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  1. Subjects
  2. Maths AA
  3. 3 Geometry and trigonometry
  4. 3.8 Solving trigonometric equations

3.8 Solving trigonometric equations

Solve trigonometric equations on a given interval, exactly and with a GDC, including equations in 2x or x + c and equations that become quadratics in sin x, cos x or tan x.

  • IB Mathematics: Analysis and Approaches
  • Part of 3 Geometry and trigonometry
  • SL and HL

Key terms introduced here

Each is in the Maths AA glossary, with every other term in the subject.

Trigonometric equation

An equation involving circular functions of an unknown angle, such as 2sin⁡x=12\sin x = 12sinx=1. It usually has infinitely many solutions, so it is solved on a stated interval.

Notes on 3.8 Solving trigonometric equations

26 min readLast reviewed 14 Oct 2026

Learning objectives

  • Solve equations of the form sin⁡x=k\sin x = ksinx=k, cos⁡x=k\cos x = kcosx=k and tan⁡x=k\tan x = ktanx=k, finding every solution in a given interval.

  • Use the symmetry of the unit circle to find a second solution from the first.

  • Solve trigonometric equations graphically with a graphic display calculator (GDC).

  • Solve equations such as sin⁡2x=0.5\sin 2x = 0.5sin2x=0.5 and cos⁡(x−π3)=−12\cos\left(x - \frac{\pi}{3}\right) = -\frac{1}{2}cos(x−3π​)=−21​ by changing the interval.

  • Solve equations that lead to quadratic equations in sin⁡x\sin xsinx, cos⁡x\cos xcosx or tan⁡x\tan xtanx, rejecting impossible values.

  • Use the Pythagorean and double angle identities to rewrite an equation in terms of one circular function.

A trigonometric equation asks for the angles at which a circular function takes a given value: the times when the tide is 2 m deep, the angles at which a projectile reaches a given range, the moments when a wheel's capsule is level with a platform. Because circular functions repeat, such an equation usually has infinitely many solutions, and a question always says which interval of angles to search.

Solving one well uses three ideas together: the calculator (or an exact value) gives one solution, the symmetry of the unit circle gives a second, and the period of the function gives all the others. More complicated equations are reduced to these simple ones by algebra.

Scope: solving trigonometric equations in a finite interval, graphically and analytically, including equations that lead to quadratics. Exact values and the signs in each quadrant are in 3.5, the identities used are in 3.6 and solving quadratics is in 2.7. HL students meet further methods in 3.10 and 3.11.

What it means to solve a trigonometric equation

Definition

A trigonometric equation is an equation involving circular functions of an unknown angle, such as 2sin⁡x=12\sin x = 12sinx=1 or cos⁡2x=sin⁡x\cos 2x = \sin xcos2x=sinx. To solve it on an interval is to find every value of the unknown in that interval for which the equation is true.

Every time the graph of y=sin⁡xy = \sin xy=sinx crosses the line y=0.5y = 0.5y=0.5, there is a solution of sin⁡x=0.5\sin x = 0.5sinx=0.5. The sine curve keeps rising and falling forever, so it crosses the line twice in every cycle of length 2π2\pi2π, and there are infinitely many solutions.

−6−4−2024681012−1.5−1−0.500.511.5xyy = 0.5π/65π/613π/617π/6−7π/6−11π/6
  • y = sin x
The line y = 0.5 meets the sine curve twice in every cycle. Each pair of solutions is 2π further on than the previous pair.

The solutions in this graph are

x=π6+2kπorx=5π6+2kπ,k∈Zx = \frac{\pi}{6} + 2k\pi \quad \text{or} \quad x = \frac{5\pi}{6} + 2k\pi, \qquad k \in \mathbb{Z}x=6π​+2kπorx=65π​+2kπ,k∈Z

A question restricts the answer to an interval, such as 0≤x≤2π0 \le x \le 2\pi0≤x≤2π or −180∘<x≤180∘-180^\circ < x \le 180^\circ−180∘<x≤180∘, and the task is to list exactly the solutions inside it: no more and no fewer.

The value given by a calculator

The inverse functions on a calculator, written sin⁡−1\sin^{-1}sin−1, cos⁡−1\cos^{-1}cos−1 and tan⁡−1\tan^{-1}tan−1, return a single angle:

Function

Output range (radians)

Output range (degrees)

sin⁡−1k\sin^{-1} ksin−1k

−π2≤x≤π2-\frac{\pi}{2} \le x \le \frac{\pi}{2}−2π​≤x≤2π​

−90∘≤x≤90∘-90^\circ \le x \le 90^\circ−90∘≤x≤90∘

cos⁡−1k\cos^{-1} kcos−1k

0≤x≤π0 \le x \le \pi0≤x≤π

0∘≤x≤180∘0^\circ \le x \le 180^\circ0∘≤x≤180∘

tan⁡−1k\tan^{-1} ktan−1k

−π2<x<π2-\frac{\pi}{2} < x < \frac{\pi}{2}−2π​<x<2π​

−90∘<x<90∘-90^\circ < x < 90^\circ−90∘<x<90∘

This single value is one solution out of infinitely many. It may not even lie in the interval the question asks about, so it is a starting point, not the answer.

Common mistake

Writing down only the value the calculator gives. For sin⁡x=0.3\sin x = 0.3sinx=0.3, 0≤x≤2π0 \le x \le 2\pi0≤x≤2π, the calculator gives x=0.305x = 0.305x=0.305, but x=π−0.305=2.84x = \pi - 0.305 = 2.84x=π−0.305=2.84 is also a solution. Every solution in the interval must be listed.

Solving sin x = k, cos x = k and tan x = k

The second solution in each cycle comes from the symmetry of the unit circle. The point at angle xxx on the unit circle is (cos⁡x,sin⁡x)(\cos x, \sin x)(cosx,sinx), so an equation in sin⁡x\sin xsinx fixes the height of the point, an equation in cos⁡x\cos xcosx fixes its horizontal position, and an equation in tan⁡x\tan xtanx fixes the gradient of the radius.

Three unit circles. sin x = k: the line y = k meets the circle at angles α and π − α. cos x = k: the line x = k meets it at α and 2π − α. tan x = k: a line through O meets it at α and π + α. Each pair makes equal angles α with the x-axis.
Each equation is met at two points of the circle that make the same angle α with the x-axis: mirror images in the y-axis for sine, in the x-axis for cosine, and opposite ends of a diameter for tangent.
  • sin⁡x=k\sin x = ksinx=k: the horizontal line y=ky = ky=k meets the circle at two points that are reflections of each other in the yyy-axis. If one is at angle α\alphaα, the other is at π−α\pi - \alphaπ−α.

  • cos⁡x=k\cos x = kcosx=k: the vertical line x=kx = kx=k meets the circle at two points that are reflections in the xxx-axis, at angles α\alphaα and −α-\alpha−α. Within 0≤x≤2π0 \le x \le 2\pi0≤x≤2π, the second is written 2π−α2\pi - \alpha2π−α.

  • tan⁡x=k\tan x = ktanx=k: the line through OOO with gradient kkk meets the circle at the two ends of a diameter, at angles α\alphaα and π+α\pi + \alphaπ+α.

All other solutions come from adding or subtracting whole periods: 2π2\pi2π for sine and cosine, π\piπ for tangent. In degrees, the same rules read 180∘−α180^\circ - \alpha180∘−α, 360∘−α360^\circ - \alpha360∘−α and 180∘+α180^\circ + \alpha180∘+α, with periods 360∘360^\circ360∘ and 180∘180^\circ180∘.

Equation

First solution α\alphaα

Second solution

Add multiples of

sin⁡x=k\sin x = ksinx=k, −1≤k≤1-1 \le k \le 1−1≤k≤1

sin⁡−1k\sin^{-1} ksin−1k

π−α\pi - \alphaπ−α

2π2\pi2π

cos⁡x=k\cos x = kcosx=k, −1≤k≤1-1 \le k \le 1−1≤k≤1

cos⁡−1k\cos^{-1} kcos−1k

2π−α2\pi - \alpha2π−α (or −α-\alpha−α)

2π2\pi2π

tan⁡x=k\tan x = ktanx=k, any kkk

tan⁡−1k\tan^{-1} ktan−1k

π+α\pi + \alphaπ+α

π\piπ (the second solution is already one period on)

sin⁡x=k\sin x = ksinx=k and cos⁡x=k\cos x = kcosx=k have no solutions when k>1k > 1k>1 or k<−1k < -1k<−1, because sine and cosine never leave the interval [−1,1][-1, 1][−1,1]. A value such as sin⁡x=1.5\sin x = 1.5sinx=1.5 is impossible and is rejected, not solved.

A method for every interval

  1. Rearrange the equation to the form sin⁡x=k\sin x = ksinx=k, cos⁡x=k\cos x = kcosx=k or tan⁡x=k\tan x = ktanx=k.

  2. Find one solution α\alphaα, exactly (from the unit circle and the related angle, 3.5) or with the calculator.

  3. Use the symmetry rule to find the second solution in the same cycle.

  4. Add or subtract the period to both solutions until every value in the interval has been found, and discard any outside it.

  5. Check the count: a sine or cosine equation with −1<k<1-1 < k < 1−1<k<1 has two solutions in each full cycle.

A sketch of the graph and the horizontal line y=ky = ky=k over the interval shows how many solutions to expect before any calculation.

Worked example

Solve 2sin⁡x=12\sin x = 12sinx=1 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

Rearrange: sin⁡x=12\sin x = \frac{1}{2}sinx=21​.

The exact value sin⁡π6=12\sin\frac{\pi}{6} = \frac{1}{2}sin6π​=21​ gives α=π6\alpha = \frac{\pi}{6}α=6π​. Sine is positive, so the solutions lie in the first and second quadrants. The second solution is

π−π6=5π6\pi - \frac{\pi}{6} = \frac{5\pi}{6}π−6π​=65π​

Adding 2π2\pi2π to either value takes it beyond 2π2\pi2π, and subtracting 2π2\pi2π makes it negative, so there are no others.

x=π6orx=5π6x = \frac{\pi}{6} \quad \text{or} \quad x = \frac{5\pi}{6}x=6π​orx=65π​

The method works in the same way when the value is negative, but the calculator value often lies outside the interval and has to be moved into it first.

Worked example

Solve tan⁡x=−3\tan x = -\sqrt{3}tanx=−3​ for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

The related angle is π3\frac{\pi}{3}3π​, since tan⁡π3=3\tan\frac{\pi}{3} = \sqrt{3}tan3π​=3​. Tangent is negative in the second and fourth quadrants.

One solution is α=−π3\alpha = -\frac{\pi}{3}α=−3π​ (the calculator value), which lies outside the interval. Adding the period π\piπ repeatedly:

−π3+π=2π3−π3+2π=5π3-\frac{\pi}{3} + \pi = \frac{2\pi}{3} \qquad -\frac{\pi}{3} + 2\pi = \frac{5\pi}{3}−3π​+π=32π​−3π​+2π=35π​

The next value, 8π3\frac{8\pi}{3}38π​, is greater than 2π2\pi2π.

x=2π3orx=5π3x = \frac{2\pi}{3} \quad \text{or} \quad x = \frac{5\pi}{3}x=32π​orx=35π​

Check: 2π3\frac{2\pi}{3}32π​ is in the second quadrant and 5π3\frac{5\pi}{3}35π​ is in the fourth, where tangent is negative.

For a cosine equation, the second solution is the negative of the first. This form is the most convenient when the interval is centred on zero, such as −π≤x≤π-\pi \le x \le \pi−π≤x≤π.

Worked example

Solve cos⁡x=−22\cos x = -\frac{\sqrt{2}}{2}cosx=−22​​ for −π≤x≤π-\pi \le x \le \pi−π≤x≤π.

Show the solution

The related angle is π4\frac{\pi}{4}4π​, and cosine is negative in the second and third quadrants. The calculator value is

α=cos⁡−1(−22)=3π4\alpha = \cos^{-1}\left(-\frac{\sqrt{2}}{2}\right) = \frac{3\pi}{4}α=cos−1(−22​​)=43π​

For cosine the second solution is −α=−3π4-\alpha = -\frac{3\pi}{4}−α=−43π​, which lies in the interval. Adding or subtracting 2π2\pi2π to either value leaves the interval.

x=−3π4orx=3π4x = -\frac{3\pi}{4} \quad \text{or} \quad x = \frac{3\pi}{4}x=−43π​orx=43π​

When the value of kkk is not one of the exact values, the calculator gives α\alphaα as a decimal. Keep at least five significant figures in working and round only at the end.

Worked example

Solve the following equations, giving answers correct to 3 significant figures.

(a) 3cos⁡x=23\cos x = 23cosx=2 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π

(b) sin⁡x=−0.4\sin x = -0.4sinx=−0.4 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π

Show the solution

(a) cos⁡x=23\cos x = \frac{2}{3}cosx=32​, so α=cos⁡−123=0.84106…\alpha = \cos^{-1}\frac{2}{3} = 0.84106\ldotsα=cos−132​=0.84106… The second solution is 2π−0.84106…=5.44211…2\pi - 0.84106\ldots = 5.44211\ldots2π−0.84106…=5.44211…

x=0.841orx=5.44x = 0.841 \quad \text{or} \quad x = 5.44x=0.841orx=5.44

(b) α=sin⁡−1(−0.4)=−0.41151…\alpha = \sin^{-1}(-0.4) = -0.41151\ldotsα=sin−1(−0.4)=−0.41151…, which is outside the interval. The second solution in the same cycle is

π−(−0.41151…)=3.55311…\pi - (-0.41151\ldots) = 3.55311\ldotsπ−(−0.41151…)=3.55311…

and adding 2π2\pi2π to the first gives −0.41151…+2π=5.87166…-0.41151\ldots + 2\pi = 5.87166\ldots−0.41151…+2π=5.87166…

x=3.55orx=5.87x = 3.55 \quad \text{or} \quad x = 5.87x=3.55orx=5.87

Both lie in the third and fourth quadrants, where sine is negative.

Common mistake

Using the sine rule π−α\pi - \alphaπ−α for a cosine equation, or 2π−α2\pi - \alpha2π−α for a sine equation. For cos⁡x=23\cos x = \frac{2}{3}cosx=32​, π−0.841=2.30\pi - 0.841 = 2.30π−0.841=2.30 is not a solution: cos⁡2.30=−0.666\cos 2.30 = -0.666cos2.30=−0.666. Check each answer by substituting it back into the original equation.

When the interval is in degrees, the same rules apply with 180∘180^\circ180∘ and 360∘360^\circ360∘. For sin⁡θ=0.3\sin\theta = 0.3sinθ=0.3, 0∘≤θ≤360∘0^\circ \le \theta \le 360^\circ0∘≤θ≤360∘, the calculator in degree mode gives θ=17.5∘\theta = 17.5^\circθ=17.5∘, and the second solution is 180∘−17.5∘=162.5∘180^\circ - 17.5^\circ = 162.5^\circ180∘−17.5∘=162.5∘. Angles in degrees are given to 1 decimal place.

Values with only one solution per cycle

When k=1k = 1k=1, k=−1k = -1k=−1 or k=0k = 0k=0, the two symmetric points on the circle coincide or sit at the ends of the axes, and the general rules can produce repeated or misleading values. These cases are best read straight from the graph:

  • sin⁡x=1\sin x = 1sinx=1 only at x=π2+2kπx = \frac{\pi}{2} + 2k\pix=2π​+2kπ; sin⁡x=−1\sin x = -1sinx=−1 only at x=3π2+2kπx = \frac{3\pi}{2} + 2k\pix=23π​+2kπ;

  • cos⁡x=1\cos x = 1cosx=1 only at x=2kπx = 2k\pix=2kπ; cos⁡x=−1\cos x = -1cosx=−1 only at x=π+2kπx = \pi + 2k\pix=π+2kπ;

  • sin⁡x=0\sin x = 0sinx=0 at x=kπx = k\pix=kπ; cos⁡x=0\cos x = 0cosx=0 at x=π2+kπx = \frac{\pi}{2} + k\pix=2π​+kπ; tan⁡x=0\tan x = 0tanx=0 at x=kπx = k\pix=kπ.

For example, cos⁡x=1\cos x = 1cosx=1 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π has the two solutions x=0x = 0x=0 and x=2πx = 2\pix=2π, both end points of the interval, while sin⁡x=1\sin x = 1sinx=1 on the same interval has only x=π2x = \frac{\pi}{2}x=2π​.

Solving trigonometric equations graphically

Some trigonometric equations mix different functions or angles in a way that has no algebraic method at this level, such as 3sin⁡2x+1=2cos⁡x3\sin 2x + 1 = 2\cos x3sin2x+1=2cosx. A GDC solves them graphically: graph each side as a separate function and find the xxx-coordinates of the points of intersection. Alternatively, graph the difference of the two sides and find its zeros.

Worked example

Use a GDC to solve 3sin⁡2x+1=2cos⁡x3\sin 2x + 1 = 2\cos x3sin2x+1=2cosx for 0≤x≤π0 \le x \le \pi0≤x≤π.

Show the solution

Set the GDC to radians and the viewing window to 0≤x≤π0 \le x \le \pi0≤x≤π. Graph y=3sin⁡2x+1y = 3\sin 2x + 1y=3sin2x+1 and y=2cos⁡xy = 2\cos xy=2cosx and use the intersect function at each crossing.

00.511.522.53−2−101234xyx = 0.165x = 1.84x = 2.58
  • y = 3sin 2x + 1
  • y = 2cos x
The two graphs cross three times between 0 and π, so the equation has three solutions there.
x=0.165,x=1.84orx=2.58(3 s.f.)x = 0.165, \quad x = 1.84 \quad \text{or} \quad x = 2.58 \quad (3 \text{ s.f.})x=0.165,x=1.84orx=2.58(3 s.f.)

Tip

Before reading off intersections, check that the viewing window covers exactly the interval in the question and that both graphs fit vertically. A crossing just outside the window, or one hidden by a window that is too short, is easy to miss.

Equations with a transformed angle

An equation such as sin⁡2x=0.5\sin 2x = 0.5sin2x=0.5 involves the function of 2x2x2x, not of xxx. The graph of y=sin⁡2xy = \sin 2xy=sin2x has period π\piπ, so it completes two cycles for every one cycle of y=sin⁡xy = \sin xy=sinx, and the equation has twice as many solutions in 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

The method is to treat the whole angle as a new unknown, solve for that, and convert back:

  1. Let uuu be the angle inside the function (for example u=2xu = 2xu=2x, or u=x−π3u = x - \frac{\pi}{3}u=x−3π​).

  2. Transform the interval for xxx into an interval for uuu, by applying to its end points the same operations that turn xxx into uuu.

  3. Solve the simple equation for uuu on the new interval, finding every solution.

  4. Convert each value of uuu back to xxx.

Worked example

Solve sin⁡2x=0.5\sin 2x = 0.5sin2x=0.5 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

Let u=2xu = 2xu=2x. Since 0≤x≤2π0 \le x \le 2\pi0≤x≤2π, multiplying by 222 gives 0≤u≤4π0 \le u \le 4\pi0≤u≤4π: two full cycles.

Solve sin⁡u=0.5\sin u = 0.5sinu=0.5 for 0≤u≤4π0 \le u \le 4\pi0≤u≤4π. The first cycle gives u=π6u = \frac{\pi}{6}u=6π​ and u=π−π6=5π6u = \pi - \frac{\pi}{6} = \frac{5\pi}{6}u=π−6π​=65π​. Adding 2π2\pi2π gives the second cycle:

u=π6, 5π6, 13π6, 17π6u = \frac{\pi}{6}, \ \frac{5\pi}{6}, \ \frac{13\pi}{6}, \ \frac{17\pi}{6}u=6π​, 65π​, 613π​, 617π​

Divide by 222 to return to xxx:

x=π12, 5π12, 13π12, 17π12x = \frac{\pi}{12}, \ \frac{5\pi}{12}, \ \frac{13\pi}{12}, \ \frac{17\pi}{12}x=12π​, 125π​, 1213π​, 1217π​
0123456−1.5−1−0.500.511.5xyy = 0.5π/125π/1213π/1217π/12
  • y = sin 2x
y = sin 2x completes two cycles between 0 and 2π, so the line y = 0.5 crosses it four times.

Common mistake

Solving sin⁡2x=0.5\sin 2x = 0.5sin2x=0.5 only for 0≤2x≤2π0 \le 2x \le 2\pi0≤2x≤2π and dividing by 222. This gives π12\frac{\pi}{12}12π​ and 5π12\frac{5\pi}{12}125π​ and misses the two solutions in the second cycle. Always change the interval before solving: if xxx runs from 000 to 2π2\pi2π, then 2x2x2x runs from 000 to 4π4\pi4π.

The same method handles a translation inside the function. The interval is shifted rather than stretched, and some solutions of the simple equation may fall outside the new interval.

Worked example

Solve 2cos⁡(x−π3)=−12\cos\left(x - \frac{\pi}{3}\right) = -12cos(x−3π​)=−1 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

cos⁡(x−π3)=−12\cos\left(x - \frac{\pi}{3}\right) = -\frac{1}{2}cos(x−3π​)=−21​. Let u=x−π3u = x - \frac{\pi}{3}u=x−3π​. Subtracting π3\frac{\pi}{3}3π​ from the end points gives

−π3≤u≤5π3-\frac{\pi}{3} \le u \le \frac{5\pi}{3}−3π​≤u≤35π​

Solve cos⁡u=−12\cos u = -\frac{1}{2}cosu=−21​: the related angle is π3\frac{\pi}{3}3π​ and cosine is negative in the second and third quadrants, so u=2π3u = \frac{2\pi}{3}u=32π​ or u=4π3u = \frac{4\pi}{3}u=34π​. Both lie in the interval; the next values, 2π3−2π\frac{2\pi}{3} - 2\pi32π​−2π and 4π3−2π=−2π3\frac{4\pi}{3} - 2\pi = -\frac{2\pi}{3}34π​−2π=−32π​, are below −π3-\frac{\pi}{3}−3π​.

Add π3\frac{\pi}{3}3π​ to return to xxx:

x=2π3+π3=πorx=4π3+π3=5π3x = \frac{2\pi}{3} + \frac{\pi}{3} = \pi \quad \text{or} \quad x = \frac{4\pi}{3} + \frac{\pi}{3} = \frac{5\pi}{3}x=32π​+3π​=πorx=34π​+3π​=35π​

The interval for uuu can also be larger than one cycle and start below zero, as in the next two examples.

Worked example

Solve the following equations.

(a) tan⁡3x=1\tan 3x = 1tan3x=1 for 0≤x≤π0 \le x \le \pi0≤x≤π

(b) 2cos⁡2x+1=02\cos 2x + 1 = 02cos2x+1=0 for −π≤x≤π-\pi \le x \le \pi−π≤x≤π

Show the solution

(a) Let u=3xu = 3xu=3x, so 0≤u≤3π0 \le u \le 3\pi0≤u≤3π. The equation tan⁡u=1\tan u = 1tanu=1 has α=π4\alpha = \frac{\pi}{4}α=4π​ and period π\piπ:

u=π4, 5π4, 9π4u = \frac{\pi}{4}, \ \frac{5\pi}{4}, \ \frac{9\pi}{4}u=4π​, 45π​, 49π​

(13π4>3π\frac{13\pi}{4} > 3\pi413π​>3π.) Dividing by 333:

x=π12, 5π12, 3π4x = \frac{\pi}{12}, \ \frac{5\pi}{12}, \ \frac{3\pi}{4}x=12π​, 125π​, 43π​

(b) cos⁡2x=−12\cos 2x = -\frac{1}{2}cos2x=−21​. Let u=2xu = 2xu=2x, so −2π≤u≤2π-2\pi \le u \le 2\pi−2π≤u≤2π. In 0≤u≤2π0 \le u \le 2\pi0≤u≤2π, cos⁡u=−12\cos u = -\frac{1}{2}cosu=−21​ gives u=2π3u = \frac{2\pi}{3}u=32π​ and 4π3\frac{4\pi}{3}34π​. Subtracting 2π2\pi2π gives the solutions in −2π≤u≤0-2\pi \le u \le 0−2π≤u≤0: u=−4π3u = -\frac{4\pi}{3}u=−34π​ and −2π3-\frac{2\pi}{3}−32π​. Dividing by 222:

x=−2π3, −π3, π3, 2π3x = -\frac{2\pi}{3}, \ -\frac{\pi}{3}, \ \frac{\pi}{3}, \ \frac{2\pi}{3}x=−32π​, −3π​, 3π​, 32π​

The four answers are symmetrical about 000, as expected for an equation in cos⁡2x\cos 2xcos2x.

In degrees, the working is identical. For sin⁡(2θ−30∘)=0.5\sin(2\theta - 30^\circ) = 0.5sin(2θ−30∘)=0.5 with 0∘≤θ≤360∘0^\circ \le \theta \le 360^\circ0∘≤θ≤360∘, the new angle u=2θ−30∘u = 2\theta - 30^\circu=2θ−30∘ runs from −30∘-30^\circ−30∘ to 690∘690^\circ690∘. The solutions u=30∘,150∘,390∘,510∘u = 30^\circ, 150^\circ, 390^\circ, 510^\circu=30∘,150∘,390∘,510∘ give θ=30∘,90∘,210∘,270∘\theta = 30^\circ, 90^\circ, 210^\circ, 270^\circθ=30∘,90∘,210∘,270∘.

Equations from sinusoidal models

A sinusoidal model from 3.7 leads to exactly this kind of equation whenever a question asks when the modelled quantity reaches a given value. In a simplified model of the London Eye, the height of a capsule ttt minutes after it leaves the lowest point is h(t)=60−60cos⁡(πt15)h(t) = 60 - 60\cos\left(\frac{\pi t}{15}\right)h(t)=60−60cos(15πt​) metres, with one revolution every 303030 minutes.

Worked example

Find, for one revolution of the wheel, the length of time for which the capsule is more than 909090 m above the ground.

Show the solution

First solve h(t)=90h(t) = 90h(t)=90 for 0≤t≤300 \le t \le 300≤t≤30:

60−60cos⁡(πt15)=90⇒cos⁡(πt15)=−1260 - 60\cos\left(\frac{\pi t}{15}\right) = 90 \quad \Rightarrow \quad \cos\left(\frac{\pi t}{15}\right) = -\frac{1}{2}60−60cos(15πt​)=90⇒cos(15πt​)=−21​

Let u=πt15u = \frac{\pi t}{15}u=15πt​; for 0≤t≤300 \le t \le 300≤t≤30, 0≤u≤2π0 \le u \le 2\pi0≤u≤2π. Then u=2π3u = \frac{2\pi}{3}u=32π​ or u=4π3u = \frac{4\pi}{3}u=34π​, so

t=15π×2π3=10ort=15π×4π3=20t = \frac{15}{\pi} \times \frac{2\pi}{3} = 10 \quad \text{or} \quad t = \frac{15}{\pi} \times \frac{4\pi}{3} = 20t=π15​×32π​=10ort=π15​×34π​=20

The capsule rises through 909090 m after 101010 minutes and falls back through it after 202020 minutes; the highest point (t=15t = 15t=15) lies between. It is above 909090 m for 20−10=1020 - 10 = 1020−10=10 minutes, one third of each revolution.

Equations leading to quadratic equations

Some trigonometric equations are quadratic equations in disguise. In 2sin⁡2x−sin⁡x−1=02\sin^2 x - \sin x - 1 = 02sin2x−sinx−1=0, the unknown sin⁡x\sin xsinx plays the part of yyy in 2y2−y−1=02y^2 - y - 1 = 02y2−y−1=0. Such an equation in quadratic form is solved in two stages: first solve the quadratic for sin⁡x\sin xsinx (2.7), then solve each resulting simple equation for xxx.

Remember the notation: sin⁡2x\sin^2 xsin2x means (sin⁡x)2(\sin x)^2(sinx)2.

Worked example

Solve 2sin⁡2x−sin⁡x−1=02\sin^2 x - \sin x - 1 = 02sin2x−sinx−1=0 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

Factorise the quadratic in sin⁡x\sin xsinx (it may help to write s=sin⁡xs = \sin xs=sinx, giving 2s2−s−1=02s^2 - s - 1 = 02s2−s−1=0):

(2sin⁡x+1)(sin⁡x−1)=0(2\sin x + 1)(\sin x - 1) = 0(2sinx+1)(sinx−1)=0

So sin⁡x=−12\sin x = -\frac{1}{2}sinx=−21​ or sin⁡x=1\sin x = 1sinx=1.

sin⁡x=1\sin x = 1sinx=1 gives x=π2x = \frac{\pi}{2}x=2π​ only.

sin⁡x=−12\sin x = -\frac{1}{2}sinx=−21​: the related angle is π6\frac{\pi}{6}6π​, and sine is negative in the third and fourth quadrants, so x=π+π6=7π6x = \pi + \frac{\pi}{6} = \frac{7\pi}{6}x=π+6π​=67π​ or x=2π−π6=11π6x = 2\pi - \frac{\pi}{6} = \frac{11\pi}{6}x=2π−6π​=611π​.

x=π2, 7π6, 11π6x = \frac{\pi}{2}, \ \frac{7\pi}{6}, \ \frac{11\pi}{6}x=2π​, 67π​, 611π​

Rejecting impossible values

One root of the quadratic may be a value that sine or cosine can never take. That root gives no solutions and is rejected with a reason.

Worked example

Solve cos⁡2x+2cos⁡x−3=0\cos^2 x + 2\cos x - 3 = 0cos2x+2cosx−3=0 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution
(cos⁡x+3)(cos⁡x−1)=0⇒cos⁡x=−3 or cos⁡x=1(\cos x + 3)(\cos x - 1) = 0 \quad \Rightarrow \quad \cos x = -3 \text{ or } \cos x = 1(cosx+3)(cosx−1)=0⇒cosx=−3 or cosx=1

Since −1≤cos⁡x≤1-1 \le \cos x \le 1−1≤cosx≤1 for all xxx, cos⁡x=−3\cos x = -3cosx=−3 has no solutions. From cos⁡x=1\cos x = 1cosx=1:

x=0orx=2πx = 0 \quad \text{or} \quad x = 2\pix=0orx=2π

When the quadratic does not factorise, use the quadratic formula, then a calculator for the angles.

Worked example

Solve tan⁡2x−3tan⁡x+1=0\tan^2 x - 3\tan x + 1 = 0tan2x−3tanx+1=0 for 0≤x≤π0 \le x \le \pi0≤x≤π, giving your answers correct to 3 significant figures.

Show the solution

By the quadratic formula with tan⁡x\tan xtanx as the unknown,

tan⁡x=3±9−42=3±52\tan x = \frac{3 \pm \sqrt{9 - 4}}{2} = \frac{3 \pm \sqrt{5}}{2}tanx=23±9−4​​=23±5​​

so tan⁡x=2.6180…\tan x = 2.6180\ldotstanx=2.6180… or tan⁡x=0.38196…\tan x = 0.38196\ldotstanx=0.38196…

Both values are positive, so the solutions lie in the first quadrant (and in the third, which is outside 0≤x≤π0 \le x \le \pi0≤x≤π). Adding the period π\piπ to either first-quadrant value takes it beyond π\piπ.

x=tan⁡−1(2.6180…)=1.21orx=tan⁡−1(0.38196…)=0.365x = \tan^{-1}(2.6180\ldots) = 1.21 \quad \text{or} \quad x = \tan^{-1}(0.38196\ldots) = 0.365x=tan−1(2.6180…)=1.21orx=tan−1(0.38196…)=0.365

Common factors: never divide by a function that could be zero

In an equation such as 2sin⁡xcos⁡x=sin⁡x2\sin x\cos x = \sin x2sinxcosx=sinx, dividing both sides by sin⁡x\sin xsinx looks tempting. It loses every solution where sin⁡x=0\sin x = 0sinx=0. Move every term to one side and factorise instead.

Common mistake

Dividing 2sin⁡xcos⁡x=sin⁡x2\sin x\cos x = \sin x2sinxcosx=sinx by sin⁡x\sin xsinx gives cos⁡x=12\cos x = \frac{1}{2}cosx=21​, and only x=π3,5π3x = \frac{\pi}{3}, \frac{5\pi}{3}x=3π​,35π​ in [0,2π][0, 2\pi][0,2π]. Factorising, sin⁡x(2cos⁡x−1)=0\sin x(2\cos x - 1) = 0sinx(2cosx−1)=0, keeps sin⁡x=0\sin x = 0sinx=0 as well, which adds x=0,π,2πx = 0, \pi, 2\pix=0,π,2π: five solutions in all.

Using identities to get one function

An equation that contains two different circular functions, or both xxx and 2x2x2x, can often be rewritten in terms of a single function of xxx with an identity from 3.6. The aim is either a quadratic in one function or a product of simple factors.

The equation contains

Identity to use

Result

cos⁡2x\cos^2 xcos2x and sin⁡x\sin xsinx

cos⁡2x=1−sin⁡2x\cos^2 x = 1 - \sin^2 xcos2x=1−sin2x

Quadratic in sin⁡x\sin xsinx

sin⁡2x\sin^2 xsin2x and cos⁡x\cos xcosx

sin⁡2x=1−cos⁡2x\sin^2 x = 1 - \cos^2 xsin2x=1−cos2x

Quadratic in cos⁡x\cos xcosx

sin⁡2x\sin 2xsin2x

sin⁡2x=2sin⁡xcos⁡x\sin 2x = 2\sin x\cos xsin2x=2sinxcosx

Usually a common factor

cos⁡2x\cos 2xcos2x and sin⁡x\sin xsinx

cos⁡2x=1−2sin⁡2x\cos 2x = 1 - 2\sin^2 xcos2x=1−2sin2x

Quadratic in sin⁡x\sin xsinx

cos⁡2x\cos 2xcos2x and cos⁡x\cos xcosx

cos⁡2x=2cos⁡2x−1\cos 2x = 2\cos^2 x - 1cos2x=2cos2x−1

Quadratic in cos⁡x\cos xcosx

sin⁡x\sin xsinx and cos⁡x\cos xcosx, both to the first power and no constant

divide by cos⁡x\cos xcosx (when cos⁡x≠0\cos x \neq 0cosx=0)

tan⁡x=k\tan x = ktanx=k

The Pythagorean identity

The Pythagorean identity cos⁡2x+sin⁡2x=1\cos^2 x + \sin^2 x = 1cos2x+sin2x=1 swaps a squared function for the other one.

Worked example

Solve 2cos⁡2x+sin⁡x=12\cos^2 x + \sin x = 12cos2x+sinx=1 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

Replace cos⁡2x\cos^2 xcos2x by 1−sin⁡2x1 - \sin^2 x1−sin2x so that only sin⁡x\sin xsinx appears:

2(1−sin⁡2x)+sin⁡x=1⇒2−2sin⁡2x+sin⁡x−1=0⇒2sin⁡2x−sin⁡x−1=02(1 - \sin^2 x) + \sin x = 1 \quad \Rightarrow \quad 2 - 2\sin^2 x + \sin x - 1 = 0 \quad \Rightarrow \quad 2\sin^2 x - \sin x - 1 = 02(1−sin2x)+sinx=1⇒2−2sin2x+sinx−1=0⇒2sin2x−sinx−1=0

This is the equation solved earlier: (2sin⁡x+1)(sin⁡x−1)=0(2\sin x + 1)(\sin x - 1) = 0(2sinx+1)(sinx−1)=0, so

x=π2, 7π6, 11π6x = \frac{\pi}{2}, \ \frac{7\pi}{6}, \ \frac{11\pi}{6}x=2π​, 67π​, 611π​

The same substitution works the other way round, turning sin⁡2x\sin^2 xsin2x into an expression in cos⁡x\cos xcosx.

Worked example

Solve 2sin⁡2x=3cos⁡x2\sin^2 x = 3\cos x2sin2x=3cosx for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution
2(1−cos⁡2x)=3cos⁡x⇒2cos⁡2x+3cos⁡x−2=0⇒(2cos⁡x−1)(cos⁡x+2)=02(1 - \cos^2 x) = 3\cos x \quad \Rightarrow \quad 2\cos^2 x + 3\cos x - 2 = 0 \quad \Rightarrow \quad (2\cos x - 1)(\cos x + 2) = 02(1−cos2x)=3cosx⇒2cos2x+3cosx−2=0⇒(2cosx−1)(cosx+2)=0

cos⁡x=−2\cos x = -2cosx=−2 is impossible. cos⁡x=12\cos x = \frac{1}{2}cosx=21​ gives

x=π3orx=2π−π3=5π3x = \frac{\pi}{3} \quad \text{or} \quad x = 2\pi - \frac{\pi}{3} = \frac{5\pi}{3}x=3π​orx=2π−3π​=35π​

The double angle identities

The double angle identities replace a function of 2x2x2x by functions of xxx. For cos⁡2x\cos 2xcos2x, choose the one of its three forms that leaves only one function in the equation.

Worked example

Solve sin⁡2x=cos⁡x\sin 2x = \cos xsin2x=cosx for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

Use sin⁡2x=2sin⁡xcos⁡x\sin 2x = 2\sin x\cos xsin2x=2sinxcosx and collect everything on one side:

2sin⁡xcos⁡x−cos⁡x=0⇒cos⁡x(2sin⁡x−1)=02\sin x\cos x - \cos x = 0 \quad \Rightarrow \quad \cos x(2\sin x - 1) = 02sinxcosx−cosx=0⇒cosx(2sinx−1)=0

So cos⁡x=0\cos x = 0cosx=0 or sin⁡x=12\sin x = \frac{1}{2}sinx=21​.

cos⁡x=0\cos x = 0cosx=0: x=π2x = \frac{\pi}{2}x=2π​ or x=3π2x = \frac{3\pi}{2}x=23π​.

sin⁡x=12\sin x = \frac{1}{2}sinx=21​: x=π6x = \frac{\pi}{6}x=6π​ or x=5π6x = \frac{5\pi}{6}x=65π​.

x=π6, π2, 5π6, 3π2x = \frac{\pi}{6}, \ \frac{\pi}{2}, \ \frac{5\pi}{6}, \ \frac{3\pi}{2}x=6π​, 2π​, 65π​, 23π​

Tip

A quick check on the number of solutions: graph both sides of the original equation on a GDC (or sketch them). For sin⁡2x=cos⁡x\sin 2x = \cos xsin2x=cosx, the graphs cross four times in [0,2π][0, 2\pi][0,2π], matching the four answers.

Worked example

Solve cos⁡2x+3cos⁡x+2=0\cos 2x + 3\cos x + 2 = 0cos2x+3cosx+2=0 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

The equation already contains cos⁡x\cos xcosx, so use cos⁡2x=2cos⁡2x−1\cos 2x = 2\cos^2 x - 1cos2x=2cos2x−1:

2cos⁡2x−1+3cos⁡x+2=0⇒2cos⁡2x+3cos⁡x+1=0⇒(2cos⁡x+1)(cos⁡x+1)=02\cos^2 x - 1 + 3\cos x + 2 = 0 \quad \Rightarrow \quad 2\cos^2 x + 3\cos x + 1 = 0 \quad \Rightarrow \quad (2\cos x + 1)(\cos x + 1) = 02cos2x−1+3cosx+2=0⇒2cos2x+3cosx+1=0⇒(2cosx+1)(cosx+1)=0

cos⁡x=−12\cos x = -\frac{1}{2}cosx=−21​: x=2π3x = \frac{2\pi}{3}x=32π​ or 4π3\frac{4\pi}{3}34π​. cos⁡x=−1\cos x = -1cosx=−1: x=πx = \pix=π.

x=2π3, π, 4π3x = \frac{2\pi}{3}, \ \pi, \ \frac{4\pi}{3}x=32π​, π, 34π​

Equations that reduce to tan x = k

When an equation has the form asin⁡x=bcos⁡xa\sin x = b\cos xasinx=bcosx, dividing both sides by cos⁡x\cos xcosx gives tan⁡x=ba\tan x = \frac{b}{a}tanx=ab​. This division is safe here: if cos⁡x=0\cos x = 0cosx=0 then sin⁡x=±1\sin x = \pm 1sinx=±1, and the equation would read ±a=0\pm a = 0±a=0, which is false for a≠0a \neq 0a=0, so no solution is lost.

Worked example

Solve sin⁡x=3cos⁡x\sin x = \sqrt{3}\cos xsinx=3​cosx for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

No solution has cos⁡x=0\cos x = 0cosx=0 (that would need sin⁡x=0\sin x = 0sinx=0 as well, which is impossible since sin⁡2x+cos⁡2x=1\sin^2 x + \cos^2 x = 1sin2x+cos2x=1). Divide by cos⁡x\cos xcosx:

tan⁡x=3\tan x = \sqrt{3}tanx=3​

So x=π3x = \frac{\pi}{3}x=3π​, and adding the period π\piπ, x=4π3x = \frac{4\pi}{3}x=34π​.

x=π3orx=4π3x = \frac{\pi}{3} \quad \text{or} \quad x = \frac{4\pi}{3}x=3π​orx=34π​

Exam-style questions on trigonometric equations

Worked example

No calculator.

(a) Show that the equation 2cos⁡2x=3sin⁡x2\cos^2 x = 3\sin x2cos2x=3sinx can be written as 2sin⁡2x+3sin⁡x−2=02\sin^2 x + 3\sin x - 2 = 02sin2x+3sinx−2=0.

(b) Hence solve 2cos⁡2x=3sin⁡x2\cos^2 x = 3\sin x2cos2x=3sinx for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

(c) Hence solve 2cos⁡22x=3sin⁡2x2\cos^2 2x = 3\sin 2x2cos22x=3sin2x for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

Show the solution

(a) Using cos⁡2x=1−sin⁡2x\cos^2 x = 1 - \sin^2 xcos2x=1−sin2x:

2(1−sin⁡2x)=3sin⁡x⇒2−2sin⁡2x−3sin⁡x=0⇒2sin⁡2x+3sin⁡x−2=02(1 - \sin^2 x) = 3\sin x \quad \Rightarrow \quad 2 - 2\sin^2 x - 3\sin x = 0 \quad \Rightarrow \quad 2\sin^2 x + 3\sin x - 2 = 02(1−sin2x)=3sinx⇒2−2sin2x−3sinx=0⇒2sin2x+3sinx−2=0

Every line is shown, because the answer is given.

(b) Factorise: (2sin⁡x−1)(sin⁡x+2)=0(2\sin x - 1)(\sin x + 2) = 0(2sinx−1)(sinx+2)=0. Since −1≤sin⁡x≤1-1 \le \sin x \le 1−1≤sinx≤1, sin⁡x=−2\sin x = -2sinx=−2 has no solutions. From sin⁡x=12\sin x = \frac{1}{2}sinx=21​,

x=π6orx=5π6x = \frac{\pi}{6} \quad \text{or} \quad x = \frac{5\pi}{6}x=6π​orx=65π​

(c) "Hence" means use part (b). The equation is the same with 2x2x2x in place of xxx, so sin⁡2x=12\sin 2x = \frac{1}{2}sin2x=21​. For 0≤x≤2π0 \le x \le 2\pi0≤x≤2π, 0≤2x≤4π0 \le 2x \le 4\pi0≤2x≤4π:

2x=π6, 5π6, 13π6, 17π6⇒x=π12, 5π12, 13π12, 17π122x = \frac{\pi}{6}, \ \frac{5\pi}{6}, \ \frac{13\pi}{6}, \ \frac{17\pi}{6} \quad \Rightarrow \quad x = \frac{\pi}{12}, \ \frac{5\pi}{12}, \ \frac{13\pi}{12}, \ \frac{17\pi}{12}2x=6π​, 65π​, 613π​, 617π​⇒x=12π​, 125π​, 1213π​, 1217π​

Exam tip

"Hence" questions usually save a lot of work: part (c) needs only the result of part (b) and a change of interval. Starting again from the beginning gets the same answer slowly, and a question that says "hence" may not award marks for a method that ignores the previous part. When rejecting a value such as sin⁡x=−2\sin x = -2sinx=−2, write the reason (−1≤sin⁡x≤1-1 \le \sin x \le 1−1≤sinx≤1) so the examiner can see it is deliberate.

The second question needs a GDC for part (c), but parts (a), (b) and (d) can be done by hand.

Worked example

GDC allowed. The depth of water, ddd metres, at the entrance to a harbour ttt hours after midnight is modelled by

d(t)=1.8cos⁡(0.5t)+4.2,0≤t≤24d(t) = 1.8\cos(0.5t) + 4.2, \qquad 0 \le t \le 24d(t)=1.8cos(0.5t)+4.2,0≤t≤24

(a) Write down the greatest and least depths.

(b) Find the period of the model.

(c) A ship can enter the harbour only when the depth is more than 555 m. Find the values of ttt for which d(t)=5d(t) = 5d(t)=5.

(d) Hence find the total time during the day when the ship can enter the harbour.

Show the solution

(a) Greatest depth 4.2+1.8=64.2 + 1.8 = 64.2+1.8=6 m; least depth 4.2−1.8=2.44.2 - 1.8 = 2.44.2−1.8=2.4 m.

(b) Period =2π0.5=4π=12.6= \frac{2\pi}{0.5} = 4\pi = 12.6=0.52π​=4π=12.6 hours (3 s.f.).

(c) 1.8cos⁡(0.5t)+4.2=51.8\cos(0.5t) + 4.2 = 51.8cos(0.5t)+4.2=5 gives cos⁡(0.5t)=0.81.8=49\cos(0.5t) = \frac{0.8}{1.8} = \frac{4}{9}cos(0.5t)=1.80.8​=94​. Let u=0.5tu = 0.5tu=0.5t, so 0≤u≤120 \le u \le 120≤u≤12. The first solution is u=cos⁡−149=1.1102…u = \cos^{-1}\frac{4}{9} = 1.1102\ldotsu=cos−194​=1.1102…, and the others in the interval are 2π−1.1102…2\pi - 1.1102\ldots2π−1.1102…, 2π+1.1102…2\pi + 1.1102\ldots2π+1.1102… and 4π−1.1102…4\pi - 1.1102\ldots4π−1.1102… (the next one, 4π+1.1102…=13.74\pi + 1.1102\ldots = 13.74π+1.1102…=13.7, is beyond 121212). Doubling to return to ttt:

t=2.22,10.3,14.8,22.9(3 s.f.)t = 2.22, \quad 10.3, \quad 14.8, \quad 22.9 \quad (3 \text{ s.f.})t=2.22,10.3,14.8,22.9(3 s.f.)

The same values come from the intersections of y=d(t)y = d(t)y=d(t) and y=5y = 5y=5 on a GDC.

(d) The depth starts at its maximum (d(0)=6d(0) = 6d(0)=6), so it is above 555 m for 0≤t<2.22050 \le t < 2.22050≤t<2.2205, 10.346<t<14.78710.346 < t < 14.78710.346<t<14.787 and 22.912<t≤2422.912 < t \le 2422.912<t≤24. The total time is

2.2205+(14.787−10.346)+(24−22.912)=7.75 hours (3 s.f.)2.2205 + (14.787 - 10.346) + (24 - 22.912) = 7.75 \text{ hours (3 s.f.)}2.2205+(14.787−10.346)+(24−22.912)=7.75 hours (3 s.f.)

Exam tip

Read the interval in the question carefully before solving. Check whether it is in radians or degrees, whether the end points are included (≤\le≤) or not (<<<), and whether it starts below zero. A missing solution or an extra one outside the interval each cost a mark, so count the solutions against a sketch. Give exact answers in terms of π\piπ when the question has no calculator, and 3 significant figures (or 1 decimal place for degrees) otherwise.

A last type of question asks for the number of solutions rather than the solutions themselves.

Worked example

Let f(x)=2sin⁡x+1f(x) = 2\sin x + 1f(x)=2sinx+1 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π. Find the values of kkk for which the equation f(x)=kf(x) = kf(x)=k has exactly two solutions.

Show the solution

The graph of fff has amplitude 222 and principal axis y=1y = 1y=1. It starts at (0,1)(0, 1)(0,1), rises to a maximum (π2,3)(\frac{\pi}{2}, 3)(2π​,3), falls through (π,1)(\pi, 1)(π,1) to a minimum (3π2,−1)(\frac{3\pi}{2}, -1)(23π​,−1) and ends at (2π,1)(2\pi, 1)(2π,1).

0123456−2−101234xyy = 3y = 1y = −1(0, 1)(π/2, 3)(π, 1)(3π/2, −1)(2π, 1)
  • y = 2sin x + 1
Horizontal lines y = k meet the curve twice for −1 < k < 1 and 1 < k < 3, three times at k = 1 and once at k = 3 or k = −1.

A horizontal line y=ky = ky=k meets the graph:

  • once if k=3k = 3k=3 or k=−1k = -1k=−1 (only the maximum or the minimum);

  • three times if k=1k = 1k=1 (at x=0x = 0x=0, π\piπ and 2π2\pi2π);

  • twice for every other kkk between −1-1−1 and 333;

  • not at all if k>3k > 3k>3 or k<−1k < -1k<−1.

So there are exactly two solutions when −1<k<1-1 < k < 1−1<k<1 or 1<k<31 < k < 31<k<3.

Self-check

  • To do:

    I can explain why a trigonometric equation usually has infinitely many solutions, and find all of them in a given interval.

  • To do:

    I can find the second solution of sin⁡x=k\sin x = ksinx=k, cos⁡x=k\cos x = kcosx=k and tan⁡x=k\tan x = ktanx=k from the first, using the symmetry of the unit circle.

  • To do:

    I can solve trigonometric equations exactly using exact values, and approximately using a calculator.

  • To do:

    I can solve trigonometric equations graphically with a GDC.

  • To do:

    I can solve equations such as sin⁡2x=0.5\sin 2x = 0.5sin2x=0.5 or cos⁡(x−π3)=k\cos\left(x - \frac{\pi}{3}\right) = kcos(x−3π​)=k by changing the interval first.

  • To do:

    I can solve equations that are quadratic in sin⁡x\sin xsinx, cos⁡x\cos xcosx or tan⁡x\tan xtanx, and reject impossible values with a reason.

  • To do:

    I can use the Pythagorean and double angle identities to rewrite an equation in terms of one function.

  • To do:

    I can factorise instead of dividing by a function that could be zero.

Questions on 3.8

88 exam-style questions on this subtopic, written in the style of the IB papers. The first has its markscheme open. Counted on 20 October 2026

Question 1 · AA-000036 marks

Solve the equation 2cos⁡2x+sin⁡x=12\cos^2 x + \sin x = 12cos2x+sinx=1 for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π.

[6]6 marks

Markscheme

Using cos⁡2x=1−sin⁡2x\cos^2 x = 1 - \sin^2 xcos2x=1−sin2x: 2−2sin⁡2x+sin⁡x=12 - 2\sin^2 x + \sin x = 12−2sin2x+sinx=1 M1

2sin⁡2x−sin⁡x−1=02\sin^2 x - \sin x - 1 = 02sin2x−sinx−1=0 A1

(2sin⁡x+1)(sin⁡x−1)=0(2\sin x + 1)(\sin x - 1) = 0(2sinx+1)(sinx−1)=0, so sin⁡x=−12\sin x = -\tfrac{1}{2}sinx=−21​ or sin⁡x=1\sin x = 1sinx=1 M1A1

x=π2, 7π6, 11π6x = \frac{\pi}{2},\ \frac{7\pi}{6},\ \frac{11\pi}{6}x=2π​, 67π​, 611π​ A1A1

Award A1 for π2\frac{\pi}{2}2π​ and A1 for both other values.

Question 2 · AA-001408 marks

A bead moves anticlockwise around a circular wire. The wire is modelled by the unit circle, centre O, with distances measured in metres. At time ttt seconds, the position of the bead is

(cos⁡(0.8t),sin⁡(0.8t)),0≤t≤12.\left(\cos(0.8t), \sin(0.8t)\right), \quad 0 \le t \le 12.(cos(0.8t),sin(0.8t)),0≤t≤12.
  1. (a)

    Find the coordinates of the bead when t=2.5t = 2.5t=2.5.

    [2]2 marks

  2. (b)

    Find the value of ttt when the bead first returns to its starting position.

    [2]2 marks

  3. (c)

    Find the values of ttt for which the xxx-coordinate of the bead is −0.6-0.6−0.6 and its yyy-coordinate is positive.

    [4]4 marks

Answer it, then compare with the markscheme.Check this one with a free account
Question 3 · AA-0014616 marks

A seat on an observation wheel starts at its lowest point. The height of the seat above the ground, hhh metres, ttt minutes later is modelled by

h(t)=20−18cos⁡(πt12),0≤t≤24.h(t) = 20 - 18\cos\left(\frac{\pi t}{12}\right), \quad 0 \le t \le 24.h(t)=20−18cos(12πt​),0≤t≤24.
  1. (a)

    Find the exact height of the seat when t=9t = 9t=9.

    [2]2 marks

  2. (b)

    Write down the maximum height of the seat and the value of ttt at which it occurs.

    [2]2 marks

  3. (c)

    Find the values of ttt for which h(t)=29h(t) = 29h(t)=29.

    [4]4 marks

  4. (d)

    Hence, find the length of time during one revolution for which the seat is more than 29 m above the ground.

    [2]2 marks

  5. (e)

    Find the rate at which the height of the seat is changing when t=2t = 2t=2.

    [3]3 marks

  6. (f)

    Find the values of ttt at which the seat is descending at a rate of 3π4\dfrac{3\pi}{4}43π​ metres per minute.

    [3]3 marks

Answer it, then compare with the markscheme.Check this one with a free account

Try a quick-fire question

One of 32 short multiple-choice questions on 3.8. Pick an answer to see why it's right or wrong.

How many solutions does sin⁡2x=14\sin^2 x = \frac14sin2x=41​ have for 0≤x≤2π0 \le x \le 2\pi0≤x≤2π?

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Published for 3.8

Exam-style questions
88
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Quick-fire questions
32
Key terms
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Counted on 20 October 2026Open it in Augment

More of IB Maths AA

  • 3.7 Circular functionsBefore this in the Maths AA syllabus.
  • 3.9 Reciprocal and inverse trigonometric functionsAfter this in the Maths AA syllabus.
  • 3 Geometry and trigonometryThe whole topic, with all 18 of its subtopics.
  • IB Maths AAThe Maths AA syllabus, assessment and what Augment has for it.

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