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Trigonometry

------- | ---------- | ------------------------------------------------------------------------ | | AQA | Paper 1, 2 | Basic” date: 2025-06-02T16:25:28.480Z tags:

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Intuition

Trigonometry is the mathematics of rotation and oscillation: The unit circle is the key, as you rotate around it, the xx-coordinate traces out cos⁡θ\cos\theta and the yy-coordinate traces out sin⁡θ\sin\theta. 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⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1 is just Pythagoras’ theorem applied to the unit circle. Every point on the unit circle satisfies x2+y2=1x^2 + y^2 = 1, and since x=cos⁡θx = \cos\theta and y=sin⁡θy = \sin\theta, the identity follows immediately. This is why trig identities are really just geometric relationships in disguise.

Board Coverage

BoardPaperNotes
AQAPaper 1, 2Basic trig in P1; compound/double angle, trig equations in P2
EdexcelP1, P2Similar split
OCR (A)Paper 1, 2Includes small angle approximations
CIE (9709)P1, P2, P3Trig functions in P1; identities and equations in P2; further trig in P3

1. The Unit Circle Definitions

Definition. Consider the unit circle (radius 1, centre at the origin). For an angle θ\theta Measured anticlockwise from the positive xx-axis, the point on the circle is (cos⁡θ,sin⁡θ)(\cos\theta, \sin\theta).

Definition.

cos⁡θ=thex−coordinateofthepointontheunitcircleatangleθ\cos\theta = \mathrm{the } x\mathrm{-coordinate of the point on the unit circle at angle } \theta sin⁡θ=they−coordinateofthepointontheunitcircleatangleθ\sin\theta = \mathrm{the } y\mathrm{-coordinate of the point on the unit circle at angle } \theta tan⁡θ=sin⁡θcos⁡θ(cos⁡θ≠0)\tan\theta = \frac{\sin\theta}{\cos\theta} \quad (\cos\theta \neq 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 and cos⁡\cos are periodic with period 2π2\pi.

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(radians)=arclengthr\theta\mathrm{ (radians)} = \frac{\mathrm{arc length}}{r}

The full circle: 2π2\pi radians =360∘= 360^\circ So π\pi radians =180∘= 180^\circ.

Theorem (Arc length and sector area). For a sector of radius rr and angle θ\theta (in Radians):

Arclengths=rθ\mathrm{Arc length } s = r\theta SectorareaA=12r2θ\mathrm{Sector area } A = \frac{1}{2}r^2\theta

Proof. By definition, θ=s/r\theta = s/r So s=rθs = r\theta. The sector is a fraction θ2π\frac{\theta}{2\pi} of the full circle (area πr2\pi r^2), so A=θ2π⋅πr2=12r2θA = \frac{\theta}{2\pi} \cdot \pi r^2 = \frac{1}{2}r^2\theta. ■\blacksquare


2. Fundamental Identities

2.1 Pythagorean Identity

Theorem. For all θ∈R\theta \in \mathbb{R}:

sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1

Proof. The point (cos⁡θ,sin⁡θ)(\cos\theta, \sin\theta) lies on the unit circle x2+y2=1x^2 + y^2 = 1.

cos⁡2θ+sin⁡2θ=1■\cos^2\theta + \sin^2\theta = 1 \quad \blacksquare

Corollary. Dividing by cos⁡2θ\cos^2\theta (where cos⁡θ≠0\cos\theta \neq 0):

1+tan⁡2θ=sec⁡2θ1 + \tan^2\theta = \sec^2\theta

Dividing by sin⁡2θ\sin^2\theta (where sin⁡θ≠0\sin\theta \neq 0):

cot⁡2θ+1=cosec⁡2θ\cot^2\theta + 1 = \cosec^2\theta

3. Compound Angle Formulas

3.1 Sine of a Sum

Theorem. For all A,B∈RA, B \in \mathbb{R}:

sin⁡(A+B)=sin⁡Acos⁡B+cos⁡Asin⁡B\sin(A + B) = \sin A \cos B + \cos A \sin B

Proof (using rotation matrices). Consider the rotation of the plane by angle AA followed by Rotation by angle BB. The combined rotation is by angle A+BA + B.

The rotation matrix by angle θ\theta is:

R(θ)=(cos⁡θ−sin⁡θsin⁡θcos⁡θ)R(\theta) = \begin{pmatrix} \cos\theta & -\sin\theta \\ \sin\theta & \cos\theta \end{pmatrix}

Matrix multiplication gives: R(A)R(B)=R(A+B)R(A)R(B) = R(A + B).

(cos⁡A−sin⁡Asin⁡Acos⁡A)(cos⁡B−sin⁡Bsin⁡Bcos⁡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}

The (2,1)(2, 1) entry of the product is:

sin⁡Acos⁡B+cos⁡Asin⁡B=sin⁡(A+B)■\sin A \cos B + \cos A \sin B = \sin(A + B) \quad \blacksquare

3.2 Cosine of a Sum

Theorem.

cos⁡(A+B)=cos⁡Acos⁡B−sin⁡Asin⁡B\cos(A + B) = \cos A \cos B - \sin A \sin B

Proof. From the (1,1)(1, 1) entry of the matrix product above:

cos⁡Acos⁡B−sin⁡Asin⁡B=cos⁡(A+B)■\cos A \cos B - \sin A \sin B = \cos(A + B) \quad \blacksquare

3.3 Tangent of a Sum

Theorem.

tan⁡(A+B)=tan⁡A+tan⁡B1−tan⁡Atan⁡B\tan(A + B) = \frac{\tan A + \tan B}{1 - \tan A \tan B}

Proof.

tan⁡(A+B)=sin⁡(A+B)cos⁡(A+B)=sin⁡Acos⁡B+cos⁡Asin⁡Bcos⁡Acos⁡B−sin⁡Asin⁡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}

Divide numerator and denominator by cos⁡Acos⁡B\cos A \cos B:

=tan⁡A+tan⁡B1−tan⁡Atan⁡B■= \frac{\tan A + \tan B}{1 - \tan A \tan B} \quad \blacksquare

3.4 Difference Formulas

Theorem.

sin⁡(A−B)=sin⁡Acos⁡B−cos⁡Asin⁡Bcos⁡(A−B)=cos⁡Acos⁡B+sin⁡Asin⁡Btan⁡(A−B)=tan⁡A−tan⁡B1+tan⁡Atan⁡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}

Proof. Replace BB with −B-B in the sum formulas, using sin⁡(−B)=−sin⁡B\sin(-B) = -\sin B and cos⁡(−B)=cos⁡B\cos(-B) = \cos B. ■\blacksquare


4. Double Angle Formulas

Setting A=BA = B in the compound angle formulas:

sin⁡2A=2sin⁡Acos⁡Acos⁡2A=cos⁡2A−sin⁡2Atan⁡2A=2tan⁡A1−tan⁡2A\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}

Theorem. Three equivalent forms of cos⁡2A\cos 2A:

cos⁡2A=cos⁡2A−sin⁡2A=2cos⁡2A−1=1−2sin⁡2A\cos 2A = \cos^2 A - \sin^2 A = 2\cos^2 A - 1 = 1 - 2\sin^2 A

Proof. Using sin⁡2A=1−cos⁡2A\sin^2 A = 1 - \cos^2 A:

cos⁡2A−sin⁡2A=cos⁡2A−(1−cos⁡2A)=2cos⁡2A−1\cos^2 A - \sin^2 A = \cos^2 A - (1 - \cos^2 A) = 2\cos^2 A - 1

Using cos⁡2A=1−sin⁡2A\cos^2 A = 1 - \sin^2 A:

cos⁡2A−sin⁡2A=(1−sin⁡2A)−sin⁡2A=1−2sin⁡2A\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 2A2A purely in terms of functions of AA. They are the algebraic backbone of many trigonometric manipulations and are essential for Integration.


5. Solving Trigonometric Equations

5.1 Basic Strategy

  1. Use identities to reduce to a single trigonometric function.
  2. Solve the resulting equation.
  3. Find all solutions in the required interval.

5.2 Key Solutions

sin⁡θ=a  ⟹  θ=arcsin⁡(a)+2nπorπ−arcsin⁡(a)+2nπcos⁡θ=a  ⟹  θ=±arccos⁡(a)+2nπtan⁡θ=a  ⟹  θ=arctan⁡(a)+nπ\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}

ExampleSolve 2sin⁡2θ+3cos⁡θ−3=02\sin^2\theta + 3\cos\theta - 3 = 0 for 0≤θ<2π0 \leq \theta < 2\pi.

Using sin⁡2θ=1−cos⁡2θ\sin^2\theta = 1 - \cos^2\theta:

2(1−cos⁡2θ)+3cos⁡θ−3=02(1 - \cos^2\theta) + 3\cos\theta - 3 = 0−2cos⁡2θ+3cos⁡θ−1=0-2\cos^2\theta + 3\cos\theta - 1 = 02cos⁡2θ−3cos⁡θ+1=02\cos^2\theta - 3\cos\theta + 1 = 0(2cos⁡θ−1)(cos⁡θ−1)=0(2\cos\theta - 1)(\cos\theta - 1) = 0

cos⁡θ=12  ⟹  θ=π3\cos\theta = \frac{1}{2} \implies \theta = \frac{\pi}{3} or 5π3\frac{5\pi}{3}.

cos⁡θ=1  ⟹  θ=0\cos\theta = 1 \implies \theta = 0.

Solutions: θ=0,π3,5π3\theta = 0, \frac{\pi}{3}, \frac{5\pi}{3}.


6. Small Angle Approximations

Theorem. For small θ\theta (in radians):

sin⁡θ≈θ−θ36cos⁡θ≈1−θ22tan⁡θ≈θ+θ33\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}

These follow from the Maclaurin series expansions (see Differentiation).

For the linear approximations (when θ\theta 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

Intuition. Near the origin, the curves y=sin⁡θy = \sin\theta and y=tan⁡θy = \tan\theta are almost Indistinguishable from the line y=θy = \theta. The curve y=cos⁡θy = \cos\theta is nearly flat at y=1y = 1.


7. Half-Angle Formulas

Theorem. For all θ\theta:

sin⁡θ2=±1−cos⁡θ2\sin\frac{\theta}{2} = \pm\sqrt{\frac{1 - \cos\theta}{2}} cos⁡θ2=±1+cos⁡θ2\cos\frac{\theta}{2} = \pm\sqrt{\frac{1 + \cos\theta}{2}} tan⁡θ2=sin⁡θ1+cos⁡θ=1−cos⁡θsin⁡θ\tan\frac{\theta}{2} = \frac{\sin\theta}{1 + \cos\theta} = \frac{1 - \cos\theta}{\sin\theta}

7.1 Derivation

Starting from cos⁡2A=1−2sin⁡2A\cos 2A = 1 - 2\sin^2 A and substituting A=θ2A = \frac{\theta}{2}:

cos⁡θ=1−2sin⁡2θ2\cos\theta = 1 - 2\sin^2\frac{\theta}{2} 2sin⁡2θ2=1−cos⁡θ2\sin^2\frac{\theta}{2} = 1 - \cos\theta sin⁡θ2=±1−cos⁡θ2■\sin\frac{\theta}{2} = \pm\sqrt{\frac{1 - \cos\theta}{2}} \quad \blacksquare

Similarly, from cos⁡2A=2cos⁡2A−1\cos 2A = 2\cos^2 A - 1:

cos⁡θ=2cos⁡2θ2−1\cos\theta = 2\cos^2\frac{\theta}{2} - 1 2cos⁡2θ2=1+cos⁡θ2\cos^2\frac{\theta}{2} = 1 + \cos\theta cos⁡θ2=±1+cos⁡θ2■\cos\frac{\theta}{2} = \pm\sqrt{\frac{1 + \cos\theta}{2}} \quad \blacksquare

7.2 Tangent Half-Angle Formulas

The tangent half-angle formulas avoid the ambiguity of the ±\pm sign:

tan⁡θ2=sin⁡θ1+cos⁡θ\tan\frac{\theta}{2} = \frac{\sin\theta}{1 + \cos\theta}

Proof. Using the double angle formulas:

sin⁡θ1+cos⁡θ=2sin⁡θ2cos⁡θ21+(2cos⁡2θ2−1)=2sin⁡θ2cos⁡θ22cos⁡2θ2=sin⁡θ2cos⁡θ2=tan⁡θ2■\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

Similarly:

tan⁡θ2=1−cos⁡θsin⁡θ\tan\frac{\theta}{2} = \frac{1 - \cos\theta}{\sin\theta}

Proof. 1−cos⁡θsin⁡θ=1−(1−2sin⁡2θ2)2sin⁡θ2cos⁡θ2=2sin⁡2θ22sin⁡θ2cos⁡θ2=sin⁡θ2cos⁡θ2=tan⁡θ2■\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

7.3 Sign Determination

The ±\pm in the sine and cosine half-angle formulas depends on the quadrant of θ2\frac{\theta}{2} Not the quadrant of θ\theta itself. Always determine which quadrant θ2\frac{\theta}{2} lies in Before choosing the sign.

Quadrant of θ2\frac{\theta}{2}sin⁡θ2\sin\frac{\theta}{2}cos⁡θ2\cos\frac{\theta}{2}
I: 0<θ2<π20 \lt \frac{\theta}{2} \lt \frac{\pi}{2}++++
II: π2<θ2<π\frac{\pi}{2} \lt \frac{\theta}{2} \lt \pi++−-
III: π<θ2<3π2\pi \lt \frac{\theta}{2} \lt \frac{3\pi}{2}−-−-
IV: 3π2<θ2<2π\frac{3\pi}{2} \lt \frac{\theta}{2} \lt 2\pi−-++

Worked exampleFind the exact value of sin⁡π8\sin\frac{\pi}{8}.

Since 0<π8<π20 \lt \frac{\pi}{8} \lt \frac{\pi}{2} (first quadrant), sin⁡π8>0\sin\frac{\pi}{8} > 0 So we Take the positive root.

sin⁡π8=1−cos⁡π42=1−222=2−24=2−22\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}

8. R-Addition Formula (Harmonic Form)

Theorem. For real numbers aa and bb:

asin⁡θ+bcos⁡θ=Rsin⁡(θ+α)a\sin\theta + b\cos\theta = R\sin(\theta + \alpha)

Where R=a2+b2R = \sqrt{a^2 + b^2} and tan⁡α=ba\tan\alpha = \dfrac{b}{a}.

8.1 Cosine Form

Alternatively, the same expression can be written as:

asin⁡θ+bcos⁡θ=Rcos⁡(θ−β)a\sin\theta + b\cos\theta = R\cos(\theta - \beta)

Where R=a2+b2R = \sqrt{a^2 + b^2} and tan⁡β=ab\tan\beta = \dfrac{a}{b}.

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:

Rsin⁡(θ+α)=Rsin⁡θcos⁡α+Rcos⁡θsin⁡αR\sin(\theta + \alpha) = R\sin\theta\cos\alpha + R\cos\theta\sin\alpha

Equating coefficients with asin⁡θ+bcos⁡θa\sin\theta + b\cos\theta:

Rcos⁡α=a,Rsin⁡α=bR\cos\alpha = a, \qquad R\sin\alpha = b

Squaring and adding: R2cos⁡2α+R2sin⁡2α=a2+b2R^2\cos^2\alpha + R^2\sin^2\alpha = a^2 + b^2 So R2=a2+b2R^2 = a^2 + b^2 and R=a2+b2R = \sqrt{a^2 + b^2}.

Dividing the second equation by the first: tan⁡α=ba\tan\alpha = \dfrac{b}{a}. ■\blacksquare

The cosine form is derived similarly by expanding Rcos⁡(θ−β)=Rcos⁡θcos⁡β+Rsin⁡θsin⁡βR\cos(\theta - \beta) = R\cos\theta\cos\beta + R\sin\theta\sin\beta and equating coefficients.

8.3 Applications: Maximum and Minimum

Since −1≤sin⁡(θ+α)≤1-1 \leq \sin(\theta + \alpha) \leq 1:

−R≤asin⁡θ+bcos⁡θ≤R-R \leq a\sin\theta + b\cos\theta \leq R
  • Maximum =R=a2+b2= R = \sqrt{a^2 + b^2} Occurring when θ+α=π2+2nπ\theta + \alpha = \frac{\pi}{2} + 2n\pi.
  • Minimum =−R= -R Occurring when θ+α=3π2+2nπ\theta + \alpha = \frac{3\pi}{2} + 2n\pi.

Example: Finding maximum and minimumFind the maximum and minimum values of 3sin⁡θ−4cos⁡θ3\sin\theta - 4\cos\theta and the values of θ\theta at which they occur, for 0≤θ<2π0 \leq \theta \lt 2\pi.

R=9+16=5R = \sqrt{9 + 16} = 5.

Here a=3a = 3 and b=−4b = -4. Writing 3sin⁡θ−4cos⁡θ=5sin⁡(θ+α)3\sin\theta - 4\cos\theta = 5\sin(\theta + \alpha) where tan⁡α=−43\tan\alpha = \dfrac{-4}{3} So α=−arctan⁡43\alpha = -\arctan\dfrac{4}{3}.

Maximum =5= 5 when θ+α=π2\theta + \alpha = \frac{\pi}{2}:

θ=π2−α=π2+arctan⁡43≈2.214rad\theta = \frac{\pi}{2} - \alpha = \frac{\pi}{2} + \arctan\frac{4}{3} \approx 2.214 \mathrm{ rad}

Minimum =−5= -5 when θ+α=3π2\theta + \alpha = \frac{3\pi}{2}:

θ=3π2−α=3π2+arctan⁡43≈5.356rad\theta = \frac{3\pi}{2} - \alpha = \frac{3\pi}{2} + \arctan\frac{4}{3} \approx 5.356 \mathrm{ rad}

8.4 Solving Equations

The R-addition formula converts asin⁡θ+bcos⁡θ=ka\sin\theta + b\cos\theta = k into Rsin⁡(θ+α)=kR\sin(\theta + \alpha) = k A Standard trigonometric equation.

Example: Solving an equationSolve sin⁡θ+cos⁡θ=1\sin\theta + \cos\theta = 1 for 0≤θ<2π0 \leq \theta \lt 2\pi.

R=1+1=2R = \sqrt{1 + 1} = \sqrt{2}, α=arctan⁡1=π4\alpha = \arctan 1 = \frac{\pi}{4}.

2sin⁡ ⁣(θ+π4)=1\sqrt{2}\sin\!\left(\theta + \frac{\pi}{4}\right) = 1sin⁡ ⁣(θ+π4)=12=sin⁡π4\sin\!\left(\theta + \frac{\pi}{4}\right) = \frac{1}{\sqrt{2}} = \sin\frac{\pi}{4}θ+π4=π4+2nπorθ+π4=3π4+2nπ\theta + \frac{\pi}{4} = \frac{\pi}{4} + 2n\pi \quad \mathrm{or} \quad \theta + \frac{\pi}{4} = \frac{3\pi}{4} + 2n\piθ=2nπorθ=π2+2nπ\theta = 2n\pi \quad \mathrm{or} \quad \theta = \frac{\pi}{2} + 2n\pi

For 0≤θ<2π0 \leq \theta \lt 2\pi: θ=0\theta = 0 or θ=π2\theta = \frac{\pi}{2}.


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, sec⁡\sec, csc⁡\csc, cot⁡\cot with their definitions in terms of sin⁡\sin and cos⁡\cos: tan⁡θ=sin⁡θcos⁡θ\tan\theta = \frac{\sin\theta}{\cos\theta}, sec⁡θ=1cos⁡θ\sec\theta = \frac{1}{\cos\theta} 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±ba \pm b in a denominator or numerator, multiply top and Bottom by the conjugate a∓ba \mp b to produce a difference of squares.

Example 1: Strategy 2 (express in sin and cos)Prove that cot⁡A+tan⁡A=2sin⁡2A\cot A + \tan A = \dfrac{2}{\sin 2A}.

cot⁡A+tan⁡A=cos⁡Asin⁡A+sin⁡Acos⁡A=cos⁡2A+sin⁡2Asin⁡Acos⁡A=1sin⁡Acos⁡A=22sin⁡Acos⁡A=2sin⁡2A■\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}

Example 2: Strategy 3 (use known identities)Prove that sin⁡3A=3sin⁡A−4sin⁡3A\sin 3A = 3\sin A - 4\sin^3 A.

sin⁡3A=sin⁡(2A+A)=sin⁡2Acos⁡A+cos⁡2Asin⁡A=2sin⁡Acos⁡2A+(1−2sin⁡2A)sin⁡A=2sin⁡A(1−sin⁡2A)+sin⁡A−2sin⁡3A=2sin⁡A−2sin⁡3A+sin⁡A−2sin⁡3A=3sin⁡A−4sin⁡3A■\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}

Example 3: Strategy 4 (multiply by conjugate)Prove that 1sec⁡A+tan⁡A=sec⁡A−tan⁡A\dfrac{1}{\sec A + \tan A} = \sec A - \tan A.

Multiply numerator and denominator by sec⁡A−tan⁡A\sec A - \tan A:

1sec⁡A+tan⁡A⋅sec⁡A−tan⁡Asec⁡A−tan⁡A=sec⁡A−tan⁡Asec⁡2A−tan⁡2A=sec⁡A−tan⁡A1+tan⁡2A−tan⁡2A=sec⁡A−tan⁡A1=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}

Where we used sec⁡2A=1+tan⁡2A\sec^2 A = 1 + \tan^2 A so that sec⁡2A−tan⁡2A=1\sec^2 A - \tan^2 A = 1.

Example 4: Strategy 1 (work with one side)Prove that cos⁡2A1+sin⁡2A=cos⁡A−sin⁡Acos⁡A+sin⁡A\dfrac{\cos 2A}{1 + \sin 2A} = \dfrac{\cos A - \sin A}{\cos A + \sin A}.

Working from the LHS:

cos⁡2A1+sin⁡2A=cos⁡2A−sin⁡2A1+2sin⁡Acos⁡A=(cos⁡A−sin⁡A)(cos⁡A+sin⁡A)cos⁡2A+2sin⁡Acos⁡A+sin⁡2A=(cos⁡A−sin⁡A)(cos⁡A+sin⁡A)(cos⁡A+sin⁡A)2=cos⁡A−sin⁡Acos⁡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}

10. Trigonometric Graphs

10.1 Key Features

FunctionPeriodAmplitudeDomainRange
sin⁡x\sin x2π2\pi11R\mathbb{R}[−1,1][-1, 1]
cos⁡x\cos x2π2\pi11R\mathbb{R}[−1,1][-1, 1]
tan⁡x\tan xπ\piundefinedx≠π2+nπx \neq \frac{\pi}{2} + n\piR\mathbb{R}

Key values of sin⁡\sin and cos⁡\cos:

Angle00π6\frac{\pi}{6}π4\frac{\pi}{4}π3\frac{\pi}{3}π2\frac{\pi}{2}π\pi3π2\frac{3\pi}{2}2π2\pi
sin⁡\sin0012\frac{1}{2}22\frac{\sqrt{2}}{2}32\frac{\sqrt{3}}{2}1100−1-100
cos⁡\cos1132\frac{\sqrt{3}}{2}22\frac{\sqrt{2}}{2}12\frac{1}{2}00−1-10011

10.2 Transformations

For the general form y=Asin⁡(Bx+C)+Dy = A\sin(Bx + C) + D (and similarly for cos⁡\cos):

  • ∣A∣|A| is the amplitude (vertical stretch from the midline)
  • The period is 2π∣B∣\dfrac{2\pi}{|B|}
  • The phase shift is −CB-\dfrac{C}{B} (horizontal shift)
  • DD is the vertical shift (midline is y=Dy = D)

For tan⁡\tan The period is π∣B∣\dfrac{\pi}{|B|} 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=Asin⁡(Bx+C)+Dy = A\sin(Bx + C) + D.

Worked exampleDescribe the key features of y=2sin⁡ ⁣(2x−π3)y = 2\sin\!\left(2x - \frac{\pi}{3}\right) for 0≤x≤2π0 \leq x \leq 2\pi. Amplitude: ∣A∣=2|A| = 2 So the range is [−2,2][-2, 2]. Period: 2π∣B∣=2π2=π\dfrac{2\pi}{|B|} = \dfrac{2\pi}{2} = \pi. Phase shift: −CB=−−π/32=π6-\dfrac{C}{B} = -\dfrac{-\pi/3}{2} = \dfrac{\pi}{6} (shift right by π6\frac{\pi}{6}). Key points. The first cycle begins at x=π6x = \frac{\pi}{6} (where the curve crosses the midline Upward). Subsequent key points within [0,2π][0, 2\pi]: - Maximum at x=5π12x = \frac{5\pi}{12} (value 22) - Midline crossing (down) at x=2π3x = \frac{2\pi}{3} - Minimum at x=11π12x = \frac{11\pi}{12} (value −2-2) - Midline crossing (up) at x=7π6x = \frac{7\pi}{6} Since the period is π\pi The second cycle repeats with all xx-values shifted by π\pi: - Maximum at x=17π12x = \frac{17\pi}{12} (value 22) - Minimum at x=23π12x = \frac{23\pi}{12} (value −2-2) yy-intercept: y=2sin⁡ ⁣(−π3)=−3≈−1.73y = 2\sin\!\left(-\frac{\pi}{3}\right) = -\sqrt{3} \approx -1.73.

11. Problem Set

Problem 1. Prove that sin⁡2θ1+cos⁡2θ=tan⁡θ\frac{\sin 2\theta}{1 + \cos 2\theta} = \tan\theta.

Solutionsin⁡2θ1+cos⁡2θ=2sin⁡θcos⁡θ1+(2cos⁡2θ−1)=2sin⁡θcos⁡θ2cos⁡2θ=sin⁡θcos⁡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}

If you get this wrong, revise: Double angle formulas


Problem 2. Solve sin⁡2x=sin⁡x\sin 2x = \sin x for 0≤x<2π0 \leq x < 2\pi.

Solution2sin⁡xcos⁡x=sin⁡x2\sin x\cos x = \sin xsin⁡x(2cos⁡x−1)=0\sin x(2\cos x - 1) = 0

sin⁡x=0  ⟹  x=0,π\sin x = 0 \implies x = 0, \pi.

2cos⁡x−1=0  ⟹  cos⁡x=12  ⟹  x=π3,5π32\cos x - 1 = 0 \implies \cos x = \frac{1}{2} \implies x = \frac{\pi}{3}, \frac{5\pi}{3}.

Solutions: x=0,π3,π,5π3x = 0, \frac{\pi}{3}, \pi, \frac{5\pi}{3}.

If you get this wrong, revise: Solving trig equations


Problem 3. Express 4sin⁡θ−3cos⁡θ4\sin\theta - 3\cos\theta in the form Rsin⁡(θ−α)R\sin(\theta - \alpha) Where R>0R > 0 and 0<α<π20 < \alpha < \frac{\pi}{2}.

SolutionRsin⁡(θ−α)=R(sin⁡θcos⁡α−cos⁡θsin⁡α)=Rcos⁡αsin⁡θ−Rsin⁡αcos⁡θR\sin(\theta - \alpha) = R(\sin\theta\cos\alpha - \cos\theta\sin\alpha) = R\cos\alpha\sin\theta - R\sin\alpha\cos\theta.

Comparing coefficients: Rcos⁡α=4R\cos\alpha = 4 and Rsin⁡α=3R\sin\alpha = 3.

R2=42+32=25  ⟹  R=5R^2 = 4^2 + 3^2 = 25 \implies R = 5tan⁡α=34  ⟹  α=arctan⁡(34)≈0.6435rad\tan\alpha = \frac{3}{4} \implies \alpha = \arctan\left(\frac{3}{4}\right) \approx 0.6435 \mathrm{ rad}4sin⁡θ−3cos⁡θ=5sin⁡(θ−0.6435)4\sin\theta - 3\cos\theta = 5\sin(\theta - 0.6435)

If you get this wrong, revise: Compound angle formulas


Problem 4. Find the exact value of sin⁡75∘\sin 75^\circ.

Solutionsin⁡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=22⋅32+22⋅12=6+24= \frac{\sqrt{2}}{2} \cdot \frac{\sqrt{3}}{2} + \frac{\sqrt{2}}{2} \cdot \frac{1}{2} = \frac{\sqrt{6} + \sqrt{2}}{4}

If you get this wrong, revise: Compound angle formulas


Problem 5. Prove that 1−cos⁡2θsin⁡2θ=tan⁡θ\frac{1 - \cos 2\theta}{\sin 2\theta} = \tan\theta.

Solution1−cos⁡2θsin⁡2θ=1−(1−2sin⁡2θ)2sin⁡θcos⁡θ=2sin⁡2θ2sin⁡θcos⁡θ=sin⁡θcos⁡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}

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.

SolutionArc length: s=rθ=8×1.2=9.6s = r\theta = 8 \times 1.2 = 9.6 cm.

Area: A=12r2θ=12(64)(1.2)=38.4A = \frac{1}{2}r^2\theta = \frac{1}{2}(64)(1.2) = 38.4 cm².

If you get this wrong, revise: Radian measure


Problem 7. Solve 3cos⁡2x+2sin⁡x−2=03\cos^2 x + 2\sin x - 2 = 0 for −π≤x≤π-\pi \leq x \leq \pi.

Solution3(1−sin⁡2x)+2sin⁡x−2=03(1 - \sin^2 x) + 2\sin x - 2 = 0

3−3sin⁡2x+2sin⁡x−2=03 - 3\sin^2 x + 2\sin x - 2 = 0

−3sin⁡2x+2sin⁡x+1=0-3\sin^2 x + 2\sin x + 1 = 0

3sin⁡2x−2sin⁡x−1=03\sin^2 x - 2\sin x - 1 = 0

(3sin⁡x+1)(sin⁡x−1)=0(3\sin x + 1)(\sin x - 1) = 0

sin⁡x=−13  ⟹  x=arcsin⁡(−13)≈−0.3398\sin x = -\frac{1}{3} \implies x = \arcsin(-\frac{1}{3}) \approx -0.3398 or x=−π−arcsin⁡(−13)=−π+0.3398≈−2.802x = -\pi - \arcsin(-\frac{1}{3}) = -\pi + 0.3398 \approx -2.802 (since 3.481>π3.481 > \pi Subtract 2π2\pi to stay in [−π,π][-\pi, \pi]).

sin⁡x=1  ⟹  x=π2\sin x = 1 \implies x = \frac{\pi}{2}.

Solutions: x≈−2.802,−0.340,π2x \approx -2.802, -0.340, \frac{\pi}{2}.

If you get this wrong, revise: Solving trig equations


Problem 8. Use small angle approximations to estimate sin⁡0.05cos⁡0.05\frac{\sin 0.05}{\cos 0.05}.

Solutionsin⁡0.05≈0.05\sin 0.05 \approx 0.05

cos⁡0.05≈1−0.0522=1−0.00125=0.99875\cos 0.05 \approx 1 - \frac{0.05^2}{2} = 1 - 0.00125 = 0.99875

sin⁡0.05cos⁡0.05≈0.050.99875≈0.05006\frac{\sin 0.05}{\cos 0.05} \approx \frac{0.05}{0.99875} \approx 0.05006

(Alternatively, tan⁡0.05≈0.05\tan 0.05 \approx 0.05 directly.)

If you get this wrong, revise: Small angle approximations


Problem 9. Prove that 1+sin⁡2Acos⁡2A=tan⁡ ⁣(A+π4)\dfrac{1 + \sin 2A}{\cos 2A} = \tan\!\left(A + \dfrac{\pi}{4}\right).

SolutionWorking from the LHS:

1+sin⁡2Acos⁡2A=1+2sin⁡Acos⁡Acos⁡2A−sin⁡2A=sin⁡2A+2sin⁡Acos⁡A+cos⁡2A(cos⁡A−sin⁡A)(cos⁡A+sin⁡A)=(sin⁡A+cos⁡A)2(cos⁡A−sin⁡A)(cos⁡A+sin⁡A)=sin⁡A+cos⁡Acos⁡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}

Dividing numerator and denominator by cos⁡A\cos A:

=tan⁡A+11−tan⁡A= \frac{\tan A + 1}{1 - \tan A}

From the tangent compound angle formula:

tan⁡ ⁣(A+π4)=tan⁡A+tan⁡π41−tan⁡Atan⁡π4=tan⁡A+11−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

If you get this wrong, revise: Compound angle formulas


Problem 10. The area of a sector is 20cm220\mathrm{ cm}^2 and the arc length is 10cm10\mathrm{ cm}. Find the radius and the angle.

Solutions=rθ=10  ⟹  θ=10rs = r\theta = 10 \implies \theta = \frac{10}{r}A=12r2θ=12r2⋅10r=5r=20  ⟹  r=4A = \frac{1}{2}r^2\theta = \frac{1}{2}r^2 \cdot \frac{10}{r} = 5r = 20 \implies r = 4θ=104=2.5radians\theta = \frac{10}{4} = 2.5 \mathrm{ radians}

If you get this wrong, revise: Radian measure


Problem 11. Find the exact value of cos⁡π12\cos\dfrac{\pi}{12} using a half-angle formula.

Solutioncos⁡π12=cos⁡π/62\cos\frac{\pi}{12} = \cos\frac{\pi/6}{2} So we apply the half-angle formula with θ=π6\theta = \frac{\pi}{6}.

Since 0<π12<π20 \lt \frac{\pi}{12} \lt \frac{\pi}{2} (first quadrant), cos⁡π12>0\cos\frac{\pi}{12} > 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⁡π12=cos⁡ ⁣(π3−π4)=cos⁡π3cos⁡π4+sin⁡π3sin⁡π4=6+24\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} and one can check that 2+32=6+24\dfrac{\sqrt{2+\sqrt{3}}}{2} = \dfrac{\sqrt{6}+\sqrt{2}}{4}.

If you get this wrong, revise: Half-angle formulas


Problem 12. Find the maximum value of 2sin⁡θ+5cos⁡θ2\sin\theta + 5\cos\theta and the smallest positive Value of θ\theta at which it occurs.

SolutionR=4+25=29R = \sqrt{4 + 25} = \sqrt{29}.

The maximum value is R=29R = \sqrt{29}.

Writing 2sin⁡θ+5cos⁡θ=29sin⁡(θ+α)2\sin\theta + 5\cos\theta = \sqrt{29}\sin(\theta + \alpha) where tan⁡α=52\tan\alpha = \dfrac{5}{2}.

The maximum occurs when sin⁡(θ+α)=1\sin(\theta + \alpha) = 1 I.e., θ+α=π2\theta + \alpha = \frac{\pi}{2}.

θ=π2−α=π2−arctan⁡52≈0.3805rad\theta = \frac{\pi}{2} - \alpha = \frac{\pi}{2} - \arctan\frac{5}{2} \approx 0.3805 \mathrm{ rad}

Since arctan⁡52≈1.1903<π2\arctan\frac{5}{2} \approx 1.1903 < \frac{\pi}{2} This θ\theta is positive and is the Smallest positive value.

If you get this wrong, revise: R-addition formula


Problem 13. Prove that sin⁡3Asin⁡A−cos⁡3Acos⁡A=2\dfrac{\sin 3A}{\sin A} - \dfrac{\cos 3A}{\cos A} = 2.

Solutionsin⁡3Asin⁡A−cos⁡3Acos⁡A=sin⁡3Acos⁡A−cos⁡3Asin⁡Asin⁡Acos⁡A=sin⁡(3A−A)sin⁡Acos⁡A=sin⁡2Asin⁡Acos⁡A=2sin⁡Acos⁡Asin⁡Acos⁡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}

If you get this wrong, revise: Proof strategies


Problem 14. Solve sin⁡θ+3cos⁡θ=1\sin\theta + \sqrt{3}\cos\theta = 1 for 0≤θ<2π0 \leq \theta \lt 2\pi.

SolutionR=1+3=2R = \sqrt{1 + 3} = 2, α=arctan⁡3=π3\alpha = \arctan\sqrt{3} = \frac{\pi}{3}.

2sin⁡ ⁣(θ+π3)=12\sin\!\left(\theta + \frac{\pi}{3}\right) = 1sin⁡ ⁣(θ+π3)=12\sin\!\left(\theta + \frac{\pi}{3}\right) = \frac{1}{2}θ+π3=π6+2nπorθ+π3=5π6+2nπ\theta + \frac{\pi}{3} = \frac{\pi}{6} + 2n\pi \quad \mathrm{or} \quad \theta + \frac{\pi}{3} = \frac{5\pi}{6} + 2n\pi

Case 1: θ=π6−π3+2nπ=−π6+2nπ\theta = \frac{\pi}{6} - \frac{\pi}{3} + 2n\pi = -\frac{\pi}{6} + 2n\pi.

For n=1n = 1: θ=−π6+2π=11π6\theta = -\frac{\pi}{6} + 2\pi = \frac{11\pi}{6}.

Case 2: θ=5π6−π3+2nπ=π2+2nπ\theta = \frac{5\pi}{6} - \frac{\pi}{3} + 2n\pi = \frac{\pi}{2} + 2n\pi.

For n=0n = 0: θ=π2\theta = \frac{\pi}{2}.

Solutions: θ=π2\theta = \frac{\pi}{2} or θ=11π6\theta = \frac{11\pi}{6}.

If you get this wrong, revise: R-addition formula


Problem 15. Prove that 1−tan⁡2A1+tan⁡2A=cos⁡2A\dfrac{1 - \tan^2 A}{1 + \tan^2 A} = \cos 2A.

SolutionUsing sec⁡2A=1+tan⁡2A\sec^2 A = 1 + \tan^2 A:

1−tan⁡2A1+tan⁡2A=1−tan⁡2Asec⁡2A=(1−tan⁡2A)cos⁡2A=cos⁡2A−tan⁡2Acos⁡2A=cos⁡2A−sin⁡2Acos⁡2A⋅cos⁡2A=cos⁡2A−sin⁡2A=cos⁡2A■\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}

If you get this wrong, revise: Proof strategies


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.