------- | ---------- | ------------------------------------------------------------------------ | | AQA | Paper 1, 2 | Basic” date: 2025-06-02T16:25:28.480Z tags:
Maths ALevel categories: Maths Intuition Trigonometry is the mathematics of rotation and oscillation: The unit circle is the key, as you rotate around it, the x x x -coordinate traces out cos θ \cos\theta cos θ and the y y y -coordinate traces out sin θ \sin\theta sin θ . This connects circular motion to wave patterns, which is why trigonometry appears in physics (waves, SHM), engineering (signal processing), and music (sound waves).
Why it matters: Trigonometry is essential for any problem involving angles, periodic phenomena, or circular motion. It’s the bridge between geometry (shapes) and algebra (equations), and it’s the foundation for calculus (differentiation/integration of trig functions).
The key insight: The identity sin 2 θ + cos 2 θ = 1 \sin^2\theta + \cos^2\theta = 1 sin 2 θ + cos 2 θ = 1 is just Pythagoras’ theorem applied to the unit circle. Every point on the unit circle satisfies x 2 + y 2 = 1 x^2 + y^2 = 1 x 2 + y 2 = 1 , and since x = cos θ x = \cos\theta x = cos θ and y = sin θ y = \sin\theta y = sin θ , the identity follows immediately. This is why trig identities are really just geometric relationships in disguise.
Board Coverage Board Paper Notes AQA Paper 1, 2 Basic trig in P1; compound/double angle, trig equations in P2 Edexcel P1, P2 Similar split OCR (A) Paper 1, 2 Includes small angle approximations CIE (9709) P1, P2, P3 Trig functions in P1; identities and equations in P2; further trig in P3
Note
All boards provide trigonometric identities in the formula booklet, but not their proofs.
You need to know which identities exist and how to apply them.
1. The Unit Circle Definitions Definition. Consider the unit circle (radius 1, centre at the origin). For an angle θ \theta θ Measured anticlockwise from the positive x x x -axis, the point on the circle is ( cos θ , sin θ ) (\cos\theta, \sin\theta) ( cos θ , sin θ ) .
Definition.
cos θ = t h e x − c o o r d i n a t e o f t h e p o i n t o n t h e u n i t c i r c l e a t a n g l e θ \cos\theta = \mathrm{the } x\mathrm{-coordinate of the point on the unit circle at angle } \theta cos θ = the x − coordinateofthepointontheunitcircleatangle θ sin θ = t h e y − c o o r d i n a t e o f t h e p o i n t o n t h e u n i t c i r c l e a t a n g l e θ \sin\theta = \mathrm{the } y\mathrm{-coordinate of the point on the unit circle at angle } \theta sin θ = the y − coordinateofthepointontheunitcircleatangle θ tan θ = sin θ cos θ ( cos θ ≠ 0 ) \tan\theta = \frac{\sin\theta}{\cos\theta} \quad (\cos\theta \neq 0) tan θ = cos θ sin θ ( cos θ = 0 ) Intuition. These definitions extend the right-triangle definitions (SOH CAH TOA) to all angles, Not just those between 0° and 90°. The unit circle makes clear why sin \sin sin and cos \cos cos are periodic with period 2 π 2\pi 2 π .
1.1 Radian Measure Definition. One radian is the angle subtended at the centre of a circle by an arc equal in Length to the radius.
θ ( r a d i a n s ) = a r c l e n g t h r \theta\mathrm{ (radians)} = \frac{\mathrm{arc length}}{r} θ ( radians ) = r arclength The full circle: 2 π 2\pi 2 π radians = 360 ∘ = 360^\circ = 36 0 ∘ So π \pi π radians = 180 ∘ = 180^\circ = 18 0 ∘ .
Theorem (Arc length and sector area). For a sector of radius r r r and angle θ \theta θ (in Radians):
A r c l e n g t h s = r θ \mathrm{Arc length } s = r\theta Arclength s = r θ S e c t o r a r e a A = 1 2 r 2 θ \mathrm{Sector area } A = \frac{1}{2}r^2\theta Sectorarea A = 2 1 r 2 θ Proof. By definition, θ = s / r \theta = s/r θ = s / r So s = r θ s = r\theta s = r θ . The sector is a fraction θ 2 π \frac{\theta}{2\pi} 2 π θ of the full circle (area π r 2 \pi r^2 π r 2 ), so A = θ 2 π ⋅ π r 2 = 1 2 r 2 θ A = \frac{\theta}{2\pi} \cdot \pi r^2 = \frac{1}{2}r^2\theta A = 2 π θ ⋅ π r 2 = 2 1 r 2 θ . ■ \blacksquare ■
2. Fundamental Identities 2.1 Pythagorean Identity Theorem. For all θ ∈ R \theta \in \mathbb{R} θ ∈ R :
sin 2 θ + cos 2 θ = 1 \sin^2\theta + \cos^2\theta = 1 sin 2 θ + cos 2 θ = 1 Proof. The point ( cos θ , sin θ ) (\cos\theta, \sin\theta) ( cos θ , sin θ ) lies on the unit circle x 2 + y 2 = 1 x^2 + y^2 = 1 x 2 + y 2 = 1 .
cos 2 θ + sin 2 θ = 1 ■ \cos^2\theta + \sin^2\theta = 1 \quad \blacksquare cos 2 θ + sin 2 θ = 1 ■ Corollary. Dividing by cos 2 θ \cos^2\theta cos 2 θ (where cos θ ≠ 0 \cos\theta \neq 0 cos θ = 0 ):
1 + tan 2 θ = sec 2 θ 1 + \tan^2\theta = \sec^2\theta 1 + tan 2 θ = sec 2 θ Dividing by sin 2 θ \sin^2\theta sin 2 θ (where sin θ ≠ 0 \sin\theta \neq 0 sin θ = 0 ):
cot 2 θ + 1 = cosec 2 θ \cot^2\theta + 1 = \cosec^2\theta cot 2 θ + 1 = cosec 2 θ 3.1 Sine of a Sum Theorem. For all A , B ∈ R A, B \in \mathbb{R} A , B ∈ R :
sin ( A + B ) = sin A cos B + cos A sin B \sin(A + B) = \sin A \cos B + \cos A \sin B sin ( A + B ) = sin A cos B + cos A sin B Proof (using rotation matrices). Consider the rotation of the plane by angle A A A followed by Rotation by angle B B B . The combined rotation is by angle A + B A + B A + B .
The rotation matrix by angle θ \theta θ is:
R ( θ ) = ( cos θ − sin θ sin θ cos θ ) R(\theta) = \begin{pmatrix} \cos\theta & -\sin\theta \\ \sin\theta & \cos\theta \end{pmatrix} R ( θ ) = ( cos θ sin θ − sin θ cos θ ) Matrix multiplication gives: R ( A ) R ( B ) = R ( A + B ) R(A)R(B) = R(A + B) R ( A ) R ( B ) = R ( A + B ) .
( cos A − sin A sin A cos A ) ( cos B − sin B sin B cos B ) = ( cos ( A + B ) − sin ( A + B ) sin ( A + B ) cos ( A + B ) ) \begin{pmatrix} \cos A & -\sin A \\ \sin A & \cos A \end{pmatrix}\begin{pmatrix} \cos B & -\sin B \\ \sin B & \cos B \end{pmatrix} = \begin{pmatrix} \cos(A+B) & -\sin(A+B) \\ \sin(A+B) & \cos(A+B) \end{pmatrix} ( cos A sin A − sin A cos A ) ( cos B sin B − sin B cos B ) = ( cos ( A + B ) sin ( A + B ) − sin ( A + B ) cos ( A + B ) ) The ( 2 , 1 ) (2, 1) ( 2 , 1 ) entry of the product is:
sin A cos B + cos A sin B = sin ( A + B ) ■ \sin A \cos B + \cos A \sin B = \sin(A + B) \quad \blacksquare sin A cos B + cos A sin B = sin ( A + B ) ■ 3.2 Cosine of a Sum Theorem.
cos ( A + B ) = cos A cos B − sin A sin B \cos(A + B) = \cos A \cos B - \sin A \sin B cos ( A + B ) = cos A cos B − sin A sin B Proof. From the ( 1 , 1 ) (1, 1) ( 1 , 1 ) entry of the matrix product above:
cos A cos B − sin A sin B = cos ( A + B ) ■ \cos A \cos B - \sin A \sin B = \cos(A + B) \quad \blacksquare cos A cos B − sin A sin B = cos ( A + B ) ■ 3.3 Tangent of a Sum Theorem.
tan ( A + B ) = tan A + tan B 1 − tan A tan B \tan(A + B) = \frac{\tan A + \tan B}{1 - \tan A \tan B} tan ( A + B ) = 1 − tan A tan B tan A + tan B Proof.
tan ( A + B ) = sin ( A + B ) cos ( A + B ) = sin A cos B + cos A sin B cos A cos B − sin A sin B \begin{aligned} \tan(A + B) &= \frac{\sin(A + B)}{\cos(A + B)} \\ &= \frac{\sin A \cos B + \cos A \sin B}{\cos A \cos B - \sin A \sin B} \end{aligned} tan ( A + B ) = cos ( A + B ) sin ( A + B ) = cos A cos B − sin A sin B sin A cos B + cos A sin B Divide numerator and denominator by cos A cos B \cos A \cos B cos A cos B :
= tan A + tan B 1 − tan A tan B ■ = \frac{\tan A + \tan B}{1 - \tan A \tan B} \quad \blacksquare = 1 − tan A tan B tan A + tan B ■ Theorem.
sin ( A − B ) = sin A cos B − cos A sin B cos ( A − B ) = cos A cos B + sin A sin B tan ( A − B ) = tan A − tan B 1 + tan A tan B \begin{aligned} \sin(A - B) &= \sin A \cos B - \cos A \sin B \\ \cos(A - B) &= \cos A \cos B + \sin A \sin B \\ \tan(A - B) &= \frac{\tan A - \tan B}{1 + \tan A \tan B} \end{aligned} sin ( A − B ) cos ( A − B ) tan ( A − B ) = sin A cos B − cos A sin B = cos A cos B + sin A sin B = 1 + tan A tan B tan A − tan B Proof. Replace B B B with − B -B − B in the sum formulas, using sin ( − B ) = − sin B \sin(-B) = -\sin B sin ( − B ) = − sin B and cos ( − B ) = cos B \cos(-B) = \cos B cos ( − B ) = cos B . ■ \blacksquare ■
Setting A = B A = B A = B in the compound angle formulas:
sin 2 A = 2 sin A cos A cos 2 A = cos 2 A − sin 2 A tan 2 A = 2 tan A 1 − tan 2 A \begin{aligned} \sin 2A &= 2\sin A \cos A \\ \cos 2A &= \cos^2 A - \sin^2 A \\ \tan 2A &= \frac{2\tan A}{1 - \tan^2 A} \end{aligned} sin 2 A cos 2 A tan 2 A = 2 sin A cos A = cos 2 A − sin 2 A = 1 − tan 2 A 2 tan A Theorem. Three equivalent forms of cos 2 A \cos 2A cos 2 A :
cos 2 A = cos 2 A − sin 2 A = 2 cos 2 A − 1 = 1 − 2 sin 2 A \cos 2A = \cos^2 A - \sin^2 A = 2\cos^2 A - 1 = 1 - 2\sin^2 A cos 2 A = cos 2 A − sin 2 A = 2 cos 2 A − 1 = 1 − 2 sin 2 A Proof. Using sin 2 A = 1 − cos 2 A \sin^2 A = 1 - \cos^2 A sin 2 A = 1 − cos 2 A :
cos 2 A − sin 2 A = cos 2 A − ( 1 − cos 2 A ) = 2 cos 2 A − 1 \cos^2 A - \sin^2 A = \cos^2 A - (1 - \cos^2 A) = 2\cos^2 A - 1 cos 2 A − sin 2 A = cos 2 A − ( 1 − cos 2 A ) = 2 cos 2 A − 1
Using cos 2 A = 1 − sin 2 A \cos^2 A = 1 - \sin^2 A cos 2 A = 1 − sin 2 A :
cos 2 A − sin 2 A = ( 1 − sin 2 A ) − sin 2 A = 1 − 2 sin 2 A \cos^2 A - \sin^2 A = (1 - \sin^2 A) - \sin^2 A = 1 - 2\sin^2 A cos 2 A − sin 2 A = ( 1 − sin 2 A ) − sin 2 A = 1 − 2 sin 2 A ■ \blacksquare ■
Intuition. The double angle formulas express functions of 2 A 2A 2 A purely in terms of functions of A A A . They are the algebraic backbone of many trigonometric manipulations and are essential for Integration.
5. Solving Trigonometric Equations 5.1 Basic Strategy Use identities to reduce to a single trigonometric function. Solve the resulting equation. Find all solutions in the required interval. 5.2 Key Solutions sin θ = a ⟹ θ = arcsin ( a ) + 2 n π o r π − arcsin ( a ) + 2 n π cos θ = a ⟹ θ = ± arccos ( a ) + 2 n π tan θ = a ⟹ θ = arctan ( a ) + n π \begin{aligned} \sin\theta = a &\implies \theta = \arcsin(a) + 2n\pi \mathrm{ or } \pi - \arcsin(a) + 2n\pi \\ \cos\theta = a &\implies \theta = \pm\arccos(a) + 2n\pi \\ \tan\theta = a &\implies \theta = \arctan(a) + n\pi \end{aligned} sin θ = a cos θ = a tan θ = a ⟹ θ = arcsin ( a ) + 2 nπ or π − arcsin ( a ) + 2 nπ ⟹ θ = ± arccos ( a ) + 2 nπ ⟹ θ = arctan ( a ) + nπ
Example Solve 2 sin 2 θ + 3 cos θ − 3 = 0 2\sin^2\theta + 3\cos\theta - 3 = 0 2 sin 2 θ + 3 cos θ − 3 = 0 for 0 ≤ θ < 2 π 0 \leq \theta < 2\pi 0 ≤ θ < 2 π .
Using sin 2 θ = 1 − cos 2 θ \sin^2\theta = 1 - \cos^2\theta sin 2 θ = 1 − cos 2 θ :
2 ( 1 − cos 2 θ ) + 3 cos θ − 3 = 0 2(1 - \cos^2\theta) + 3\cos\theta - 3 = 0 2 ( 1 − cos 2 θ ) + 3 cos θ − 3 = 0 − 2 cos 2 θ + 3 cos θ − 1 = 0 -2\cos^2\theta + 3\cos\theta - 1 = 0 − 2 cos 2 θ + 3 cos θ − 1 = 0 2 cos 2 θ − 3 cos θ + 1 = 0 2\cos^2\theta - 3\cos\theta + 1 = 0 2 cos 2 θ − 3 cos θ + 1 = 0 ( 2 cos θ − 1 ) ( cos θ − 1 ) = 0 (2\cos\theta - 1)(\cos\theta - 1) = 0 ( 2 cos θ − 1 ) ( cos θ − 1 ) = 0 cos θ = 1 2 ⟹ θ = π 3 \cos\theta = \frac{1}{2} \implies \theta = \frac{\pi}{3} cos θ = 2 1 ⟹ θ = 3 π or 5 π 3 \frac{5\pi}{3} 3 5 π .
cos θ = 1 ⟹ θ = 0 \cos\theta = 1 \implies \theta = 0 cos θ = 1 ⟹ θ = 0 .
Solutions: θ = 0 , π 3 , 5 π 3 \theta = 0, \frac{\pi}{3}, \frac{5\pi}{3} θ = 0 , 3 π , 3 5 π .
6. Small Angle Approximations Theorem. For small θ \theta θ (in radians):
sin θ ≈ θ − θ 3 6 cos θ ≈ 1 − θ 2 2 tan θ ≈ θ + θ 3 3 \begin{aligned} \sin\theta &\approx \theta - \frac{\theta^3}{6} \\ \cos\theta &\approx 1 - \frac{\theta^2}{2} \\ \tan\theta &\approx \theta + \frac{\theta^3}{3} \end{aligned} sin θ cos θ tan θ ≈ θ − 6 θ 3 ≈ 1 − 2 θ 2 ≈ θ + 3 θ 3 These follow from the Maclaurin series expansions (see Differentiation ).
For the linear approximations (when θ \theta θ is very small):
sin θ ≈ θ , cos θ ≈ 1 , tan θ ≈ θ \sin\theta \approx \theta, \quad \cos\theta \approx 1, \quad \tan\theta \approx \theta sin θ ≈ θ , cos θ ≈ 1 , tan θ ≈ θ Intuition. Near the origin, the curves y = sin θ y = \sin\theta y = sin θ and y = tan θ y = \tan\theta y = tan θ are almost Indistinguishable from the line y = θ y = \theta y = θ . The curve y = cos θ y = \cos\theta y = cos θ is nearly flat at y = 1 y = 1 y = 1 .
Caution
The small angle approximations are only valid when θ \theta θ is in radians , not
Degrees. This is a very common exam error.
Theorem. For all θ \theta θ :
sin θ 2 = ± 1 − cos θ 2 \sin\frac{\theta}{2} = \pm\sqrt{\frac{1 - \cos\theta}{2}} sin 2 θ = ± 2 1 − cos θ cos θ 2 = ± 1 + cos θ 2 \cos\frac{\theta}{2} = \pm\sqrt{\frac{1 + \cos\theta}{2}} cos 2 θ = ± 2 1 + cos θ tan θ 2 = sin θ 1 + cos θ = 1 − cos θ sin θ \tan\frac{\theta}{2} = \frac{\sin\theta}{1 + \cos\theta} = \frac{1 - \cos\theta}{\sin\theta} tan 2 θ = 1 + cos θ sin θ = sin θ 1 − cos θ 7.1 Derivation Starting from cos 2 A = 1 − 2 sin 2 A \cos 2A = 1 - 2\sin^2 A cos 2 A = 1 − 2 sin 2 A and substituting A = θ 2 A = \frac{\theta}{2} A = 2 θ :
cos θ = 1 − 2 sin 2 θ 2 \cos\theta = 1 - 2\sin^2\frac{\theta}{2} cos θ = 1 − 2 sin 2 2 θ 2 sin 2 θ 2 = 1 − cos θ 2\sin^2\frac{\theta}{2} = 1 - \cos\theta 2 sin 2 2 θ = 1 − cos θ sin θ 2 = ± 1 − cos θ 2 ■ \sin\frac{\theta}{2} = \pm\sqrt{\frac{1 - \cos\theta}{2}} \quad \blacksquare sin 2 θ = ± 2 1 − cos θ ■ Similarly, from cos 2 A = 2 cos 2 A − 1 \cos 2A = 2\cos^2 A - 1 cos 2 A = 2 cos 2 A − 1 :
cos θ = 2 cos 2 θ 2 − 1 \cos\theta = 2\cos^2\frac{\theta}{2} - 1 cos θ = 2 cos 2 2 θ − 1 2 cos 2 θ 2 = 1 + cos θ 2\cos^2\frac{\theta}{2} = 1 + \cos\theta 2 cos 2 2 θ = 1 + cos θ cos θ 2 = ± 1 + cos θ 2 ■ \cos\frac{\theta}{2} = \pm\sqrt{\frac{1 + \cos\theta}{2}} \quad \blacksquare cos 2 θ = ± 2 1 + cos θ ■ The tangent half-angle formulas avoid the ambiguity of the ± \pm ± sign:
tan θ 2 = sin θ 1 + cos θ \tan\frac{\theta}{2} = \frac{\sin\theta}{1 + \cos\theta} tan 2 θ = 1 + cos θ sin θ Proof. Using the double angle formulas:
sin θ 1 + cos θ = 2 sin θ 2 cos θ 2 1 + ( 2 cos 2 θ 2 − 1 ) = 2 sin θ 2 cos θ 2 2 cos 2 θ 2 = sin θ 2 cos θ 2 = tan θ 2 ■ \frac{\sin\theta}{1 + \cos\theta} = \frac{2\sin\frac{\theta}{2}\cos\frac{\theta}{2}}{1 + (2\cos^2\frac{\theta}{2} - 1)} = \frac{2\sin\frac{\theta}{2}\cos\frac{\theta}{2}}{2\cos^2\frac{\theta}{2}} = \frac{\sin\frac{\theta}{2}}{\cos\frac{\theta}{2}} = \tan\frac{\theta}{2} \quad \blacksquare 1 + cos θ sin θ = 1 + ( 2 cos 2 2 θ − 1 ) 2 sin 2 θ cos 2 θ = 2 cos 2 2 θ 2 sin 2 θ cos 2 θ = cos 2 θ sin 2 θ = tan 2 θ ■ Similarly:
tan θ 2 = 1 − cos θ sin θ \tan\frac{\theta}{2} = \frac{1 - \cos\theta}{\sin\theta} tan 2 θ = sin θ 1 − cos θ Proof. 1 − cos θ sin θ = 1 − ( 1 − 2 sin 2 θ 2 ) 2 sin θ 2 cos θ 2 = 2 sin 2 θ 2 2 sin θ 2 cos θ 2 = sin θ 2 cos θ 2 = tan θ 2 ■ \frac{1 - \cos\theta}{\sin\theta} = \frac{1 - (1 - 2\sin^2\frac{\theta}{2})}{2\sin\frac{\theta}{2}\cos\frac{\theta}{2}} = \frac{2\sin^2\frac{\theta}{2}}{2\sin\frac{\theta}{2}\cos\frac{\theta}{2}} = \frac{\sin\frac{\theta}{2}}{\cos\frac{\theta}{2}} = \tan\frac{\theta}{2} \quad \blacksquare s i n θ 1 − c o s θ = 2 s i n 2 θ c o s 2 θ 1 − ( 1 − 2 s i n 2 2 θ ) = 2 s i n 2 θ c o s 2 θ 2 s i n 2 2 θ = c o s 2 θ s i n 2 θ = tan 2 θ ■
7.3 Sign Determination The ± \pm ± in the sine and cosine half-angle formulas depends on the quadrant of θ 2 \frac{\theta}{2} 2 θ Not the quadrant of θ \theta θ itself. Always determine which quadrant θ 2 \frac{\theta}{2} 2 θ lies in Before choosing the sign.
Quadrant of θ 2 \frac{\theta}{2} 2 θ sin θ 2 \sin\frac{\theta}{2} sin 2 θ cos θ 2 \cos\frac{\theta}{2} cos 2 θ I: 0 < θ 2 < π 2 0 \lt \frac{\theta}{2} \lt \frac{\pi}{2} 0 < 2 θ < 2 π + + + + + + II: π 2 < θ 2 < π \frac{\pi}{2} \lt \frac{\theta}{2} \lt \pi 2 π < 2 θ < π + + + − - − III: π < θ 2 < 3 π 2 \pi \lt \frac{\theta}{2} \lt \frac{3\pi}{2} π < 2 θ < 2 3 π − - − − - − IV: 3 π 2 < θ 2 < 2 π \frac{3\pi}{2} \lt \frac{\theta}{2} \lt 2\pi 2 3 π < 2 θ < 2 π − - − + + +
Worked example Find the exact value of sin π 8 \sin\frac{\pi}{8} sin 8 π .
Since 0 < π 8 < π 2 0 \lt \frac{\pi}{8} \lt \frac{\pi}{2} 0 < 8 π < 2 π (first quadrant), sin π 8 > 0 \sin\frac{\pi}{8} > 0 sin 8 π > 0 So we Take the positive root.
sin π 8 = 1 − cos π 4 2 = 1 − 2 2 2 = 2 − 2 4 = 2 − 2 2 \sin\frac{\pi}{8} = \sqrt{\frac{1 - \cos\frac{\pi}{4}}{2}} = \sqrt{\frac{1 - \frac{\sqrt{2}}{2}}{2}} = \sqrt{\frac{2 - \sqrt{2}}{4}} = \frac{\sqrt{2 - \sqrt{2}}}{2} sin 8 π = 2 1 − cos 4 π = 2 1 − 2 2 = 4 2 − 2 = 2 2 − 2 Theorem. For real numbers a a a and b b b :
a sin θ + b cos θ = R sin ( θ + α ) a\sin\theta + b\cos\theta = R\sin(\theta + \alpha) a sin θ + b cos θ = R sin ( θ + α ) Where R = a 2 + b 2 R = \sqrt{a^2 + b^2} R = a 2 + b 2 and tan α = b a \tan\alpha = \dfrac{b}{a} tan α = a b .
Alternatively, the same expression can be written as:
a sin θ + b cos θ = R cos ( θ − β ) a\sin\theta + b\cos\theta = R\cos(\theta - \beta) a sin θ + b cos θ = R cos ( θ − β ) Where R = a 2 + b 2 R = \sqrt{a^2 + b^2} R = a 2 + b 2 and tan β = a b \tan\beta = \dfrac{a}{b} tan β = b a .
Both forms are equivalent; the choice between them is a matter of convenience depending on whether a Sine or cosine expansion is more natural for the problem at hand.
8.2 Derivation Expand the right-hand side of the sine form:
R sin ( θ + α ) = R sin θ cos α + R cos θ sin α R\sin(\theta + \alpha) = R\sin\theta\cos\alpha + R\cos\theta\sin\alpha R sin ( θ + α ) = R sin θ cos α + R cos θ sin α Equating coefficients with a sin θ + b cos θ a\sin\theta + b\cos\theta a sin θ + b cos θ :
R cos α = a , R sin α = b R\cos\alpha = a, \qquad R\sin\alpha = b R cos α = a , R sin α = b Squaring and adding: R 2 cos 2 α + R 2 sin 2 α = a 2 + b 2 R^2\cos^2\alpha + R^2\sin^2\alpha = a^2 + b^2 R 2 cos 2 α + R 2 sin 2 α = a 2 + b 2 So R 2 = a 2 + b 2 R^2 = a^2 + b^2 R 2 = a 2 + b 2 and R = a 2 + b 2 R = \sqrt{a^2 + b^2} R = a 2 + b 2 .
Dividing the second equation by the first: tan α = b a \tan\alpha = \dfrac{b}{a} tan α = a b . ■ \blacksquare ■
The cosine form is derived similarly by expanding R cos ( θ − β ) = R cos θ cos β + R sin θ sin β R\cos(\theta - \beta) = R\cos\theta\cos\beta + R\sin\theta\sin\beta R cos ( θ − β ) = R cos θ cos β + R sin θ sin β and equating coefficients.
8.3 Applications: Maximum and Minimum Since − 1 ≤ sin ( θ + α ) ≤ 1 -1 \leq \sin(\theta + \alpha) \leq 1 − 1 ≤ sin ( θ + α ) ≤ 1 :
− R ≤ a sin θ + b cos θ ≤ R -R \leq a\sin\theta + b\cos\theta \leq R − R ≤ a sin θ + b cos θ ≤ R Maximum = R = a 2 + b 2 = R = \sqrt{a^2 + b^2} = R = a 2 + b 2 Occurring when θ + α = π 2 + 2 n π \theta + \alpha = \frac{\pi}{2} + 2n\pi θ + α = 2 π + 2 nπ .Minimum = − R = -R = − R Occurring when θ + α = 3 π 2 + 2 n π \theta + \alpha = \frac{3\pi}{2} + 2n\pi θ + α = 2 3 π + 2 nπ .
Example: Finding maximum and minimum Find the maximum and minimum values of 3 sin θ − 4 cos θ 3\sin\theta - 4\cos\theta 3 sin θ − 4 cos θ and the values of θ \theta θ at which they occur, for 0 ≤ θ < 2 π 0 \leq \theta \lt 2\pi 0 ≤ θ < 2 π .
R = 9 + 16 = 5 R = \sqrt{9 + 16} = 5 R = 9 + 16 = 5 .
Here a = 3 a = 3 a = 3 and b = − 4 b = -4 b = − 4 . Writing 3 sin θ − 4 cos θ = 5 sin ( θ + α ) 3\sin\theta - 4\cos\theta = 5\sin(\theta + \alpha) 3 sin θ − 4 cos θ = 5 sin ( θ + α ) where tan α = − 4 3 \tan\alpha = \dfrac{-4}{3} tan α = 3 − 4 So α = − arctan 4 3 \alpha = -\arctan\dfrac{4}{3} α = − arctan 3 4 .
Maximum = 5 = 5 = 5 when θ + α = π 2 \theta + \alpha = \frac{\pi}{2} θ + α = 2 π :
θ = π 2 − α = π 2 + arctan 4 3 ≈ 2.214 r a d \theta = \frac{\pi}{2} - \alpha = \frac{\pi}{2} + \arctan\frac{4}{3} \approx 2.214 \mathrm{ rad} θ = 2 π − α = 2 π + arctan 3 4 ≈ 2.214 rad Minimum = − 5 = -5 = − 5 when θ + α = 3 π 2 \theta + \alpha = \frac{3\pi}{2} θ + α = 2 3 π :
θ = 3 π 2 − α = 3 π 2 + arctan 4 3 ≈ 5.356 r a d \theta = \frac{3\pi}{2} - \alpha = \frac{3\pi}{2} + \arctan\frac{4}{3} \approx 5.356 \mathrm{ rad} θ = 2 3 π − α = 2 3 π + arctan 3 4 ≈ 5.356 rad 8.4 Solving Equations The R-addition formula converts a sin θ + b cos θ = k a\sin\theta + b\cos\theta = k a sin θ + b cos θ = k into R sin ( θ + α ) = k R\sin(\theta + \alpha) = k R sin ( θ + α ) = k A Standard trigonometric equation.
Example: Solving an equation Solve sin θ + cos θ = 1 \sin\theta + \cos\theta = 1 sin θ + cos θ = 1 for 0 ≤ θ < 2 π 0 \leq \theta \lt 2\pi 0 ≤ θ < 2 π .
R = 1 + 1 = 2 R = \sqrt{1 + 1} = \sqrt{2} R = 1 + 1 = 2 , α = arctan 1 = π 4 \alpha = \arctan 1 = \frac{\pi}{4} α = arctan 1 = 4 π .
2 sin ( θ + π 4 ) = 1 \sqrt{2}\sin\!\left(\theta + \frac{\pi}{4}\right) = 1 2 sin ( θ + 4 π ) = 1 sin ( θ + π 4 ) = 1 2 = sin π 4 \sin\!\left(\theta + \frac{\pi}{4}\right) = \frac{1}{\sqrt{2}} = \sin\frac{\pi}{4} sin ( θ + 4 π ) = 2 1 = sin 4 π θ + π 4 = π 4 + 2 n π o r θ + π 4 = 3 π 4 + 2 n π \theta + \frac{\pi}{4} = \frac{\pi}{4} + 2n\pi \quad \mathrm{or} \quad \theta + \frac{\pi}{4} = \frac{3\pi}{4} + 2n\pi θ + 4 π = 4 π + 2 nπ or θ + 4 π = 4 3 π + 2 nπ θ = 2 n π o r θ = π 2 + 2 n π \theta = 2n\pi \quad \mathrm{or} \quad \theta = \frac{\pi}{2} + 2n\pi θ = 2 nπ or θ = 2 π + 2 nπ For 0 ≤ θ < 2 π 0 \leq \theta \lt 2\pi 0 ≤ θ < 2 π : θ = 0 \theta = 0 θ = 0 or θ = π 2 \theta = \frac{\pi}{2} θ = 2 π .
9. Trigonometric Identities: Proof Strategies Proving trigonometric identities is a core exam skill. The following strategies cover the most Common approaches.
9.1 Strategy 1: Work with One Side Start from the more complicated side and simplify it until it matches the simpler side. This avoids the logical error of assuming what you are trying to prove.
9.2 Strategy 2: Express Everything in Sine and Cosine Replace tan \tan tan , sec \sec sec , csc \csc csc , cot \cot cot with their definitions in terms of sin \sin sin and cos \cos cos : tan θ = sin θ cos θ \tan\theta = \frac{\sin\theta}{\cos\theta} tan θ = c o s θ s i n θ , sec θ = 1 cos θ \sec\theta = \frac{1}{\cos\theta} sec θ = c o s θ 1 Etc.
9.3 Strategy 3: Use Known Identities Apply the Pythagorean identity, compound angle, or double angle formulas to create simplifications.
9.4 Strategy 4: Multiply by the Conjugate When you see expressions of the form a ± b a \pm b a ± b in a denominator or numerator, multiply top and Bottom by the conjugate a ∓ b a \mp b a ∓ b to produce a difference of squares.
Example 1: Strategy 2 (express in sin and cos) Prove that cot A + tan A = 2 sin 2 A \cot A + \tan A = \dfrac{2}{\sin 2A} cot A + tan A = sin 2 A 2 .
cot A + tan A = cos A sin A + sin A cos A = cos 2 A + sin 2 A sin A cos A = 1 sin A cos A = 2 2 sin A cos A = 2 sin 2 A ■ \begin{aligned} \cot A + \tan A &= \frac{\cos A}{\sin A} + \frac{\sin A}{\cos A} \\ &= \frac{\cos^2 A + \sin^2 A}{\sin A \cos A} \\ &= \frac{1}{\sin A \cos A} \\ &= \frac{2}{2\sin A \cos A} = \frac{2}{\sin 2A} \quad \blacksquare \end{aligned} cot A + tan A = sin A cos A + cos A sin A = sin A cos A cos 2 A + sin 2 A = sin A cos A 1 = 2 sin A cos A 2 = sin 2 A 2 ■
Example 2: Strategy 3 (use known identities) Prove that sin 3 A = 3 sin A − 4 sin 3 A \sin 3A = 3\sin A - 4\sin^3 A sin 3 A = 3 sin A − 4 sin 3 A .
sin 3 A = sin ( 2 A + A ) = sin 2 A cos A + cos 2 A sin A = 2 sin A cos 2 A + ( 1 − 2 sin 2 A ) sin A = 2 sin A ( 1 − sin 2 A ) + sin A − 2 sin 3 A = 2 sin A − 2 sin 3 A + sin A − 2 sin 3 A = 3 sin A − 4 sin 3 A ■ \begin{aligned} \sin 3A &= \sin(2A + A) \\ &= \sin 2A \cos A + \cos 2A \sin A \\ &= 2\sin A \cos^2 A + (1 - 2\sin^2 A)\sin A \\ &= 2\sin A(1 - \sin^2 A) + \sin A - 2\sin^3 A \\ &= 2\sin A - 2\sin^3 A + \sin A - 2\sin^3 A \\ &= 3\sin A - 4\sin^3 A \quad \blacksquare \end{aligned} sin 3 A = sin ( 2 A + A ) = sin 2 A cos A + cos 2 A sin A = 2 sin A cos 2 A + ( 1 − 2 sin 2 A ) sin A = 2 sin A ( 1 − sin 2 A ) + sin A − 2 sin 3 A = 2 sin A − 2 sin 3 A + sin A − 2 sin 3 A = 3 sin A − 4 sin 3 A ■
Example 3: Strategy 4 (multiply by conjugate) Prove that 1 sec A + tan A = sec A − tan A \dfrac{1}{\sec A + \tan A} = \sec A - \tan A sec A + tan A 1 = sec A − tan A .
Multiply numerator and denominator by sec A − tan A \sec A - \tan A sec A − tan A :
1 sec A + tan A ⋅ sec A − tan A sec A − tan A = sec A − tan A sec 2 A − tan 2 A = sec A − tan A 1 + tan 2 A − tan 2 A = sec A − tan A 1 = sec A − tan A ■ \begin{aligned} \frac{1}{\sec A + \tan A} \cdot \frac{\sec A - \tan A}{\sec A - \tan A} &= \frac{\sec A - \tan A}{\sec^2 A - \tan^2 A} \\ &= \frac{\sec A - \tan A}{1 + \tan^2 A - \tan^2 A} \\ &= \frac{\sec A - \tan A}{1} \\ &= \sec A - \tan A \quad \blacksquare \end{aligned} sec A + tan A 1 ⋅ sec A − tan A sec A − tan A = sec 2 A − tan 2 A sec A − tan A = 1 + tan 2 A − tan 2 A sec A − tan A = 1 sec A − tan A = sec A − tan A ■ Where we used sec 2 A = 1 + tan 2 A \sec^2 A = 1 + \tan^2 A sec 2 A = 1 + tan 2 A so that sec 2 A − tan 2 A = 1 \sec^2 A - \tan^2 A = 1 sec 2 A − tan 2 A = 1 .
Example 4: Strategy 1 (work with one side) Prove that cos 2 A 1 + sin 2 A = cos A − sin A cos A + sin A \dfrac{\cos 2A}{1 + \sin 2A} = \dfrac{\cos A - \sin A}{\cos A + \sin A} 1 + sin 2 A cos 2 A = cos A + sin A cos A − sin A .
Working from the LHS:
cos 2 A 1 + sin 2 A = cos 2 A − sin 2 A 1 + 2 sin A cos A = ( cos A − sin A ) ( cos A + sin A ) cos 2 A + 2 sin A cos A + sin 2 A = ( cos A − sin A ) ( cos A + sin A ) ( cos A + sin A ) 2 = cos A − sin A cos A + sin A ■ \begin{aligned} \frac{\cos 2A}{1 + \sin 2A} &= \frac{\cos^2 A - \sin^2 A}{1 + 2\sin A \cos A} \\ &= \frac{(\cos A - \sin A)(\cos A + \sin A)}{\cos^2 A + 2\sin A\cos A + \sin^2 A} \\ &= \frac{(\cos A - \sin A)(\cos A + \sin A)}{(\cos A + \sin A)^2} \\ &= \frac{\cos A - \sin A}{\cos A + \sin A} \quad \blacksquare \end{aligned} 1 + sin 2 A cos 2 A = 1 + 2 sin A cos A cos 2 A − sin 2 A = cos 2 A + 2 sin A cos A + sin 2 A ( cos A − sin A ) ( cos A + sin A ) = ( cos A + sin A ) 2 ( cos A − sin A ) ( cos A + sin A ) = cos A + sin A cos A − sin A ■ 10. Trigonometric Graphs 10.1 Key Features Function Period Amplitude Domain Range sin x \sin x sin x 2 π 2\pi 2 π 1 1 1 R \mathbb{R} R [ − 1 , 1 ] [-1, 1] [ − 1 , 1 ] cos x \cos x cos x 2 π 2\pi 2 π 1 1 1 R \mathbb{R} R [ − 1 , 1 ] [-1, 1] [ − 1 , 1 ] tan x \tan x tan x π \pi π undefined x ≠ π 2 + n π x \neq \frac{\pi}{2} + n\pi x = 2 π + nπ R \mathbb{R} R
Key values of sin \sin sin and cos \cos cos :
Angle 0 0 0 π 6 \frac{\pi}{6} 6 π π 4 \frac{\pi}{4} 4 π π 3 \frac{\pi}{3} 3 π π 2 \frac{\pi}{2} 2 π π \pi π 3 π 2 \frac{3\pi}{2} 2 3 π 2 π 2\pi 2 π sin \sin sin 0 0 0 1 2 \frac{1}{2} 2 1 2 2 \frac{\sqrt{2}}{2} 2 2 3 2 \frac{\sqrt{3}}{2} 2 3 1 1 1 0 0 0 − 1 -1 − 1 0 0 0 cos \cos cos 1 1 1 3 2 \frac{\sqrt{3}}{2} 2 3 2 2 \frac{\sqrt{2}}{2} 2 2 1 2 \frac{1}{2} 2 1 0 0 0 − 1 -1 − 1 0 0 0 1 1 1
For the general form y = A sin ( B x + C ) + D y = A\sin(Bx + C) + D y = A sin ( B x + C ) + D (and similarly for cos \cos cos ):
∣ A ∣ |A| ∣ A ∣ is the amplitude (vertical stretch from the midline)The period is 2 π ∣ B ∣ \dfrac{2\pi}{|B|} ∣ B ∣ 2 π The phase shift is − C B -\dfrac{C}{B} − B C (horizontal shift) D D D is the vertical shift (midline is y = D y = D y = D )For tan \tan tan The period is π ∣ B ∣ \dfrac{\pi}{|B|} ∣ B ∣ π and amplitude is not defined.
Use the sliders to adjust the amplitude, period, phase shift, and Vertical translation of the trigonometric functions. Observe how each parameter affects the graph of y = A sin ( B x + C ) + D y = A\sin(Bx + C) + D y = A sin ( B x + C ) + D .
Worked example Describe the key features of y = 2 sin ( 2 x − π 3 ) y = 2\sin\!\left(2x - \frac{\pi}{3}\right) y = 2 sin ( 2 x − 3 π ) for 0 ≤ x ≤ 2 π 0 \leq x \leq 2\pi 0 ≤ x ≤ 2 π . Amplitude: ∣ A ∣ = 2 |A| = 2 ∣ A ∣ = 2 So the range is [ − 2 , 2 ] [-2, 2] [ − 2 , 2 ] . Period: 2 π ∣ B ∣ = 2 π 2 = π \dfrac{2\pi}{|B|} = \dfrac{2\pi}{2} = \pi ∣ B ∣ 2 π = 2 2 π = π . Phase shift: − C B = − − π / 3 2 = π 6 -\dfrac{C}{B} = -\dfrac{-\pi/3}{2} = \dfrac{\pi}{6} − B C = − 2 − π /3 = 6 π (shift right by π 6 \frac{\pi}{6} 6 π ). Key points. The first cycle begins at x = π 6 x = \frac{\pi}{6} x = 6 π (where the curve crosses the midline Upward). Subsequent key points within [ 0 , 2 π ] [0, 2\pi] [ 0 , 2 π ] : - Maximum at x = 5 π 12 x = \frac{5\pi}{12} x = 12 5 π (value 2 2 2 ) - Midline crossing (down) at x = 2 π 3 x = \frac{2\pi}{3} x = 3 2 π - Minimum at x = 11 π 12 x = \frac{11\pi}{12} x = 12 11 π (value − 2 -2 − 2 ) - Midline crossing (up) at x = 7 π 6 x = \frac{7\pi}{6} x = 6 7 π Since the period is π \pi π The second cycle repeats with all x x x -values shifted by π \pi π : - Maximum at x = 17 π 12 x = \frac{17\pi}{12} x = 12 17 π (value 2 2 2 ) - Minimum at x = 23 π 12 x = \frac{23\pi}{12} x = 12 23 π (value − 2 -2 − 2 ) y y y -intercept: y = 2 sin ( − π 3 ) = − 3 ≈ − 1.73 y = 2\sin\!\left(-\frac{\pi}{3}\right) = -\sqrt{3} \approx -1.73 y = 2 sin ( − 3 π ) = − 3 ≈ − 1.73 .
11. Problem Set Problem 1. Prove that sin 2 θ 1 + cos 2 θ = tan θ \frac{\sin 2\theta}{1 + \cos 2\theta} = \tan\theta 1 + c o s 2 θ s i n 2 θ = tan θ .
Solution sin 2 θ 1 + cos 2 θ = 2 sin θ cos θ 1 + ( 2 cos 2 θ − 1 ) = 2 sin θ cos θ 2 cos 2 θ = sin θ cos θ = tan θ ■ \begin{aligned} \frac{\sin 2\theta}{1 + \cos 2\theta} &= \frac{2\sin\theta\cos\theta}{1 + (2\cos^2\theta - 1)} \\ &= \frac{2\sin\theta\cos\theta}{2\cos^2\theta} \\ &= \frac{\sin\theta}{\cos\theta} = \tan\theta \quad \blacksquare \end{aligned} 1 + cos 2 θ sin 2 θ = 1 + ( 2 cos 2 θ − 1 ) 2 sin θ cos θ = 2 cos 2 θ 2 sin θ cos θ = cos θ sin θ = tan θ ■ If you get this wrong, revise: Double angle formulas
Problem 2. Solve sin 2 x = sin x \sin 2x = \sin x sin 2 x = sin x for 0 ≤ x < 2 π 0 \leq x < 2\pi 0 ≤ x < 2 π .
Solution 2 sin x cos x = sin x 2\sin x\cos x = \sin x 2 sin x cos x = sin x sin x ( 2 cos x − 1 ) = 0 \sin x(2\cos x - 1) = 0 sin x ( 2 cos x − 1 ) = 0 sin x = 0 ⟹ x = 0 , π \sin x = 0 \implies x = 0, \pi sin x = 0 ⟹ x = 0 , π .
2 cos x − 1 = 0 ⟹ cos x = 1 2 ⟹ x = π 3 , 5 π 3 2\cos x - 1 = 0 \implies \cos x = \frac{1}{2} \implies x = \frac{\pi}{3}, \frac{5\pi}{3} 2 cos x − 1 = 0 ⟹ cos x = 2 1 ⟹ x = 3 π , 3 5 π .
Solutions: x = 0 , π 3 , π , 5 π 3 x = 0, \frac{\pi}{3}, \pi, \frac{5\pi}{3} x = 0 , 3 π , π , 3 5 π .
If you get this wrong, revise: Solving trig equations
Problem 3. Express 4 sin θ − 3 cos θ 4\sin\theta - 3\cos\theta 4 sin θ − 3 cos θ in the form R sin ( θ − α ) R\sin(\theta - \alpha) R sin ( θ − α ) Where R > 0 R > 0 R > 0 and 0 < α < π 2 0 < \alpha < \frac{\pi}{2} 0 < α < 2 π .
Solution R sin ( θ − α ) = R ( sin θ cos α − cos θ sin α ) = R cos α sin θ − R sin α cos θ R\sin(\theta - \alpha) = R(\sin\theta\cos\alpha - \cos\theta\sin\alpha) = R\cos\alpha\sin\theta - R\sin\alpha\cos\theta R sin ( θ − α ) = R ( sin θ cos α − cos θ sin α ) = R cos α sin θ − R sin α cos θ .
Comparing coefficients: R cos α = 4 R\cos\alpha = 4 R cos α = 4 and R sin α = 3 R\sin\alpha = 3 R sin α = 3 .
R 2 = 4 2 + 3 2 = 25 ⟹ R = 5 R^2 = 4^2 + 3^2 = 25 \implies R = 5 R 2 = 4 2 + 3 2 = 25 ⟹ R = 5 tan α = 3 4 ⟹ α = arctan ( 3 4 ) ≈ 0.6435 r a d \tan\alpha = \frac{3}{4} \implies \alpha = \arctan\left(\frac{3}{4}\right) \approx 0.6435 \mathrm{ rad} tan α = 4 3 ⟹ α = arctan ( 4 3 ) ≈ 0.6435 rad 4 sin θ − 3 cos θ = 5 sin ( θ − 0.6435 ) 4\sin\theta - 3\cos\theta = 5\sin(\theta - 0.6435) 4 sin θ − 3 cos θ = 5 sin ( θ − 0.6435 ) If you get this wrong, revise: Compound angle formulas
Problem 4. Find the exact value of sin 75 ∘ \sin 75^\circ sin 7 5 ∘ .
Solution sin 75 ° = sin ( 45 ° + 30 ° ) = sin 45 ° cos 30 ° + cos 45 ° sin 30 ∘ \sin 75° = \sin(45° + 30°) = \sin 45°\cos 30° + \cos 45°\sin 30^\circ sin 75° = sin ( 45° + 30° ) = sin 45° cos 30° + cos 45° sin 3 0 ∘ = 2 2 ⋅ 3 2 + 2 2 ⋅ 1 2 = 6 + 2 4 = \frac{\sqrt{2}}{2} \cdot \frac{\sqrt{3}}{2} + \frac{\sqrt{2}}{2} \cdot \frac{1}{2} = \frac{\sqrt{6} + \sqrt{2}}{4} = 2 2 ⋅ 2 3 + 2 2 ⋅ 2 1 = 4 6 + 2 If you get this wrong, revise: Compound angle formulas
Problem 5. Prove that 1 − cos 2 θ sin 2 θ = tan θ \frac{1 - \cos 2\theta}{\sin 2\theta} = \tan\theta s i n 2 θ 1 − c o s 2 θ = tan θ .
Solution 1 − cos 2 θ sin 2 θ = 1 − ( 1 − 2 sin 2 θ ) 2 sin θ cos θ = 2 sin 2 θ 2 sin θ cos θ = sin θ cos θ = tan θ ■ \begin{aligned} \frac{1 - \cos 2\theta}{\sin 2\theta} &= \frac{1 - (1 - 2\sin^2\theta)}{2\sin\theta\cos\theta} \\ &= \frac{2\sin^2\theta}{2\sin\theta\cos\theta} \\ &= \frac{\sin\theta}{\cos\theta} = \tan\theta \quad \blacksquare \end{aligned} sin 2 θ 1 − cos 2 θ = 2 sin θ cos θ 1 − ( 1 − 2 sin 2 θ ) = 2 sin θ cos θ 2 sin 2 θ = cos θ sin θ = tan θ ■ If you get this wrong, revise: Double angle formulas
Problem 6. A sector of a circle of radius 8 cm has an angle of 1.2 radians. Find the arc length And the area of the sector.
Solution Arc length: s = r θ = 8 × 1.2 = 9.6 s = r\theta = 8 \times 1.2 = 9.6 s = r θ = 8 × 1.2 = 9.6 cm.
Area: A = 1 2 r 2 θ = 1 2 ( 64 ) ( 1.2 ) = 38.4 A = \frac{1}{2}r^2\theta = \frac{1}{2}(64)(1.2) = 38.4 A = 2 1 r 2 θ = 2 1 ( 64 ) ( 1.2 ) = 38.4 cm².
If you get this wrong, revise: Radian measure
Problem 7. Solve 3 cos 2 x + 2 sin x − 2 = 0 3\cos^2 x + 2\sin x - 2 = 0 3 cos 2 x + 2 sin x − 2 = 0 for − π ≤ x ≤ π -\pi \leq x \leq \pi − π ≤ x ≤ π .
Solution 3 ( 1 − sin 2 x ) + 2 sin x − 2 = 0 3(1 - \sin^2 x) + 2\sin x - 2 = 0 3 ( 1 − sin 2 x ) + 2 sin x − 2 = 0
3 − 3 sin 2 x + 2 sin x − 2 = 0 3 - 3\sin^2 x + 2\sin x - 2 = 0 3 − 3 sin 2 x + 2 sin x − 2 = 0
− 3 sin 2 x + 2 sin x + 1 = 0 -3\sin^2 x + 2\sin x + 1 = 0 − 3 sin 2 x + 2 sin x + 1 = 0
3 sin 2 x − 2 sin x − 1 = 0 3\sin^2 x - 2\sin x - 1 = 0 3 sin 2 x − 2 sin x − 1 = 0
( 3 sin x + 1 ) ( sin x − 1 ) = 0 (3\sin x + 1)(\sin x - 1) = 0 ( 3 sin x + 1 ) ( sin x − 1 ) = 0
sin x = − 1 3 ⟹ x = arcsin ( − 1 3 ) ≈ − 0.3398 \sin x = -\frac{1}{3} \implies x = \arcsin(-\frac{1}{3}) \approx -0.3398 sin x = − 3 1 ⟹ x = arcsin ( − 3 1 ) ≈ − 0.3398 or x = − π − arcsin ( − 1 3 ) = − π + 0.3398 ≈ − 2.802 x = -\pi - \arcsin(-\frac{1}{3}) = -\pi + 0.3398 \approx -2.802 x = − π − arcsin ( − 3 1 ) = − π + 0.3398 ≈ − 2.802 (since 3.481 > π 3.481 > \pi 3.481 > π Subtract 2 π 2\pi 2 π to stay in [ − π , π ] [-\pi, \pi] [ − π , π ] ).
sin x = 1 ⟹ x = π 2 \sin x = 1 \implies x = \frac{\pi}{2} sin x = 1 ⟹ x = 2 π .
Solutions: x ≈ − 2.802 , − 0.340 , π 2 x \approx -2.802, -0.340, \frac{\pi}{2} x ≈ − 2.802 , − 0.340 , 2 π .
If you get this wrong, revise: Solving trig equations
Problem 8. Use small angle approximations to estimate sin 0.05 cos 0.05 \frac{\sin 0.05}{\cos 0.05} c o s 0.05 s i n 0.05 .
Solution sin 0.05 ≈ 0.05 \sin 0.05 \approx 0.05 sin 0.05 ≈ 0.05
cos 0.05 ≈ 1 − 0.05 2 2 = 1 − 0.00125 = 0.99875 \cos 0.05 \approx 1 - \frac{0.05^2}{2} = 1 - 0.00125 = 0.99875 cos 0.05 ≈ 1 − 2 0.0 5 2 = 1 − 0.00125 = 0.99875
sin 0.05 cos 0.05 ≈ 0.05 0.99875 ≈ 0.05006 \frac{\sin 0.05}{\cos 0.05} \approx \frac{0.05}{0.99875} \approx 0.05006 cos 0.05 sin 0.05 ≈ 0.99875 0.05 ≈ 0.05006 (Alternatively, tan 0.05 ≈ 0.05 \tan 0.05 \approx 0.05 tan 0.05 ≈ 0.05 directly.)
If you get this wrong, revise: Small angle approximations
Problem 9. Prove that 1 + sin 2 A cos 2 A = tan ( A + π 4 ) \dfrac{1 + \sin 2A}{\cos 2A} = \tan\!\left(A + \dfrac{\pi}{4}\right) cos 2 A 1 + sin 2 A = tan ( A + 4 π ) .
Solution Working from the LHS:
1 + sin 2 A cos 2 A = 1 + 2 sin A cos A cos 2 A − sin 2 A = sin 2 A + 2 sin A cos A + cos 2 A ( cos A − sin A ) ( cos A + sin A ) = ( sin A + cos A ) 2 ( cos A − sin A ) ( cos A + sin A ) = sin A + cos A cos A − sin A \begin{aligned} \frac{1 + \sin 2A}{\cos 2A} &= \frac{1 + 2\sin A \cos A}{\cos^2 A - \sin^2 A} \\ &= \frac{\sin^2 A + 2\sin A \cos A + \cos^2 A}{(\cos A - \sin A)(\cos A + \sin A)} \\ &= \frac{(\sin A + \cos A)^2}{(\cos A - \sin A)(\cos A + \sin A)} \\ &= \frac{\sin A + \cos A}{\cos A - \sin A} \end{aligned} cos 2 A 1 + sin 2 A = cos 2 A − sin 2 A 1 + 2 sin A cos A = ( cos A − sin A ) ( cos A + sin A ) sin 2 A + 2 sin A cos A + cos 2 A = ( cos A − sin A ) ( cos A + sin A ) ( sin A + cos A ) 2 = cos A − sin A sin A + cos A Dividing numerator and denominator by cos A \cos A cos A :
= tan A + 1 1 − tan A = \frac{\tan A + 1}{1 - \tan A} = 1 − tan A tan A + 1 From the tangent compound angle formula:
tan ( A + π 4 ) = tan A + tan π 4 1 − tan A tan π 4 = tan A + 1 1 − tan A ■ \tan\!\left(A + \frac{\pi}{4}\right) = \frac{\tan A + \tan\frac{\pi}{4}}{1 - \tan A \tan\frac{\pi}{4}} = \frac{\tan A + 1}{1 - \tan A} \quad \blacksquare tan ( A + 4 π ) = 1 − tan A tan 4 π tan A + tan 4 π = 1 − tan A tan A + 1 ■ If you get this wrong, revise: Compound angle formulas
Problem 10. The area of a sector is 20 c m 2 20\mathrm{ cm}^2 20 cm 2 and the arc length is 10 c m 10\mathrm{ cm} 10 cm . Find the radius and the angle.
Solution s = r θ = 10 ⟹ θ = 10 r s = r\theta = 10 \implies \theta = \frac{10}{r} s = r θ = 10 ⟹ θ = r 10 A = 1 2 r 2 θ = 1 2 r 2 ⋅ 10 r = 5 r = 20 ⟹ r = 4 A = \frac{1}{2}r^2\theta = \frac{1}{2}r^2 \cdot \frac{10}{r} = 5r = 20 \implies r = 4 A = 2 1 r 2 θ = 2 1 r 2 ⋅ r 10 = 5 r = 20 ⟹ r = 4 θ = 10 4 = 2.5 r a d i a n s \theta = \frac{10}{4} = 2.5 \mathrm{ radians} θ = 4 10 = 2.5 radians If you get this wrong, revise: Radian measure
Problem 11. Find the exact value of cos π 12 \cos\dfrac{\pi}{12} cos 12 π using a half-angle formula.
Solution cos π 12 = cos π / 6 2 \cos\frac{\pi}{12} = \cos\frac{\pi/6}{2} cos 12 π = cos 2 π /6 So we apply the half-angle formula with θ = π 6 \theta = \frac{\pi}{6} θ = 6 π .
Since 0 < π 12 < π 2 0 \lt \frac{\pi}{12} \lt \frac{\pi}{2} 0 < 12 π < 2 π (first quadrant), cos π 12 > 0 \cos\frac{\pi}{12} > 0 cos 12 π > 0 .
\begin\{aligned\} \cos\frac\{\pi\}\{12\} &= \sqrt\{\frac\{1 + \cos\frac\{\pi\}\{6\}\}\{2\}\} \\ &= \sqrt\{\frac\{1 + \frac\{\sqrt\{3\}\}\{2\}\}\{2\}\} \\ &= \sqrt\{\frac\{2 + \sqrt\{3\}\}\{4\}\} \\ &= \frac\{\sqrt\{2 + \sqrt\{3\}\}\}\{2\} \end\{aligned\} This can also be verified using the compound angle formula: cos π 12 = cos ( π 3 − π 4 ) = cos π 3 cos π 4 + sin π 3 sin π 4 = 6 + 2 4 \cos\frac{\pi}{12} = \cos\!\left(\frac{\pi}{3} - \frac{\pi}{4}\right) = \cos\frac{\pi}{3}\cos\frac{\pi}{4} + \sin\frac{\pi}{3}\sin\frac{\pi}{4} = \frac{\sqrt{6} + \sqrt{2}}{4} cos 12 π = cos ( 3 π − 4 π ) = cos 3 π cos 4 π + sin 3 π sin 4 π = 4 6 + 2 and one can check that 2 + 3 2 = 6 + 2 4 \dfrac{\sqrt{2+\sqrt{3}}}{2} = \dfrac{\sqrt{6}+\sqrt{2}}{4} 2 2 + 3 = 4 6 + 2 .
If you get this wrong, revise: Half-angle formulas
Problem 12. Find the maximum value of 2 sin θ + 5 cos θ 2\sin\theta + 5\cos\theta 2 sin θ + 5 cos θ and the smallest positive Value of θ \theta θ at which it occurs.
Solution R = 4 + 25 = 29 R = \sqrt{4 + 25} = \sqrt{29} R = 4 + 25 = 29 .
The maximum value is R = 29 R = \sqrt{29} R = 29 .
Writing 2 sin θ + 5 cos θ = 29 sin ( θ + α ) 2\sin\theta + 5\cos\theta = \sqrt{29}\sin(\theta + \alpha) 2 sin θ + 5 cos θ = 29 sin ( θ + α ) where tan α = 5 2 \tan\alpha = \dfrac{5}{2} tan α = 2 5 .
The maximum occurs when sin ( θ + α ) = 1 \sin(\theta + \alpha) = 1 sin ( θ + α ) = 1 I.e., θ + α = π 2 \theta + \alpha = \frac{\pi}{2} θ + α = 2 π .
θ = π 2 − α = π 2 − arctan 5 2 ≈ 0.3805 r a d \theta = \frac{\pi}{2} - \alpha = \frac{\pi}{2} - \arctan\frac{5}{2} \approx 0.3805 \mathrm{ rad} θ = 2 π − α = 2 π − arctan 2 5 ≈ 0.3805 rad Since arctan 5 2 ≈ 1.1903 < π 2 \arctan\frac{5}{2} \approx 1.1903 < \frac{\pi}{2} arctan 2 5 ≈ 1.1903 < 2 π This θ \theta θ is positive and is the Smallest positive value.
If you get this wrong, revise: R-addition formula
Problem 13. Prove that sin 3 A sin A − cos 3 A cos A = 2 \dfrac{\sin 3A}{\sin A} - \dfrac{\cos 3A}{\cos A} = 2 sin A sin 3 A − cos A cos 3 A = 2 .
Solution sin 3 A sin A − cos 3 A cos A = sin 3 A cos A − cos 3 A sin A sin A cos A = sin ( 3 A − A ) sin A cos A = sin 2 A sin A cos A = 2 sin A cos A sin A cos A = 2 ■ \begin{aligned} \frac{\sin 3A}{\sin A} - \frac{\cos 3A}{\cos A} &= \frac{\sin 3A \cos A - \cos 3A \sin A}{\sin A \cos A} \\ &= \frac{\sin(3A - A)}{\sin A \cos A} \\ &= \frac{\sin 2A}{\sin A \cos A} \\ &= \frac{2\sin A \cos A}{\sin A \cos A} \\ &= 2 \quad \blacksquare \end{aligned} sin A sin 3 A − cos A cos 3 A = sin A cos A sin 3 A cos A − cos 3 A sin A = sin A cos A sin ( 3 A − A ) = sin A cos A sin 2 A = sin A cos A 2 sin A cos A = 2 ■ If you get this wrong, revise: Proof strategies
Problem 14. Solve sin θ + 3 cos θ = 1 \sin\theta + \sqrt{3}\cos\theta = 1 sin θ + 3 cos θ = 1 for 0 ≤ θ < 2 π 0 \leq \theta \lt 2\pi 0 ≤ θ < 2 π .
Solution R = 1 + 3 = 2 R = \sqrt{1 + 3} = 2 R = 1 + 3 = 2 , α = arctan 3 = π 3 \alpha = \arctan\sqrt{3} = \frac{\pi}{3} α = arctan 3 = 3 π .
2 sin ( θ + π 3 ) = 1 2\sin\!\left(\theta + \frac{\pi}{3}\right) = 1 2 sin ( θ + 3 π ) = 1 sin ( θ + π 3 ) = 1 2 \sin\!\left(\theta + \frac{\pi}{3}\right) = \frac{1}{2} sin ( θ + 3 π ) = 2 1 θ + π 3 = π 6 + 2 n π o r θ + π 3 = 5 π 6 + 2 n π \theta + \frac{\pi}{3} = \frac{\pi}{6} + 2n\pi \quad \mathrm{or} \quad \theta + \frac{\pi}{3} = \frac{5\pi}{6} + 2n\pi θ + 3 π = 6 π + 2 nπ or θ + 3 π = 6 5 π + 2 nπ Case 1: θ = π 6 − π 3 + 2 n π = − π 6 + 2 n π \theta = \frac{\pi}{6} - \frac{\pi}{3} + 2n\pi = -\frac{\pi}{6} + 2n\pi θ = 6 π − 3 π + 2 nπ = − 6 π + 2 nπ .
For n = 1 n = 1 n = 1 : θ = − π 6 + 2 π = 11 π 6 \theta = -\frac{\pi}{6} + 2\pi = \frac{11\pi}{6} θ = − 6 π + 2 π = 6 11 π .
Case 2: θ = 5 π 6 − π 3 + 2 n π = π 2 + 2 n π \theta = \frac{5\pi}{6} - \frac{\pi}{3} + 2n\pi = \frac{\pi}{2} + 2n\pi θ = 6 5 π − 3 π + 2 nπ = 2 π + 2 nπ .
For n = 0 n = 0 n = 0 : θ = π 2 \theta = \frac{\pi}{2} θ = 2 π .
Solutions: θ = π 2 \theta = \frac{\pi}{2} θ = 2 π or θ = 11 π 6 \theta = \frac{11\pi}{6} θ = 6 11 π .
If you get this wrong, revise: R-addition formula
Problem 15. Prove that 1 − tan 2 A 1 + tan 2 A = cos 2 A \dfrac{1 - \tan^2 A}{1 + \tan^2 A} = \cos 2A 1 + tan 2 A 1 − tan 2 A = cos 2 A .
Solution Using sec 2 A = 1 + tan 2 A \sec^2 A = 1 + \tan^2 A sec 2 A = 1 + tan 2 A :
1 − tan 2 A 1 + tan 2 A = 1 − tan 2 A sec 2 A = ( 1 − tan 2 A ) cos 2 A = cos 2 A − tan 2 A cos 2 A = cos 2 A − sin 2 A cos 2 A ⋅ cos 2 A = cos 2 A − sin 2 A = cos 2 A ■ \begin{aligned} \frac{1 - \tan^2 A}{1 + \tan^2 A} &= \frac{1 - \tan^2 A}{\sec^2 A} \\ &= (1 - \tan^2 A)\cos^2 A \\ &= \cos^2 A - \tan^2 A \cos^2 A \\ &= \cos^2 A - \frac{\sin^2 A}{\cos^2 A} \cdot \cos^2 A \\ &= \cos^2 A - \sin^2 A \\ &= \cos 2A \quad \blacksquare \end{aligned} 1 + tan 2 A 1 − tan 2 A = sec 2 A 1 − tan 2 A = ( 1 − tan 2 A ) cos 2 A = cos 2 A − tan 2 A cos 2 A = cos 2 A − cos 2 A sin 2 A ⋅ cos 2 A = cos 2 A − sin 2 A = cos 2 A ■ If you get this wrong, revise: Proof strategies
Tip
Tip Ready to test your understanding of Trigonometry ? The contains the hardest questions
within the A-Level specification for this topic, each with a full worked solution.
Unit tests probe edge cases and common misconceptions. Integration tests combine Trigonometry with other pure mathematics topics to test synthesis under exam conditions.
See for instructions on self-marking and building a personal test matrix.
Common Pitfalls Rounding too early in multi-step calculations. Carry full precision through and round only the final answer.
Confusing the domain and range of functions, or not considering restrictions (e.g., denominator cannot be zero).
Forgetting the + c +c + c constant of integration in indefinite integrals, or misusing boundary conditions in definite integrals.
Dropping negative signs during algebraic manipulation. Substitute back to verify your answer.
flowchart TD
A[08 Trigonometryx] --> B[Key Concepts]
A --> C[Core Principles]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
C --> F[Design patterns]
D --> G[Real-world usage]
Summary The key principles covered in this topic are linked in the sub-pages above. Focus on understanding the definitions, applying the formulas or frameworks, and evaluating strengths and limitations of each approach.
Worked Examples Worked examples demonstrating the application of key concepts are covered in the detailed sub-pages linked above.
Cross-References Differentiation — Trigonometric derivatives and small angle approximations connect directly to differentiation techniques.Integration — Trigonometric integrals and substitutions require fluency with the identities and substitutions covered here.Further Pure Mathematics 1 — Complex numbers use modulus-argument form, which is built on the trigonometric functions defined in this topic.Functions — Trigonometric functions are key examples of periodic, composite, and inverse functions.