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Derivatives of trigonometric functions in radians (QCE Mathematical Methods Unit 3)

Syllabus dot point

“Differentiate trigonometric functions, including compositions of the form sin⁡(f(x))\sin(f(x)), cos⁡(f(x))\cos(f(x)) and tan⁡(f(x))\tan(f(x)), working in radians”

7 min read

Quick answer

In radians, sin⁡x\sin x, cos⁡x\cos x and tan⁡x\tan x differentiate to cos⁡x\cos x, −sin⁡x-\sin x and sec⁡2x\sec^2 x respectively, and the chain rule extends this to ddxsin⁡(f(x))=f′(x)cos⁡(f(x))\frac{d}{dx} \sin(f(x)) = f'(x) \cos(f(x)) and analogous forms for cos⁡\cos and tan⁡\tan.

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  1. What this dot point is asking
  2. The answer
  3. Exam-style questions

What this dot point is asking

QCAA wants you to differentiate trigonometric functions and their compositions in radians, including combinations with the product, quotient and chain rules. Trigonometric derivatives appear in Paper 1 short answer, in Paper 2 modelling questions about oscillating quantities (tides, sound, AC currents, planetary orbits), and in PSMTs that involve periodic phenomena.

The answer

Why radians

In Methods, all calculus on trig functions is done with xx in radians. The formula ddx(sin⁡x)=cos⁡x\frac{d}{dx}(\sin x) = \cos x is only true when xx is in radians. If you work in degrees the derivative picks up an awkward factor of π180\frac{\pi}{180}, which is why QCAA requires radians for calculus questions and why most calculators default to degree mode on a fresh reset (always check and switch to radians).

The standard derivatives

ddx(sin⁡x)=cos⁡x\frac{d}{dx}(\sin x) = \cos x

ddx(cos⁡x)=−sin⁡x\frac{d}{dx}(\cos x) = -\sin x

ddx(tan⁡x)=sec⁡2x=1cos⁡2x\frac{d}{dx}(\tan x) = \sec^2 x = \frac{1}{\cos^2 x}

The minus sign on the derivative of cos⁡\cos is the single most common Paper 1 trap. Memorise it.

Chain-rule generalisations

For any differentiable inner f(x)f(x):

ddx(sin⁡(f(x)))=f′(x)cos⁡(f(x))\frac{d}{dx}\bigl(\sin(f(x))\bigr) = f'(x) \cos(f(x))

ddx(cos⁡(f(x)))=−f′(x)sin⁡(f(x))\frac{d}{dx}\bigl(\cos(f(x))\bigr) = -f'(x) \sin(f(x))

ddx(tan⁡(f(x)))=f′(x)sec⁡2(f(x))\frac{d}{dx}\bigl(\tan(f(x))\bigr) = f'(x) \sec^2(f(x))

The most common case is a linear inner function, where the chain rule factor is just a constant.

Linear inside argument

For constants aa and bb:

ddx(sin⁡(ax+b))=acos⁡(ax+b)\frac{d}{dx}\bigl(\sin(a x + b)\bigr) = a \cos(a x + b)

ddx(cos⁡(ax+b))=−asin⁡(ax+b)\frac{d}{dx}\bigl(\cos(a x + b)\bigr) = -a \sin(a x + b)

This is the most heavily examined form. Almost every modelling question is of the type Asin⁡(ωt+ϕ)+CA \sin(\omega t + \phi) + C.

Where the standard derivatives come from

The derivative of sin⁡x\sin x being cos⁡x\cos x follows from first principles using the limit lim⁡h→0sin⁡hh=1\lim_{h \to 0}\dfrac{\sin h}{h} = 1, which holds only when hh is in radians. That single limit is the reason calculus on trigonometric functions must use radians: in degrees the limit is π180\dfrac{\pi}{180} instead of 11, and the clean derivative formulas break. Knowing this justifies the radian requirement rather than treating it as an arbitrary rule.

Velocity, acceleration and oscillation

Differentiating a sinusoidal displacement gives a sinusoidal velocity, and differentiating again gives acceleration. For s(t)=Asin⁡(ωt)s(t) = A\sin(\omega t), the velocity is Aωcos⁡(ωt)A\omega\cos(\omega t) and the acceleration is −Aω2sin⁡(ωt)=−ω2s-A\omega^2\sin(\omega t) = -\omega^2 s. The acceleration being proportional to the negative of the displacement is the defining equation of simple harmonic motion, which is why sinusoidal models describe tides, sound and oscillating springs. QCAA modelling questions frequently ask for the velocity or the times of maximum speed, both of which come straight from these derivatives.

Worked example

Five differentiation tasks on trigonometric functions in radians, illustrating the chain rule, the product rule, and an application to velocity.

Step 1: Apply the chain rule directly to y=cos⁡(3x−1)y = \cos(3x - 1)

The outer function is cos⁡\cos and the inner function is 3x−13x - 1. The derivative of cos⁡\cos is −sin⁡-\sin, and the inner function contributes a factor of 33. Notice the minus sign appears because ddxcos⁡=−sin⁡\frac{d}{dx} \cos = -\sin.

dydx=−3sin⁡(3x−1)\frac{dy}{dx} = -3 \sin(3x - 1)

Step 2: Differentiate when the inner function is a polynomial, y=sin⁡(x2)y = \sin(x^2)

The outer function is sin⁡\sin and the inner function is x2x^2. Identifying f(x)=x2f(x) = x^2 with f′(x)=2xf'(x) = 2x, the chain rule gives the factor 2x2x in front.

dydx=2xcos⁡(x2)\frac{dy}{dx} = 2x \cos(x^2)

Step 3: Combine the chain and product rules for y=x2sin⁡xy = x^2 \sin x

The outermost structure is a product of u=x2u = x^2 and v=sin⁡xv = \sin x, so we apply the product rule. The inner function of sin⁡x\sin x is simply xx, so no chain rule is needed on the trig factor.

dydx=u′v+uv′=2xsin⁡x+x2cos⁡x\frac{dy}{dx} = u'v + uv' = 2x \sin x + x^2 \cos x

Step 4: Find velocity from a sinusoidal displacement

A particle moves with displacement s(t)=4sin⁡(2t)s(t) = 4 \sin(2t) metres. Velocity is the derivative of displacement, and the chain rule on sin⁡(2t)\sin(2t) produces a factor of 22.

v(t)=s′(t)=4×2cos⁡(2t)=8cos⁡(2t)v(t) = s'(t) = 4 \times 2 \cos(2t) = 8 \cos(2t)

Substituting t=π6t = \dfrac{\pi}{6} and using the exact value cos⁡ ⁣(π3)=12\cos\!\left(\dfrac{\pi}{3}\right) = \dfrac{1}{2}:

v ⁣(π6)=8cos⁡ ⁣(π3)=8×12=4 m/sv\!\left(\frac{\pi}{6}\right) = 8 \cos\!\left(\frac{\pi}{3}\right) = 8 \times \frac{1}{2} = 4 \text{ m/s}

Final answer: the particle's velocity at t=π6t = \dfrac{\pi}{6} s is 44 m/s. The exact value cos⁡(π/3)=12\cos(\pi/3) = \tfrac{1}{2} is expected without a calculator on Paper 1.

Step 5: Differentiate y=tan⁡(3x)y = \tan(3x)

The derivative of tan⁡\tan is sec⁡2\sec^2, and the inner function 3x3x contributes a chain rule factor of 33.

dydx=3sec⁡2(3x)=3cos⁡2(3x)\frac{dy}{dx} = 3 \sec^2(3x) = \frac{3}{\cos^2(3x)}

Common traps
Working in degrees
ddx(sin⁡x)=cos⁡x\frac{d}{dx}(\sin x) = \cos x only when xx is in radians. Set your calculator to radians for Paper 2. Paper 1 problems are always in radians by convention.
Dropping the minus sign on cos⁡\cos
ddx(cos⁡x)=−sin⁡x\frac{d}{dx}(\cos x) = -\sin x. Reversing the sign turns a maximum into a minimum and a velocity into its negative.
Missing the chain rule factor
ddx(sin⁡(2x))=2cos⁡(2x)\frac{d}{dx}(\sin(2x)) = 2 \cos(2x), not cos⁡(2x)\cos(2x). The factor of 22 comes from differentiating the inner 2x2x.
Forgetting exact values
Paper 1 expects sin⁡(π/6)=1/2\sin(\pi/6) = 1/2, cos⁡(π/4)=2/2\cos(\pi/4) = \sqrt{2}/2, tan⁡(π/3)=3\tan(\pi/3) = \sqrt{3} and the related angle values without a calculator. Drill the unit circle.
Combining identities incorrectly
sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1, not sin⁡2x−cos⁡2x=1\sin^2 x - \cos^2 x = 1. Sign errors here lead to wrong derivatives on optimisation questions.

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
Paper 1 (technique). Differentiate y=sin⁡(4x)+cos⁡(2x)y = \sin(4x) + \cos(2x) with respect to xx.
Show worked answer →

Differentiate term by term using the chain rule.

For sin⁡(4x)\sin(4x): inner function 4x4x has derivative 44, so ddxsin⁡(4x)=4cos⁡(4x)\frac{d}{dx} \sin(4x) = 4 \cos(4x).

For cos⁡(2x)\cos(2x): inner function 2x2x has derivative 22, so ddxcos⁡(2x)=−2sin⁡(2x)\frac{d}{dx} \cos(2x) = -2 \sin(2x).

dydx=4cos⁡(4x)−2sin⁡(2x).\frac{dy}{dx} = 4 \cos(4x) - 2 \sin(2x).

Markers reward both chain rule factors and the correct minus sign on the derivative of cos⁡\cos. Forgetting either factor of 22 or 44 is the most common Paper 1 mistake on this style of question.

Practice4 marks
Paper 1 (technique). Given f(x)=sin⁡(2x)cos⁡(2x)f(x) = \sin(2x) \cos(2x), (a) determine f′(x)f'(x) using the product rule and (b) verify by first rewriting f(x)f(x) using the double-angle identity.
Show worked answer →

(a) Product rule with u=sin⁡(2x)u = \sin(2x), v=cos⁡(2x)v = \cos(2x), u′=2cos⁡(2x)u' = 2 \cos(2x), v′=−2sin⁡(2x)v' = -2 \sin(2x).

f′(x)=u′v+uv′=2cos⁡(2x)⋅cos⁡(2x)+sin⁡(2x)⋅(−2sin⁡(2x))f'(x) = u' v + u v' = 2 \cos(2x) \cdot \cos(2x) + \sin(2x) \cdot (-2 \sin(2x))
=2cos⁡2(2x)−2sin⁡2(2x)=2cos⁡(4x).= 2 \cos^2(2x) - 2 \sin^2(2x) = 2 \cos(4x).

(b) Identity: sin⁡(2x)cos⁡(2x)=12sin⁡(4x)\sin(2x) \cos(2x) = \frac{1}{2} \sin(4x). Differentiate: f′(x)=12⋅4cos⁡(4x)=2cos⁡(4x)f'(x) = \frac{1}{2} \cdot 4 \cos(4x) = 2 \cos(4x). Matches.

Markers reward both methods reaching the same answer, with explicit use of cos⁡2−sin⁡2=cos⁡(2⋅angle)\cos^2 - \sin^2 = \cos(2 \cdot \text{angle}) in part (a). The verification in part (b) shows mathematical maturity and earns the final mark.

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