Radian Measure
Definition
The radian is the standard unit of angular measure. An angle θ \theta θ in radians is defined as the
ratio of the arc length s s s subtended by the angle to the radius r r r :
θ = s r \theta = \frac{s}{r} θ = r s
One radian is the angle subtended at the centre of a circle by an arc equal in length to the radius.
Since the circumference of a circle is 2 π r 2\pi r 2 π r , a full revolution is 2 π 2\pi 2 π radians.
Conversion Between Degrees and Radians
π r a d = 180 ∘ \pi \mathrm{ rad} = 180^{\circ} π rad = 18 0 ∘
To convert from degrees to radians:
θ r a d = θ d e g × π 180 \theta_{\mathrm{rad}} = \theta_{\mathrm{deg}} \times \frac{\pi}{180} θ rad = θ deg × 180 π
To convert from radians to degrees:
θ d e g = θ r a d × 180 π \theta_{\mathrm{deg}} = \theta_{\mathrm{rad}} \times \frac{180}{\pi} θ deg = θ rad × π 180
Arc Length
For a circle of radius r r r with a central angle θ \theta θ (in radians):
s = r θ s = r\theta s = r θ
Sector Area
The area of a sector with central angle θ \theta θ (in radians) and radius r r r :
A = 1 2 r 2 θ A = \frac{1}{2}r^2\theta A = 2 1 r 2 θ
Worked Example: Arc Length and Sector Area
Problem: A sector has radius 5 5 5 cm and central angle 3 π 4 \frac{3\pi}{4} 4 3 π radians. Find the arc
length and the area of the sector.
Solution:
Arc length:
s = r θ = 5 × 3 π 4 = 15 π 4 ≈ 11.78 c m s = r\theta = 5 \times \frac{3\pi}{4} = \frac{15\pi}{4} \approx 11.78 \mathrm{ cm} s = r θ = 5 × 4 3 π = 4 15 π ≈ 11.78 cm
Sector area:
A = 1 2 r 2 θ = 1 2 ( 25 ) ( 3 π 4 ) = 75 π 8 ≈ 29.45 c m 2 A = \frac{1}{2}r^2\theta = \frac{1}{2}(25)\left(\frac{3\pi}{4}\right) = \frac{75\pi}{8} \approx 29.45 \mathrm{ cm}^2 A = 2 1 r 2 θ = 2 1 ( 25 ) ( 4 3 π ) = 8 75 π ≈ 29.45 cm 2
Trigonometric Functions
Right-Angle Definitions
sin θ = o p p o s i t e h y p o t e n u s e , cos θ = a d j a c e n t h y p o t e n u s e , tan θ = o p p o s i t e a d j a c e n t = sin θ cos θ \sin \theta = \frac{\mathrm{opposite}}{\mathrm{hypotenuse}}, \quad
\cos \theta = \frac{\mathrm{adjacent}}{\mathrm{hypotenuse}}, \quad
\tan \theta = \frac{\mathrm{opposite}}{\mathrm{adjacent}} = \frac{\sin \theta}{\cos \theta} sin θ = hypotenuse opposite , cos θ = hypotenuse adjacent , tan θ = adjacent opposite = cos θ sin θ
Reciprocal Trigonometric Functions
csc θ = 1 sin θ , sec θ = 1 cos θ , cot θ = 1 tan θ = cos θ sin θ \csc\theta = \frac{1}{\sin\theta}, \quad \sec\theta = \frac{1}{\cos\theta}, \quad \cot\theta = \frac{1}{\tan\theta} = \frac{\cos\theta}{\sin\theta} csc θ = sin θ 1 , sec θ = cos θ 1 , cot θ = tan θ 1 = sin θ cos θ
These are defined wherever the denominator is non-zero.
Graphs of Reciprocal Functions
Function Domain Range Asymptotes x x x -interceptsy = csc x y = \csc x y = csc x x ≠ n π x \neq n\pi x = nπ y ≤ − 1 y \le -1 y ≤ − 1 or y ≥ 1 y \ge 1 y ≥ 1 x = n π x = n\pi x = nπ none y = sec x y = \sec x y = sec x x ≠ π 2 + n π x \neq \frac{\pi}{2} + n\pi x = 2 π + nπ y ≤ − 1 y \le -1 y ≤ − 1 or y ≥ 1 y \ge 1 y ≥ 1 x = π 2 + n π x = \frac{\pi}{2} + n\pi x = 2 π + nπ none y = cot x y = \cot x y = cot x x ≠ n π x \neq n\pi x = nπ all real y y y x = n π x = n\pi x = nπ x = π 2 + n π x = \frac{\pi}{2} + n\pi x = 2 π + nπ
The Unit Circle
The unit circle is a circle of radius 1 1 1 centred at the origin. Any point on the unit circle has
coordinates ( cos θ , sin θ ) (\cos\theta, \sin\theta) ( cos θ , sin θ ) , where θ \theta θ is the angle measured anticlockwise from the
positive x x x -axis.
This definition extends trigonometric functions to all real numbers, not just acute angles. The
Pythagorean identity follows directly from the fact that every point on the unit circle satisfies
x 2 + y 2 = 1 x^2 + y^2 = 1 x 2 + y 2 = 1 .
Key Values
θ \theta θ 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 θ \sin\theta sin θ 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 θ \cos\theta cos θ 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 tan θ \tan\theta tan θ 0 0 0 1 3 \frac{1}{\sqrt{3}} 3 1 1 1 1 3 \sqrt{3} 3 undefined 0 0 0 undefined 0 0 0
All, Sine, Tan, Cos (ASTC)
The signs of trig functions in each quadrant:
A ll positive in the first quadrant (0 < θ < π 2 0 \lt \theta \lt \frac{\pi}{2} 0 < θ < 2 π )
S ine positive in the second quadrant (π 2 < θ < π \frac{\pi}{2} \lt \theta \lt \pi 2 π < θ < π )
T angent positive in the third quadrant (π < θ < 3 π 2 \pi \lt \theta \lt \frac{3\pi}{2} π < θ < 2 3 π )
C osine positive in the fourth quadrant (3 π 2 < θ < 2 π \frac{3\pi}{2} \lt \theta \lt 2\pi 2 3 π < θ < 2 π )
Graphs of Trigonometric Functions
y = sin x y = \sin x y = sin x
Domain: all real x x x
Range: − 1 ≤ y ≤ 1 -1 \le y \le 1 − 1 ≤ y ≤ 1
Period: 2 π 2\pi 2 π
x x x -intercepts at x = 0 , π , 2 π , … x = 0, \pi, 2\pi, \ldots x = 0 , π , 2 π , …
y = cos x y = \cos x y = cos x
Domain: all real x x x
Range: − 1 ≤ y ≤ 1 -1 \le y \le 1 − 1 ≤ y ≤ 1
Period: 2 π 2\pi 2 π
y y y -intercept at ( 0 , 1 ) (0, 1) ( 0 , 1 )
y = tan x y = \tan x y = tan x
Domain: all real x x x except x = π 2 + n π x = \frac{\pi}{2} + n\pi x = 2 π + nπ
Range: all real y y y
Period: π \pi π
Vertical asymptotes at x = π 2 + n π x = \frac{\pi}{2} + n\pi x = 2 π + nπ
For y = a sin ( b x + c ) + d y = a\sin(bx + c) + d y = a sin ( b x + c ) + d :
∣ a ∣ |a| ∣ a ∣ = amplitude
2 π ∣ b ∣ \frac{2\pi}{|b|} ∣ b ∣ 2 π = period
c c c = horizontal phase shift (shift left by c b \frac{c}{b} b c )
d d d = vertical shift
Exam Tip When sketching trig graphs, always label axis intercepts, maximum/minimum points,
and show at least one full period clearly.
Trigonometric Functions: y = A sin(Bx + C) + D
Use the sliders to see how changing a a a , b b b , c c c , and d d d in y = a sin ( b x + c ) + d y = a\sin(bx + c) + d y = a sin ( b x + c ) + d affects the
graph.
Trigonometric Identities
Pythagorean Identities
\begin`\{aligned}`
\sin^2\theta + \cos^2\theta &= 1\\
1 + \tan^2\theta &= \sec^2\theta\\
1 + \cot^2\theta &= \csc^2\theta
\end`\{aligned}`
Proof of sin 2 θ + cos 2 θ = 1 \sin^2\theta + \cos^2\theta = 1 sin 2 θ + cos 2 θ = 1
By the unit circle definition, a point on the unit circle at angle θ \theta θ has coordinates
( cos θ , sin θ ) (\cos\theta, \sin\theta) ( cos θ , sin θ ) . Since every point on the unit circle satisfies x 2 + y 2 = 1 x^2 + y^2 = 1 x 2 + y 2 = 1 , we
substitute:
cos 2 θ + sin 2 θ = 1 \cos^2\theta + \sin^2\theta = 1 cos 2 θ + sin 2 θ = 1
This completes the proof.
Proof of 1 + tan 2 θ = sec 2 θ 1 + \tan^2\theta = \sec^2\theta 1 + tan 2 θ = sec 2 θ
Starting from sin 2 θ + cos 2 θ = 1 \sin^2\theta + \cos^2\theta = 1 sin 2 θ + cos 2 θ = 1 , divide both sides by cos 2 θ \cos^2\theta cos 2 θ :
sin 2 θ cos 2 θ + cos 2 θ cos 2 θ = 1 cos 2 θ \frac{\sin^2\theta}{\cos^2\theta} + \frac{\cos^2\theta}{\cos^2\theta} = \frac{1}{\cos^2\theta} cos 2 θ sin 2 θ + cos 2 θ cos 2 θ = cos 2 θ 1
tan 2 θ + 1 = sec 2 θ \tan^2\theta + 1 = \sec^2\theta tan 2 θ + 1 = sec 2 θ
Proof of 1 + cot 2 θ = csc 2 θ 1 + \cot^2\theta = \csc^2\theta 1 + cot 2 θ = csc 2 θ
Starting from sin 2 θ + cos 2 θ = 1 \sin^2\theta + \cos^2\theta = 1 sin 2 θ + cos 2 θ = 1 , divide both sides by sin 2 θ \sin^2\theta sin 2 θ :
sin 2 θ sin 2 θ + cos 2 θ sin 2 θ = 1 sin 2 θ \frac{\sin^2\theta}{\sin^2\theta} + \frac{\cos^2\theta}{\sin^2\theta} = \frac{1}{\sin^2\theta} sin 2 θ sin 2 θ + sin 2 θ cos 2 θ = sin 2 θ 1
1 + cot 2 θ = csc 2 θ 1 + \cot^2\theta = \csc^2\theta 1 + cot 2 θ = csc 2 θ
Compound Angle Identities
\begin`\{aligned}`
\sin(A \pm B) &= \sin A \cos B \pm \cos A \sin B\\
\cos(A \pm B) &= \cos A \cos B \mp \sin A \sin B\\
\tan(A \pm B) &= \frac{\tan A \pm \tan B}{1 \mp \tan A \tan B}
\end`\{aligned}`
Consider rotating the point ( 1 , 0 ) (1, 0) ( 1 , 0 ) by angle A + B A + B A + B anticlockwise. The resulting coordinates are
( cos ( A + B ) , sin ( A + B ) ) (\cos(A + B), \sin(A + B)) ( cos ( A + B ) , sin ( A + B )) .
Equivalently, we can first rotate by B B B , then by A A A . The rotation matrix for angle α \alpha α is:
R(\alpha) = \begin`\{pmatrix}` \cos\alpha & -\sin\alpha \\ \sin\alpha & \cos\alpha \end`\{pmatrix}`
The composite rotation R ( A ) R ( B ) R(A)R(B) R ( A ) R ( B ) applied to ( 1 , 0 ) (1, 0) ( 1 , 0 ) :
\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}` 1 \\ 0 \end`\{pmatrix}`
First multiply the matrices:
R(A)R(B) = \begin`\{pmatrix}` \cos A \cos B - \sin A \sin B & -\cos A \sin B - \sin A \cos B \\ \sin A \cos B + \cos A \sin B & -\sin A \sin B + \cos A \cos B \end`\{pmatrix}`
Applying to ( 1 , 0 ) (1, 0) ( 1 , 0 ) gives the top-left and bottom-left entries:
cos ( A + B ) = cos A cos B − sin A sin B , sin ( A + B ) = sin A cos B + cos A sin B \cos(A + B) = \cos A \cos B - \sin A \sin B, \quad \sin(A + B) = \sin A \cos B + \cos A \sin B cos ( A + B ) = cos A cos B − sin A sin B , sin ( A + B ) = sin A cos B + cos A sin B
The formulas for A − B A - B A − B follow by substituting − B -B − B and using sin ( − B ) = − sin B \sin(-B) = -\sin B sin ( − B ) = − sin B ,
cos ( − B ) = cos B \cos(-B) = \cos B cos ( − B ) = cos B .
Double Angle Identities
Setting A = B = θ A = B = \theta A = B = θ in the compound angle formulas:
\begin`\{aligned}`
\sin 2\theta &= 2\sin\theta \cos\theta\\[4pt]
\cos 2\theta &= \cos^2\theta - \sin^2\theta\\
\tan 2\theta &= \frac{2\tan\theta}{1 - \tan^2\theta}
\end`\{aligned}`
Starting from cos 2 θ = cos 2 θ − sin 2 θ \cos 2\theta = \cos^2\theta - \sin^2\theta cos 2 θ = cos 2 θ − sin 2 θ :
Form 1: cos 2 θ = cos 2 θ − sin 2 θ \cos 2\theta = \cos^2\theta - \sin^2\theta cos 2 θ = cos 2 θ − sin 2 θ
Form 2: Replace sin 2 θ = 1 − cos 2 θ \sin^2\theta = 1 - \cos^2\theta sin 2 θ = 1 − cos 2 θ : cos 2 θ = 2 cos 2 θ − 1 \cos 2\theta = 2\cos^2\theta - 1 cos 2 θ = 2 cos 2 θ − 1
Form 3: Replace cos 2 θ = 1 − sin 2 θ \cos^2\theta = 1 - \sin^2\theta cos 2 θ = 1 − sin 2 θ : cos 2 θ = 1 − 2 sin 2 θ \cos 2\theta = 1 - 2\sin^2\theta cos 2 θ = 1 − 2 sin 2 θ
Triple Angle Identities
sin 3 θ = 3 sin θ − 4 sin 3 θ \sin 3\theta = 3\sin\theta - 4\sin^3\theta sin 3 θ = 3 sin θ − 4 sin 3 θ
Derivation: Using sin ( 2 θ + θ ) \sin(2\theta + \theta) sin ( 2 θ + θ ) :
sin 3 θ = sin 2 θ cos θ + cos 2 θ sin θ = 2 sin θ cos 2 θ + ( 1 − 2 sin 2 θ ) sin θ = 2 sin θ ( 1 − sin 2 θ ) + sin θ − 2 sin 3 θ = 3 sin θ − 4 sin 3 θ \sin 3\theta = \sin 2\theta \cos\theta + \cos 2\theta \sin\theta = 2\sin\theta\cos^2\theta + (1 - 2\sin^2\theta)\sin\theta = 2\sin\theta(1 - \sin^2\theta) + \sin\theta - 2\sin^3\theta = 3\sin\theta - 4\sin^3\theta sin 3 θ = sin 2 θ cos θ + cos 2 θ sin θ = 2 sin θ cos 2 θ + ( 1 − 2 sin 2 θ ) sin θ = 2 sin θ ( 1 − sin 2 θ ) + sin θ − 2 sin 3 θ = 3 sin θ − 4 sin 3 θ
Inverse Trigonometric Functions
Function Meaning Domain Range arcsin x \arcsin x arcsin x "the angle whose sine is x x x " − 1 ≤ x ≤ 1 -1 \le x \le 1 − 1 ≤ x ≤ 1 − π 2 ≤ arcsin x ≤ π 2 -\frac{\pi}{2} \le \arcsin x \le \frac{\pi}{2} − 2 π ≤ arcsin x ≤ 2 π arccos x \arccos x arccos x "the angle whose cosine is x x x " − 1 ≤ x ≤ 1 -1 \le x \le 1 − 1 ≤ x ≤ 1 0 ≤ arccos x ≤ π 0 \le \arccos x \le \pi 0 ≤ arccos x ≤ π arctan x \arctan x arctan x "the angle whose tangent is x x x " all real x x x − π 2 < arctan x < π 2 -\frac{\pi}{2} \lt \arctan x \lt \frac{\pi}{2} − 2 π < arctan x < 2 π
Properties
arcsin ( − x ) = − arcsin ( x ) , arctan ( − x ) = − arctan ( x ) , arccos ( − x ) = π − arccos ( x ) \arcsin(-x) = -\arcsin(x), \quad \arctan(-x) = -\arctan(x), \quad \arccos(-x) = \pi - \arccos(x) arcsin ( − x ) = − arcsin ( x ) , arctan ( − x ) = − arctan ( x ) , arccos ( − x ) = π − arccos ( x )
Composition Identities
For x x x in the appropriate domain:
\begin`\{aligned}`
\sin(\arcsin x) &= x, \quad \mathrm{for } -1 \le x \le 1\\
\cos(\arccos x) &= x, \quad \mathrm{for } -1 \le x \le 1\\
\tan(\arctan x) &= x, \quad \mathrm{for all real } x
\end`\{aligned}`
The reverse compositions are only true on restricted domains:
\begin`\{aligned}`
\arcsin(\sin x) &= x, \quad \mathrm{for } -\frac{\pi}{2} \le x \le \frac{\pi}{2}\\
\arccos(\cos x) &= x, \quad \mathrm{for } 0 \le x \le \pi\\
\arctan(\tan x) &= x, \quad \mathrm{for } -\frac{\pi}{2} \lt x \lt \frac{\pi}{2}
\end`\{aligned}`
Worked Example: Inverse Trig Evaluation
Problem: Evaluate sin ( arccos 1 3 ) \sin\left(\arccos\frac{1}{3}\right) sin ( arccos 3 1 ) without a calculator.
Solution:
Let θ = arccos 1 3 \theta = \arccos\frac{1}{3} θ = arccos 3 1 , so cos θ = 1 3 \cos\theta = \frac{1}{3} cos θ = 3 1 with θ ∈ [ 0 , π ] \theta \in [0, \pi] θ ∈ [ 0 , π ] . Since
cos θ > 0 \cos\theta \gt 0 cos θ > 0 , we have θ \theta θ in the first quadrant, so sin θ ≥ 0 \sin\theta \ge 0 sin θ ≥ 0 :
sin θ = 1 − 1 9 = 2 2 3 \sin\theta = \sqrt{1 - \frac{1}{9}} = \frac{2\sqrt{2}}{3} sin θ = 1 − 9 1 = 3 2 2
Exam Tip Be careful with the range of inverse trig functions. Your calculator only gives the
principal value -- you may need to find other solutions using the periodic properties or the ASTC
rule.
Sine and Cosine Rules
Sine Rule
a sin A = b sin B = c sin C \frac{a}{\sin A} = \frac{b}{\sin B} = \frac{c}{\sin C} sin A a = sin B b = sin C c
Used when you know:
Two angles and one side (AAS), or
Two sides and a non-included angle (SSA -- see ambiguous case below)
Cosine Rule
c 2 = a 2 + b 2 − 2 a b cos C c^2 = a^2 + b^2 - 2ab\cos C c 2 = a 2 + b 2 − 2 ab cos C
Or equivalently:
cos C = a 2 + b 2 − c 2 2 a b \cos C = \frac{a^2 + b^2 - c^2}{2ab} cos C = 2 ab a 2 + b 2 − c 2
Used when you know:
Two sides and the included angle (SAS), or
All three sides (SSS)
Area of a Triangle
A r e a = 1 2 a b sin C \mathrm{Area} = \frac{1}{2}ab\sin C Area = 2 1 ab sin C
Worked Example: Sine Rule
Problem: In triangle A B C ABC A B C , a = 8 a = 8 a = 8 cm, A = 45 ∘ A = 45^\circ A = 4 5 ∘ , B = 30 ∘ B = 30^\circ B = 3 0 ∘ . Find b b b .
Solution:
b = 8 sin 30 ∘ sin 45 ∘ = 4 2 2 = 4 2 ≈ 5.66 c m b = \frac{8\sin 30^{\circ}}{\sin 45^{\circ}} = \frac{4}{\frac{\sqrt{2}}{2}} = 4\sqrt{2} \approx 5.66 \mathrm{ cm} b = sin 4 5 ∘ 8 sin 3 0 ∘ = 2 2 4 = 4 2 ≈ 5.66 cm
Worked Example: Cosine Rule
Problem: Find the angle C C C in a triangle with sides a = 5 a = 5 a = 5 , b = 7 b = 7 b = 7 , c = 8 c = 8 c = 8 .
Solution:
cos C = 5 2 + 7 2 − 8 2 2 × 5 × 7 = 25 + 49 − 64 70 = 10 70 = 1 7 \cos C = \frac{5^2 + 7^2 - 8^2}{2 \times 5 \times 7} = \frac{25 + 49 - 64}{70} = \frac{10}{70} = \frac{1}{7} cos C = 2 × 5 × 7 5 2 + 7 2 − 8 2 = 70 25 + 49 − 64 = 70 10 = 7 1
C = arccos ( 1 7 ) ≈ 81.8 ∘ C = \arccos\left(\frac{1}{7}\right) \approx 81.8^{\circ} C = arccos ( 7 1 ) ≈ 81. 8 ∘
Ambiguous Case of the Sine Rule
When using the sine rule with SSA (two sides and a non-included angle), there may be two possible
triangles , one triangle , or no triangle .
Condition for Ambiguity
Given sides a a a and b b b and angle A A A (where a a a is opposite A A A ):
No triangle if a < b sin A a \lt b\sin A a < b sin A
One right-angled triangle if a = b sin A a = b\sin A a = b sin A
Two triangles if b sin A < a < b b\sin A \lt a \lt b b sin A < a < b and A < 90 ∘ A \lt 90^\circ A < 9 0 ∘
One triangle if a ≥ b a \ge b a ≥ b or A ≥ 90 ∘ A \ge 90^\circ A ≥ 9 0 ∘
Why Two Triangles?
When sin B = k \sin B = k sin B = k where 0 < k < 1 0 \lt k \lt 1 0 < k < 1 , there are two possible values for B B B :
B 1 = arcsin ( k ) a n d B 2 = 180 ∘ − arcsin ( k ) B_1 = \arcsin(k) \quad \mathrm{and} \quad B_2 = 180^{\circ} - \arcsin(k) B 1 = arcsin ( k ) and B 2 = 18 0 ∘ − arcsin ( k )
Both may be valid since B 1 + B 2 = 180 ∘ B_1 + B_2 = 180^\circ B 1 + B 2 = 18 0 ∘ (so if A + B 1 < 180 ∘ A + B_1 \lt 180^\circ A + B 1 < 18 0 ∘ , check whether
A + B 2 < 180 ∘ A + B_2 \lt 180^\circ A + B 2 < 18 0 ∘ as well).
Worked Example: Ambiguous Case
Problem: In triangle A B C ABC A B C , a = 7 a = 7 a = 7 , b = 10 b = 10 b = 10 , A = 40 ∘ A = 40^\circ A = 4 0 ∘ . Find all possible triangles.
Solution:
Using the sine rule:
sin B 10 = sin 40 ∘ 7 ⟹ sin B = 10 sin 40 ∘ 7 ≈ 0.919 \frac{\sin B}{10} = \frac{\sin 40^{\circ}}{7} \implies \sin B = \frac{10\sin 40^{\circ}}{7} \approx 0.919 10 sin B = 7 sin 4 0 ∘ ⟹ sin B = 7 10 sin 4 0 ∘ ≈ 0.919
Since 0 < 0.919 < 1 0 \lt 0.919 \lt 1 0 < 0.919 < 1 , there are two possible values for B B B :
B 1 = arcsin ( 0.919 ) ≈ 66.8 ∘ , B 2 = 180 ∘ − 66.8 ∘ = 113.2 ∘ B_1 = \arcsin(0.919) \approx 66.8^{\circ}, \quad B_2 = 180^{\circ} - 66.8^{\circ} = 113.2^{\circ} B 1 = arcsin ( 0.919 ) ≈ 66. 8 ∘ , B 2 = 18 0 ∘ − 66. 8 ∘ = 113. 2 ∘
Check both: A + B 1 = 106.8 ∘ < 180 ∘ A + B_1 = 106.8^{\circ} \lt 180^\circ A + B 1 = 106. 8 ∘ < 18 0 ∘ and A + B 2 = 153.2 ∘ < 180 ∘ A + B_2 = 153.2^{\circ} \lt 180^\circ A + B 2 = 153. 2 ∘ < 18 0 ∘ . Both are valid.
Triangle 1: B = 66.8 ∘ B = 66.8^\circ B = 66. 8 ∘ , C = 73.2 ∘ C = 73.2^\circ C = 73. 2 ∘ ,
c 1 = 7 sin 73.2 ∘ sin 40 ∘ ≈ 10.4 c_1 = \frac{7\sin 73.2^{\circ}}{\sin 40^{\circ}} \approx 10.4 c 1 = s i n 4 0 ∘ 7 s i n 73. 2 ∘ ≈ 10.4
Triangle 2: B = 113.2 ∘ B = 113.2^\circ B = 113. 2 ∘ , C = 26.8 ∘ C = 26.8^\circ C = 26. 8 ∘ ,
c 2 = 7 sin 26.8 ∘ sin 40 ∘ ≈ 4.89 c_2 = \frac{7\sin 26.8^{\circ}}{\sin 40^{\circ}} \approx 4.89 c 2 = s i n 4 0 ∘ 7 s i n 26. 8 ∘ ≈ 4.89
Non-Right-Angled Triangle Problems
Strategy
Draw and label a clear diagram.
Identify which rule(s) to apply based on the given information.
Use the sine rule for AAS or SSA, the cosine rule for SAS or SSS.
For area problems, use 1 2 a b sin C \frac{1}{2}ab\sin C 2 1 ab sin C or split into right-angled triangles.
For bearing problems, remember that bearings are measured clockwise from north.
Worked Example: Multi-Step Triangle Problem
Problem: In triangle A B C ABC A B C , a = 12 a = 12 a = 12 , b = 8 b = 8 b = 8 , A = 65 ∘ A = 65^\circ A = 6 5 ∘ . Find the area of the triangle.
Solution:
Find angle B B B using the sine rule:
sin B 8 = sin 65 ∘ 12 ⟹ sin B = 2 sin 65 ∘ 3 ≈ 0.604 \frac{\sin B}{8} = \frac{\sin 65^{\circ}}{12} \implies \sin B = \frac{2\sin 65^{\circ}}{3} \approx 0.604 8 sin B = 12 sin 6 5 ∘ ⟹ sin B = 3 2 sin 6 5 ∘ ≈ 0.604
Since b < a b \lt a b < a , there is only one solution: B ≈ 37.2 ∘ B \approx 37.2^\circ B ≈ 37. 2 ∘ , so C = 77.8 ∘ C = 77.8^\circ C = 77. 8 ∘ .
A r e a = 1 2 ( 12 ) ( 8 ) sin 77.8 ∘ ≈ 47.0 s q u a r e u n i t s \mathrm{Area} = \frac{1}{2}(12)(8)\sin 77.8^{\circ} \approx 47.0 \mathrm{ square units} Area = 2 1 ( 12 ) ( 8 ) sin 77. 8 ∘ ≈ 47.0 squareunits
Worked Example: Bearing Problem
Problem: A ship sails from port A A A on a bearing of 050 ∘ 050^\circ 05 0 ∘ for 15 15 15 km to point B B B , then
on a bearing of 110 ∘ 110^\circ 11 0 ∘ for 20 20 20 km to point C C C . Find the distance and bearing from C C C back to
A A A .
Solution:
The angle at B B B is the change in bearing: 110 ∘ − 050 ∘ = 60 ∘ 110^{\circ} - 050^{\circ} = 60^\circ 11 0 ∘ − 05 0 ∘ = 6 0 ∘ . The interior angle at B B B is
180 ∘ − 60 ∘ = 120 ∘ 180^{\circ} - 60^{\circ} = 120^\circ 18 0 ∘ − 6 0 ∘ = 12 0 ∘ .
Using the cosine rule:
A C = 15 2 + 20 2 − 2 ( 15 ) ( 20 ) cos 120 ∘ = 225 + 400 + 300 = 925 = 5 37 ≈ 30.4 k m AC = \sqrt{15^2 + 20^2 - 2(15)(20)\cos 120^{\circ}} = \sqrt{225 + 400 + 300} = \sqrt{925} = 5\sqrt{37} \approx 30.4 \mathrm{ km} A C = 1 5 2 + 2 0 2 − 2 ( 15 ) ( 20 ) cos 12 0 ∘ = 225 + 400 + 300 = 925 = 5 37 ≈ 30.4 km
To find the bearing, find angle C C C :
sin C 15 = sin 120 ∘ 5 37 ⟹ C ≈ 25.3 ∘ \frac{\sin C}{15} = \frac{\sin 120^{\circ}}{5\sqrt{37}} \implies C \approx 25.3^{\circ} 15 sin C = 5 37 sin 12 0 ∘ ⟹ C ≈ 25. 3 ∘
The bearing from C C C to A A A is 360 ∘ − 110 ∘ − 25.3 ∘ ≈ 225 ∘ 360^{\circ} - 110^{\circ} - 25.3^{\circ} \approx 225^\circ 36 0 ∘ − 11 0 ∘ − 25. 3 ∘ ≈ 22 5 ∘ .
Solving Trigonometric Equations
General Solutions
\begin`\{aligned}`
\sin\theta &= k \implies \theta = \arcsin(k) + 2n\pi \mathrm{ or } \theta = \pi - \arcsin(k) + 2n\pi\\
\cos\theta &= k \implies \theta = \arccos(k) + 2n\pi \mathrm{ or } \theta = -\arccos(k) + 2n\pi\\
\tan\theta &= k \implies \theta = \arctan(k) + n\pi
\end`\{aligned}`
where n ∈ ′ { ′ Z ′ } ′ n \in \mathbb{'\{'}Z{'\}'} n ∈ ′ { ′ Z ′ } ′ .
Worked Example: Basic Trig Equation
Problem: Solve sin 2 x = 1 2 \sin 2x = \frac{1}{2} sin 2 x = 2 1 for x ∈ [ 0 , 2 π ] x \in [0, 2\pi] x ∈ [ 0 , 2 π ] .
Solution:
Let u = 2 x u = 2x u = 2 x , so u ∈ [ 0 , 4 π ] u \in [0, 4\pi] u ∈ [ 0 , 4 π ] .
sin u = 1 2 ⟹ u = π 6 , 5 π 6 , 2 π + π 6 , 2 π + 5 π 6 \sin u = \frac{1}{2} \implies u = \frac{\pi}{6}, \frac{5\pi}{6}, 2\pi + \frac{\pi}{6}, 2\pi + \frac{5\pi}{6} sin u = 2 1 ⟹ u = 6 π , 6 5 π , 2 π + 6 π , 2 π + 6 5 π
u = π 6 , 5 π 6 , 13 π 6 , 17 π 6 u = \frac{\pi}{6}, \frac{5\pi}{6}, \frac{13\pi}{6}, \frac{17\pi}{6} u = 6 π , 6 5 π , 6 13 π , 6 17 π
x = u 2 = π 12 , 5 π 12 , 13 π 12 , 17 π 12 x = \frac{u}{2} = \frac{\pi}{12}, \frac{5\pi}{12}, \frac{13\pi}{12}, \frac{17\pi}{12} x = 2 u = 12 π , 12 5 π , 12 13 π , 12 17 π
Worked Example: Factoring
Problem: Solve 2 cos 2 x − cos x − 1 = 0 2\cos^2 x - \cos x - 1 = 0 2 cos 2 x − cos x − 1 = 0 for x ∈ [ 0 , 2 π ] x \in [0, 2\pi] x ∈ [ 0 , 2 π ] .
Solution:
Let u = cos x u = \cos x u = cos x :
2 u 2 − u − 1 = 0 ⟹ ( 2 u + 1 ) ( u − 1 ) = 0 2u^2 - u - 1 = 0 \implies (2u + 1)(u - 1) = 0 2 u 2 − u − 1 = 0 ⟹ ( 2 u + 1 ) ( u − 1 ) = 0
u = − 1 2 o r u = 1 u = -\frac{1}{2} \mathrm{ or } u = 1 u = − 2 1 or u = 1
cos x = − 1 2 ⟹ x = 2 π 3 , 4 π 3 \cos x = -\frac{1}{2} \implies x = \frac{2\pi}{3}, \frac{4\pi}{3} cos x = − 2 1 ⟹ x = 3 2 π , 3 4 π
cos x = 1 ⟹ x = 0 \cos x = 1 \implies x = 0 cos x = 1 ⟹ x = 0
So x = 0 , 2 π 3 , 4 π 3 x = 0, \frac{2\pi}{3}, \frac{4\pi}{3} x = 0 , 3 2 π , 3 4 π .
Worked Example: Using Identities
Problem: Solve sin 2 x = 3 cos 2 x \sin^2 x = 3\cos^2 x sin 2 x = 3 cos 2 x for x ∈ [ 0 , 2 π ] x \in [0, 2\pi] x ∈ [ 0 , 2 π ] .
Solution:
Replace cos 2 x \cos^2 x cos 2 x with 1 − sin 2 x 1 - \sin^2 x 1 − sin 2 x :
sin 2 x = 3 ( 1 − sin 2 x ) ⟹ sin 2 x = 3 − 3 sin 2 x ⟹ 4 sin 2 x = 3 \sin^2 x = 3(1 - \sin^2 x) \implies \sin^2 x = 3 - 3\sin^2 x \implies 4\sin^2 x = 3 sin 2 x = 3 ( 1 − sin 2 x ) ⟹ sin 2 x = 3 − 3 sin 2 x ⟹ 4 sin 2 x = 3
sin 2 x = 3 4 ⟹ sin x = ± 3 2 \sin^2 x = \frac{3}{4} \implies \sin x = \pm\frac{\sqrt{3}}{2} sin 2 x = 4 3 ⟹ sin x = ± 2 3
Since sin x > 0 \sin x \gt 0 sin x > 0 in quadrants I and II, and sin x < 0 \sin x \lt 0 sin x < 0 in quadrants III and IV:
x = π 3 , 2 π 3 , 4 π 3 , 5 π 3 x = \frac{\pi}{3}, \frac{2\pi}{3}, \frac{4\pi}{3}, \frac{5\pi}{3} x = 3 π , 3 2 π , 3 4 π , 3 5 π
Worked Example: Equations Involving tan \tan tan
Problem: Solve tan 2 x = 1 \tan 2x = 1 tan 2 x = 1 for x ∈ [ 0 , π ] x \in [0, \pi] x ∈ [ 0 , π ] .
Solution:
Since tan \tan tan has period π \pi π , tan 2 x = 1 \tan 2x = 1 tan 2 x = 1 gives 2 x = π 4 + n π 2x = \frac{\pi}{4} + n\pi 2 x = 4 π + nπ for
n ∈ ′ { ′ Z ′ } ′ n \in \mathbb{'\{'}Z{'\}'} n ∈ ′ { ′ Z ′ } ′ .
x = π 8 + n π 2 x = \frac{\pi}{8} + \frac{n\pi}{2} x = 8 π + 2 nπ
For x ∈ [ 0 , π ] x \in [0, \pi] x ∈ [ 0 , π ] :
n = 0 n = 0 n = 0 : x = π 8 x = \frac{\pi}{8} x = 8 π
n = 1 n = 1 n = 1 : x = π 8 + π 2 = 5 π 8 x = \frac{\pi}{8} + \frac{\pi}{2} = \frac{5\pi}{8} x = 8 π + 2 π = 8 5 π
n = 2 n = 2 n = 2 : x = π 8 + π = 9 π 8 > π x = \frac{\pi}{8} + \pi = \frac{9\pi}{8} \gt \pi x = 8 π + π = 8 9 π > π (outside range)
So x = π 8 , 5 π 8 x = \frac{\pi}{8}, \frac{5\pi}{8} x = 8 π , 8 5 π .
Expressions of the form a sin x + b cos x a\sin x + b\cos x a sin x + b cos x can be written as a single trigonometric function:
a sin x + b cos x = R sin ( x + α ) a\sin x + b\cos x = R\sin(x + \alpha) a sin x + b cos x = R sin ( x + 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 = \frac{b}{a} tan α = a b .
This is useful for finding maximum/minimum values and for solving equations.
Problem: Express 3 sin x + 4 cos x 3\sin x + 4\cos x 3 sin x + 4 cos x in the form R sin ( x + α ) R\sin(x + \alpha) R sin ( x + α ) , and hence solve
3 sin x + 4 cos x = 5 3\sin x + 4\cos x = 5 3 sin x + 4 cos x = 5 for x ∈ [ 0 , 2 π ] x \in [0, 2\pi] x ∈ [ 0 , 2 π ] .
Solution:
R = 3 2 + 4 2 = 5 R = \sqrt{3^2 + 4^2} = 5 R = 3 2 + 4 2 = 5
tan α = 4 3 ⟹ α = arctan 4 3 ≈ 0.927 r a d \tan\alpha = \frac{4}{3} \implies \alpha = \arctan\frac{4}{3} \approx 0.927 \mathrm{ rad} tan α = 3 4 ⟹ α = arctan 3 4 ≈ 0.927 rad
So 3 sin x + 4 cos x = 5 sin ( x + 0.927 ) 3\sin x + 4\cos x = 5\sin(x + 0.927) 3 sin x + 4 cos x = 5 sin ( x + 0.927 ) .
Solving 5 sin ( x + 0.927 ) = 5 5\sin(x + 0.927) = 5 5 sin ( x + 0.927 ) = 5 :
sin ( x + 0.927 ) = 1 ⟹ x + 0.927 = π 2 + 2 n π \sin(x + 0.927) = 1 \implies x + 0.927 = \frac{\pi}{2} + 2n\pi sin ( x + 0.927 ) = 1 ⟹ x + 0.927 = 2 π + 2 nπ
x = π 2 − 0.927 + 2 n π ≈ 0.644 + 2 n π x = \frac{\pi}{2} - 0.927 + 2n\pi \approx 0.644 + 2n\pi x = 2 π − 0.927 + 2 nπ ≈ 0.644 + 2 nπ
For x ∈ [ 0 , 2 π ] x \in [0, 2\pi] x ∈ [ 0 , 2 π ] : x ≈ 0.644 x \approx 0.644 x ≈ 0.644 rad (the next value 0.644 + 2 π 0.644 + 2\pi 0.644 + 2 π exceeds 2 π 2\pi 2 π ).
3D Trigonometry
3D trigonometry involves applying trigonometric ratios in three-dimensional problems. The key is to
identify right-angled triangles within the 3D shape.
Strategy
Draw a clear diagram of the 3D shape.
Identify the relevant 2D triangles (often by drawing auxiliary lines).
Label known sides and angles.
Apply Pythagoras' theorem, sine rule, cosine rule, or basic trig ratios.
Worked Example: 3D Problem
Problem: A pyramid has a square base of side 6 6 6 cm and vertical height 4 4 4 cm. Find the angle
between a sloping edge and the base.
Solution:
The distance from the centre of the base to a vertex is 6 2 2 = 3 2 \frac{6\sqrt{2}}{2} = 3\sqrt{2} 2 6 2 = 3 2 cm.
θ = arctan ( 4 3 2 ) = arctan ( 2 2 3 ) ≈ 43.3 ∘ \theta = \arctan\left(\frac{4}{3\sqrt{2}}\right) = \arctan\left(\frac{2\sqrt{2}}{3}\right) \approx 43.3^{\circ} θ = arctan ( 3 2 4 ) = arctan ( 3 2 2 ) ≈ 43. 3 ∘
Trigonometric Proof Strategies
General Approach
In IB exams, trigonometric proofs typically ask you to show that one expression equals another. The
standard approach is:
Start with one side -- usually the more complex side (LHS).
Apply known identities to transform it step by step toward the other side.
Never assume what you are trying to prove -- work forward from a known truth.
Useful Techniques
Factor: Look for common factors, e.g., sin x + sin x cos x = sin x ( 1 + cos x ) \sin x + \sin x\cos x = \sin x(1 + \cos x) sin x + sin x cos x = sin x ( 1 + cos x ) .
Use sin 2 + cos 2 = 1 \sin^2 + \cos^2 = 1 sin 2 + cos 2 = 1 : Convert everything to sines or everything to cosines.
Convert to sin \sin sin and cos \cos cos : When tan \tan tan , sec \sec sec , csc \csc csc , or cot \cot cot appear, express them in
terms of sin \sin sin and cos \cos cos .
Look for compound angle structure: Recognise when an expression matches sin ( A ± B ) \sin(A \pm B) sin ( A ± B ) or
cos ( A ± B ) \cos(A \pm B) cos ( A ± B ) .
Common denominator: When fractions appear, combine them over a single denominator.
Worked Example: Proof by Multiplication
Problem: Prove that sin x 1 + cos x = 1 − cos x sin x \frac{\sin x}{1 + \cos x} = \frac{1 - \cos x}{\sin x} 1 + c o s x s i n x = s i n x 1 − c o s x .
Proof:
Multiply numerator and denominator by 1 − cos x 1 - \cos x 1 − cos x :
sin x ( 1 − cos x ) ( 1 + cos x ) ( 1 − cos x ) = sin x ( 1 − cos x ) 1 − cos 2 x = sin x ( 1 − cos x ) sin 2 x = 1 − cos x sin x = R H S \frac{\sin x(1 - \cos x)}{(1 + \cos x)(1 - \cos x)} = \frac{\sin x(1 - \cos x)}{1 - \cos^2 x} = \frac{\sin x(1 - \cos x)}{\sin^2 x} = \frac{1 - \cos x}{\sin x} = \mathrm{RHS} ( 1 + cos x ) ( 1 − cos x ) sin x ( 1 − cos x ) = 1 − cos 2 x sin x ( 1 − cos x ) = sin 2 x sin x ( 1 − cos x ) = sin x 1 − cos x = RHS
Worked Example: Proof Using Identities
Problem: Prove that 1 − cos 2 x sin 2 x = tan x \frac{1 - \cos 2x}{\sin 2x} = \tan x s i n 2 x 1 − c o s 2 x = tan x .
Proof:
Using cos 2 x = 1 − 2 sin 2 x \cos 2x = 1 - 2\sin^2 x cos 2 x = 1 − 2 sin 2 x and sin 2 x = 2 sin x cos x \sin 2x = 2\sin x\cos x sin 2 x = 2 sin x cos x :
1 − ( 1 − 2 sin 2 x ) 2 sin x cos x = 2 sin 2 x 2 sin x cos x = sin x cos x = tan x = R H S \frac{1 - (1 - 2\sin^2 x)}{2\sin x\cos x} = \frac{2\sin^2 x}{2\sin x\cos x} = \frac{\sin x}{\cos x} = \tan x = \mathrm{RHS} 2 sin x cos x 1 − ( 1 − 2 sin 2 x ) = 2 sin x cos x 2 sin 2 x = cos x sin x = tan x = RHS
Worked Example: Proof with Compound Angles
Problem: Prove that sin ( A + B ) cos A cos B = tan A + tan B \frac{\sin(A + B)}{\cos A \cos B} = \tan A + \tan B c o s A c o s B s i n ( A + B ) = tan A + tan B .
Proof:
Expand sin ( A + B ) \sin(A + B) sin ( A + B ) and split the fraction:
sin A cos B + cos A sin B cos A cos B = sin A cos A + sin B cos B = tan A + tan B = R H S \frac{\sin A \cos B + \cos A \sin B}{\cos A \cos B} = \frac{\sin A}{\cos A} + \frac{\sin B}{\cos B} = \tan A + \tan B = \mathrm{RHS} cos A cos B sin A cos B + cos A sin B = cos A sin A + cos B sin B = tan A + tan B = RHS
Common Pitfalls
Forgetting to Check All Solutions
When solving sin θ = k \sin\theta = k sin θ = k or cos θ = k \cos\theta = k cos θ = k , there are always (at least) two solutions per
period. A common mistake is to find arcsin ( k ) \arcsin(k) arcsin ( k ) but forget π − arcsin ( k ) \pi - \arcsin(k) π − arcsin ( k ) .
Mixing Up Degrees and Radians
Ensure your calculator is in the correct mode. If an angle is given as π 3 \frac{\pi}{3} 3 π , it is in
radians; if given as 60 ∘ 60^\circ 6 0 ∘ , it is in degrees. Forgetting to convert is one of the most frequent
errors.
For cos ( A − B ) \cos(A - B) cos ( A − B ) :
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
The sin A sin B \sin A \sin B sin A sin B term is positive (the ∓ \mp ∓ from the ± \pm ± formula flips). Students often
incorrectly write a minus sign here.
Ambiguous Case of the Sine Rule
When using the sine rule with SSA data, always check whether two triangles are possible. If
sin B = k \sin B = k sin B = k with 0 < k < 1 0 \lt k \lt 1 0 < k < 1 and B B B is acute, then 180 ∘ − B 180^{\circ} - B 18 0 ∘ − B may also be valid.
Domain of Inverse Functions
arcsin x \arcsin x arcsin x and arctan x \arctan x arctan x return values in [ − π 2 , π 2 ] [-\frac{\pi}{2}, \frac{\pi}{2}] [ − 2 π , 2 π ] , while arccos x \arccos x arccos x
returns values in [ 0 , π ] [0, \pi] [ 0 , π ] . If the actual angle is in a different quadrant, you must adjust using
ASTC.
Problem Set
Problem 1: Radian Measure Problem: A circle has radius r = 8 r = 8 r = 8 cm. A sector of the circle has area 48 48 48 cm2 ^2 2 . Find the
exact arc length of the sector.
Solution:
Using the sector area formula A = 1 2 r 2 θ A = \frac{1}{2}r^2\theta A = 2 1 r 2 θ :
48 = 1 2 ( 64 ) θ ⟹ 48 = 32 θ ⟹ θ = 3 2 r a d 48 = \frac{1}{2}(64)\theta \implies 48 = 32\theta \implies \theta = \frac{3}{2} \mathrm{ rad} 48 = 2 1 ( 64 ) θ ⟹ 48 = 32 θ ⟹ θ = 2 3 rad Arc length s = r θ = 8 × 3 2 = 12 s = r\theta = 8 \times \frac{3}{2} = 12 s = r θ = 8 × 2 3 = 12 cm.
Problem 2: Compound Angle Identity Problem: Given that sin α = 3 5 \sin\alpha = \frac{3}{5} sin α = 5 3 and cos β = 12 13 \cos\beta = \frac{12}{13} cos β = 13 12 , where α \alpha α
and β \beta β are acute angles, find the exact value of sin ( α + β ) \sin(\alpha + \beta) sin ( α + β ) .
Solution:
Since α \alpha α is acute: cos α = 1 − 9 25 = 4 5 \cos\alpha = \sqrt{1 - \frac{9}{25}} = \frac{4}{5} cos α = 1 − 25 9 = 5 4 . Since β \beta β is
acute: sin β = 1 − 144 169 = 5 13 \sin\beta = \sqrt{1 - \frac{144}{169}} = \frac{5}{13} sin β = 1 − 169 144 = 13 5 .
sin ( α + β ) = sin α cos β + cos α sin β = 3 5 ⋅ 12 13 + 4 5 ⋅ 5 13 = 36 65 + 20 65 = 56 65 \sin(\alpha + \beta) = \sin\alpha\cos\beta + \cos\alpha\sin\beta = \frac{3}{5} \cdot \frac{12}{13} + \frac{4}{5} \cdot \frac{5}{13} = \frac{36}{65} + \frac{20}{65} = \frac{56}{65} sin ( α + β ) = sin α cos β + cos α sin β = 5 3 ⋅ 13 12 + 5 4 ⋅ 13 5 = 65 36 + 65 20 = 65 56
Problem 3: Trigonometric Equation (Factoring) Problem: Solve 2 sin 2 x − sin x − 1 = 0 2\sin^2 x - \sin x - 1 = 0 2 sin 2 x − sin x − 1 = 0 for x ∈ [ 0 , 2 π ] x \in [0, 2\pi] x ∈ [ 0 , 2 π ] .
Solution:
Let u = sin x u = \sin x u = sin x : 2 u 2 − u − 1 = 0 ⟹ ( 2 u + 1 ) ( u − 1 ) = 0 ⟹ u = − 1 2 2u^2 - u - 1 = 0 \implies (2u + 1)(u - 1) = 0 \implies u = -\frac{1}{2} 2 u 2 − u − 1 = 0 ⟹ ( 2 u + 1 ) ( u − 1 ) = 0 ⟹ u = − 2 1 or
u = 1 u = 1 u = 1 .
sin x = − 1 2 ⟹ x = 7 π 6 , 11 π 6 \sin x = -\frac{1}{2} \implies x = \frac{7\pi}{6}, \frac{11\pi}{6} sin x = − 2 1 ⟹ x = 6 7 π , 6 11 π (quadrants III and IV)
sin x = 1 ⟹ x = π 2 \sin x = 1 \implies x = \frac{\pi}{2} sin x = 1 ⟹ x = 2 π
So x = π 2 , 7 π 6 , 11 π 6 x = \frac{\pi}{2}, \frac{7\pi}{6}, \frac{11\pi}{6} x = 2 π , 6 7 π , 6 11 π .
Problem 4: Double Angle Application Problem: Solve cos 2 x = cos x \cos 2x = \cos x cos 2 x = cos x for x ∈ [ 0 , 2 π ] x \in [0, 2\pi] x ∈ [ 0 , 2 π ] .
Solution:
Using cos 2 x = 2 cos 2 x − 1 \cos 2x = 2\cos^2 x - 1 cos 2 x = 2 cos 2 x − 1 : 2 cos 2 x − 1 = cos x ⟹ 2 cos 2 x − cos x − 1 = 0 2\cos^2 x - 1 = \cos x \implies 2\cos^2 x - \cos x - 1 = 0 2 cos 2 x − 1 = cos x ⟹ 2 cos 2 x − cos x − 1 = 0 .
Let u = cos x u = \cos x u = cos x : ( 2 u + 1 ) ( u − 1 ) = 0 ⟹ u = − 1 2 (2u + 1)(u - 1) = 0 \implies u = -\frac{1}{2} ( 2 u + 1 ) ( u − 1 ) = 0 ⟹ u = − 2 1 or u = 1 u = 1 u = 1 .
cos x = − 1 2 ⟹ x = 2 π 3 , 4 π 3 \cos x = -\frac{1}{2} \implies x = \frac{2\pi}{3}, \frac{4\pi}{3} cos x = − 2 1 ⟹ x = 3 2 π , 3 4 π
cos x = 1 ⟹ x = 0 , 2 π \cos x = 1 \implies x = 0, 2\pi cos x = 1 ⟹ x = 0 , 2 π
So x = 0 , 2 π 3 , 4 π 3 , 2 π x = 0, \frac{2\pi}{3}, \frac{4\pi}{3}, 2\pi x = 0 , 3 2 π , 3 4 π , 2 π .
Problem 5: Non-Right-Angled Triangle Problem: In triangle P Q R PQR P QR , p = 13 p = 13 p = 13 , q = 14 q = 14 q = 14 , r = 15 r = 15 r = 15 . Find the largest angle of the
triangle.
Solution:
The largest angle is opposite the longest side, so it is angle R R R (opposite r = 15 r = 15 r = 15 ).
Using the cosine rule:
cos R = 13 2 + 14 2 − 15 2 2 × 13 × 14 = 169 + 196 − 225 364 = 140 364 = 5 13 \cos R = \frac{13^2 + 14^2 - 15^2}{2 \times 13 \times 14} = \frac{169 + 196 - 225}{364} = \frac{140}{364} = \frac{5}{13} cos R = 2 × 13 × 14 1 3 2 + 1 4 2 − 1 5 2 = 364 169 + 196 − 225 = 364 140 = 13 5 R = arccos 5 13 ≈ 67.4 ∘ R = \arccos\frac{5}{13} \approx 67.4^{\circ} R = arccos 13 5 ≈ 67. 4 ∘
Problem 6: Trigonometric Proof Problem: Prove that tan 2 x − sin 2 x = tan 2 x sin 2 x \tan^2 x - \sin^2 x = \tan^2 x \sin^2 x tan 2 x − sin 2 x = tan 2 x sin 2 x .
Proof:
Starting from the LHS:
tan 2 x − sin 2 x = sin 2 x cos 2 x − sin 2 x = sin 2 x ( 1 cos 2 x − 1 ) = sin 2 x ⋅ 1 − cos 2 x cos 2 x = sin 2 x ⋅ sin 2 x cos 2 x = tan 2 x sin 2 x = R H S \tan^2 x - \sin^2 x = \frac{\sin^2 x}{\cos^2 x} - \sin^2 x = \sin^2 x\left(\frac{1}{\cos^2 x} - 1\right) = \sin^2 x \cdot \frac{1 - \cos^2 x}{\cos^2 x} = \sin^2 x \cdot \frac{\sin^2 x}{\cos^2 x} = \tan^2 x \sin^2 x = \mathrm{RHS} tan 2 x − sin 2 x = cos 2 x sin 2 x − sin 2 x = sin 2 x ( cos 2 x 1 − 1 ) = sin 2 x ⋅ cos 2 x 1 − cos 2 x = sin 2 x ⋅ cos 2 x sin 2 x = tan 2 x sin 2 x = RHS
Problem 7: Harmonic Form Problem: Express sin x + 3 cos x \sin x + \sqrt{3}\cos x sin x + 3 cos x in the form R sin ( x + α ) R\sin(x + \alpha) R sin ( x + α ) and state the maximum
value.
Solution:
R = 1 2 + ( 3 ) 2 = 1 + 3 = 2 R = \sqrt{1^2 + (\sqrt{3})^2} = \sqrt{1 + 3} = 2 R = 1 2 + ( 3 ) 2 = 1 + 3 = 2 tan α = 3 1 = 3 ⟹ α = π 3 \tan\alpha = \frac{\sqrt{3}}{1} = \sqrt{3} \implies \alpha = \frac{\pi}{3} tan α = 1 3 = 3 ⟹ α = 3 π So sin x + 3 cos x = 2 sin ( x + π 3 ) \sin x + \sqrt{3}\cos x = 2\sin\left(x + \frac{\pi}{3}\right) sin x + 3 cos x = 2 sin ( x + 3 π ) .
The maximum value is R = 2 R = 2 R = 2 , occurring when x + π 3 = π 2 + 2 n π x + \frac{\pi}{3} = \frac{\pi}{2} + 2n\pi x + 3 π = 2 π + 2 nπ , i.e.,
x = π 6 + 2 n π x = \frac{\pi}{6} + 2n\pi x = 6 π + 2 nπ .
Problem 8: 3D Trigonometry Problem: A cuboid has dimensions 5 × 4 × 3 5 \times 4 \times 3 5 × 4 × 3 cm. Find the angle that the diagonal of
the cuboid makes with the base.
Solution:
The space diagonal has length 5 2 + 4 2 + 3 2 = 50 = 5 2 \sqrt{5^2 + 4^2 + 3^2} = \sqrt{50} = 5\sqrt{2} 5 2 + 4 2 + 3 2 = 50 = 5 2 cm.
The projection of this diagonal onto the base has length 5 2 + 4 2 = 41 \sqrt{5^2 + 4^2} = \sqrt{41} 5 2 + 4 2 = 41 cm.
The angle θ \theta θ between the space diagonal and its projection onto the base is the angle with the
base:
sin θ = 3 5 2 = 3 2 10 \sin\theta = \frac{3}{5\sqrt{2}} = \frac{3\sqrt{2}}{10} sin θ = 5 2 3 = 10 3 2 θ = arcsin 3 2 10 ≈ 25.1 ∘ \theta = \arcsin\frac{3\sqrt{2}}{10} \approx 25.1^{\circ} θ = arcsin 10 3 2 ≈ 25. 1 ∘ Alternatively, using the tangent:
tan θ = 3 41 ⟹ θ = arctan 3 41 ≈ 25.1 ∘ \tan\theta = \frac{3}{\sqrt{41}} \implies \theta = \arctan\frac{3}{\sqrt{41}} \approx 25.1^{\circ} tan θ = 41 3 ⟹ θ = arctan 41 3 ≈ 25. 1 ∘
Related Content at Other Levels
Diagnostic Test
Ready to test your understanding of Trigonometry ? The diagnostic test contains the hardest questions within the IB specification for this topic, each with a full worked solution.
Unit tests probe edge cases and common misconceptions. Integration tests combine Trigonometry with other IB mathematics topics to test synthesis under exam conditions.
See Diagnostic Guide for instructions on self-marking and building a personal test matrix.