(t) given x(0)=0x(0) = 0. (b) Find the displacement of the particle from t=0t = 0 to t=πt = \pi seconds.
Show worked answer →

(a) Position function. Antidifferentiate velocity.

x(t)=∫5sin⁡(2t) dt=5⋅−12cos⁡(2t)+C=−52cos⁡(2t)+Cx(t) = \int 5 \sin(2t) \, dt = 5 \cdot -\frac{1}{2} \cos(2t) + C = -\frac{5}{2} \cos(2t) + C.

Apply x(0)=0x(0) = 0: −52⋅1+C=0-\frac{5}{2} \cdot 1 + C = 0, so C=52C = \frac{5}{2}.

Therefore x(t)=52(1−cos⁡(2t))x(t) = \frac{5}{2} (1 - \cos(2t)) m.

(b) Displacement from t=0t = 0 to t=πt = \pi.

Displacement=x(π)−x(0)=52(1−cos⁡(2π))−0=52(1−1)=0\text{Displacement} = x(\pi) - x(0) = \frac{5}{2}(1 - \cos(2\pi)) - 0 = \frac{5}{2}(1 - 1) = 0 m.

The particle returns to its starting position at t=πt = \pi (one full period of sin⁡(2t)\sin(2t)).

Markers reward the antiderivative with −12-\frac{1}{2} factor, applying initial condition to find CC, and the displacement calculation showing the particle returns to start.

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