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QLDMath MethodsSyllabus dot point

Topic 2: Trigonometric functions and integration applications

Integrate trigonometric functions including sin(kx)\sin(kx), cos(kx)\cos(kx) and sec2(kx)\sec^2(kx), and apply the linear reverse-chain rule for integrals of the form f(ax+b)f(ax+b)

A focused answer to the QCE Maths Methods Unit 4 dot point on integrating trigonometric functions. Antiderivatives of sin(kx)\sin(kx), cos(kx)\cos(kx) and sec2(kx)\sec^2(kx) with the 1/k1/k reverse-chain factor, definite-integral evaluation with exact values at standard angles, and worked PSMT-style applications.

Generated by Claude Opus 4.88 min answer

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  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

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 sec2(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
sinx\sin x cosx+C-\cos x + C
cosx\cos x sinx+C\sin x + C
sec2x\sec^2 x tanx+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
sec2(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:

  • ddxsinx=+cosx\frac{d}{dx} \sin x = +\cos x (no sign change).
  • ddxcosx=sinx\frac{d}{dx} \cos x = -\sin x (sign change).

Reversing:

  • cosxdx=+sinx\int \cos x \, dx = +\sin x (no sign change).
  • sinxdx=cosx\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(2x5)dx=12sin(2x5)+C\int \cos(2x - 5) \, dx = \frac{1}{2} \sin(2x - 5) + C.
  • e4x+2dx=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 sinθ\sin \theta cosθ\cos \theta tanθ\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.

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=sinxy = \sin x and y=cosxy = \cos x on [0,π/4][0, \pi/4].

At x=0x = 0: sin0=0\sin 0 = 0, cos0=1\cos 0 = 1. So cosx>sinx\cos x > \sin x on [0,π/4)[0, \pi/4).

Area =0π/4(cosxsinx)dx=[sinx+cosx]0π/4=(sin(π/4)+cos(π/4))(0+1)=(2/2+2/2)1=21= \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.

Exam-style practice questions

Practice questions written in the style of QCAA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

2024 QCAA-style P13 marksEvaluate 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=312sin(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 (it's (sin)=+cos-(-\sin) = +\cos - wait, antiderivative of 2sinx-2\sin x is +2cosx+2\cos x here, careful), exact-value evaluation at π\pi and π/2\pi/2, and the boxed final answer.

2023 QCAA-style P24 marksA 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=512cos(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: 521+C=0-\frac{5}{2} \cdot 1 + C = 0, so C=52C = \frac{5}{2}.

Therefore x(t)=52(1cos(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(1cos(2π))0=52(11)=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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