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Solving Linear Trig Equations

A linear trig equation is one where the trig ratio appears only to the first power, like 3cos⁡x−1=03\cos x - 1 = 0. You solve it in two stages: first use ordinary algebra to isolate the trig ratio, then use the unit circle to find every angle in the interval that has that ratio. It’s the same process you used in degrees in Grade 11, but now the interval is 0≤x≤2π0 \le x \le 2\pi and all answers are in radians.

Solve for sin⁡x\sin x, cos⁡x\cos x or tan⁡x\tan x just as you would solve for a variable:

asin⁡x+b=c⇒sin⁡x=c−baa\sin x + b = c \quad\Rightarrow\quad \sin x = \frac{c - b}{a}

Sine and cosine are always between −1-1 and 11. If you get sin⁡x=1.25\sin x = 1.25 or cos⁡x=−2\cos x = -2, there is no solution. (Tangent can be any real number.)

Section titled “Step 2: Find the related (reference) angle”

The related angle θr\theta_r is the acute angle between the terminal arm and the xx-axis. Find it from the positive value of the ratio:

  • If it’s a special value (12\tfrac{1}{2}, 22\tfrac{\sqrt{2}}{2}, 32\tfrac{\sqrt{3}}{2}, 11, 3\sqrt{3}, 13\tfrac{1}{\sqrt{3}}), use the special angles for an exact answer.
  • Otherwise, use the inverse function on your calculator in radian mode: for example, θr=sin⁡−1(0.4)≈0.4115\theta_r = \sin^{-1}(0.4) \approx 0.4115.

The sign of the ratio tells you which quadrants the answers are in. Then:

Quadrant1234
Angleθr\theta_rπ−θr\pi - \theta_rπ+θr\pi + \theta_r2π−θr2\pi - \theta_r
Positive ratiosallsinetangentcosine

Most equations have two solutions in 0≤x≤2π0 \le x \le 2\pi. The exceptions are values on the axes: for example, sin⁡x=1\sin x = 1 only at x=π2x = \dfrac{\pi}{2}, and sin⁡x=0\sin x = 0 at x=0x = 0, π\pi and 2π2\pi (both endpoints count, since the interval includes them).

For an equation like cos⁡2x=12\cos 2x = \dfrac{1}{2} on 0≤x≤2π0 \le x \le 2\pi, the angle is 2x2x, and it runs over 0≤2x≤4π0 \le 2x \le 4\pi: that’s two full turns. So there are twice as many solutions.

  1. Let u=kxu = kx and find the interval for uu: 0≤u≤2kπ0 \le u \le 2k\pi.
  2. Solve for uu in the first turn, then add 2π2\pi (and 4π4\pi, …) to get the solutions in the later turns.
  3. Divide every value by kk to get xx.

The graph of y=sin⁡kxy = \sin kx or y=cos⁡kxy = \cos kx has period 2πk\dfrac{2\pi}{k}, so it completes kk cycles between 00 and 2π2\pi. That’s where the extra solutions come from.

Each solution of f(x)=cf(x) = c is the xx-coordinate of an intersection of y=f(x)y = f(x) and the horizontal line y=cy = c. Graphing both (for example, in Desmos with radians) is a quick way to check that you have the right number of solutions in roughly the right places.

Solve 2sin⁡x−3=02\sin x - \sqrt{3} = 0 for 0≤x≤2π0 \le x \le 2\pi.

Solution. Isolate sin⁡x\sin x:

2sin⁡x=3⇒sin⁡x=322\sin x = \sqrt{3} \quad\Rightarrow\quad \sin x = \frac{\sqrt{3}}{2}

The related angle is π3\dfrac{\pi}{3}. Sine is positive in quadrants 1 and 2:

x=π3orx=π−π3=2π3x = \frac{\pi}{3} \qquad\text{or}\qquad x = \pi - \frac{\pi}{3} = \frac{2\pi}{3}

Check: 2sin⁡2π3−3=2(32)−3=02\sin\dfrac{2\pi}{3} - \sqrt{3} = 2\left(\dfrac{\sqrt{3}}{2}\right) - \sqrt{3} = 0. ✓

Solve 4cos⁡x+3=14\cos x + 3 = 1 for 0≤x≤2π0 \le x \le 2\pi.

Solution.

4cos⁡x=−2⇒cos⁡x=−124\cos x = -2 \quad\Rightarrow\quad \cos x = -\frac{1}{2}

The related angle comes from the positive value 12\dfrac{1}{2}: θr=π3\theta_r = \dfrac{\pi}{3}. Cosine is negative in quadrants 2 and 3:

x=π−π3=2π3orx=π+π3=4π3x = \pi - \frac{\pi}{3} = \frac{2\pi}{3} \qquad\text{or}\qquad x = \pi + \frac{\pi}{3} = \frac{4\pi}{3}

Check: 4cos⁡4π3+3=4(−12)+3=14\cos\dfrac{4\pi}{3} + 3 = 4\left(-\dfrac{1}{2}\right) + 3 = 1. ✓

Solve 5sin⁡x+2=05\sin x + 2 = 0 for 0≤x≤2π0 \le x \le 2\pi. Round to three decimal places.

Solution.

5sin⁡x=−2⇒sin⁡x=−0.45\sin x = -2 \quad\Rightarrow\quad \sin x = -0.4

This isn’t a special value, so use the calculator (radian mode) with the positive value to get the related angle:

θr=sin⁡−1(0.4)≈0.4115\theta_r = \sin^{-1}(0.4) \approx 0.4115

Sine is negative in quadrants 3 and 4:

x=π+θr≈3.1416+0.4115≈3.553x=2π−θr≈6.2832−0.4115≈5.872\begin{aligned} x &= \pi + \theta_r \approx 3.1416 + 0.4115 \approx 3.553 \\ x &= 2\pi - \theta_r \approx 6.2832 - 0.4115 \approx 5.872 \end{aligned}
The graph of y = sin x from 0 to 2 pi and the horizontal line y = -0.4. They intersect twice, at x approximately 3.553 and 5.872, both between pi and 2 pi. −1 1 π/2 π 3π/2 2π 3.553 5.872 y = sin x y = −0.4
The line y=−0.4y = -0.4 meets y=sin⁡xy = \sin x twice in 0≤x≤2π0 \le x \le 2\pi.

Why not just press sin⁡−1(−0.4)\sin^{-1}(-0.4)? The calculator gives about −0.4115-0.4115, which is outside the interval and is only one of the angles. Working from the related angle finds both.

Solve 2cos⁡2x=12\cos 2x = 1 for 0≤x≤2π0 \le x \le 2\pi.

Solution. Isolate the cosine: cos⁡2x=12\cos 2x = \dfrac{1}{2}.

Let u=2xu = 2x. Since 0≤x≤2π0 \le x \le 2\pi, we need 0≤u≤4π0 \le u \le 4\pi.

In the first turn, cos⁡u=12\cos u = \dfrac{1}{2} at u=π3u = \dfrac{\pi}{3} (quadrant 1) and u=2π−π3=5π3u = 2\pi - \dfrac{\pi}{3} = \dfrac{5\pi}{3} (quadrant 4). Add 2π2\pi for the second turn:

u=π3, 5π3, 7π3, 11π3u = \frac{\pi}{3},\ \frac{5\pi}{3},\ \frac{7\pi}{3},\ \frac{11\pi}{3}

Divide by 22 to get xx:

x=π6, 5π6, 7π6, 11π6x = \frac{\pi}{6},\ \frac{5\pi}{6},\ \frac{7\pi}{6},\ \frac{11\pi}{6}
The graph of y = cos 2x from 0 to 2 pi, which completes two full cycles, and the line y = 1/2. They intersect four times, at x = pi/6, 5 pi/6, 7 pi/6 and 11 pi/6. −1 1 π/2 π 3π/2 2π π/6 5π/6 7π/6 11π/6 y = 1/2 y = cos 2x
y=cos⁡2xy = \cos 2x has period π\pi, so it reaches 12\dfrac{1}{2} four times in 0≤x≤2π0 \le x \le 2\pi.

Check: 2cos⁡(2⋅7π6)=2cos⁡7π3=2cos⁡π3=12\cos\left(2\cdot\dfrac{7\pi}{6}\right) = 2\cos\dfrac{7\pi}{3} = 2\cos\dfrac{\pi}{3} = 1. ✓

Calculator in degree mode. sin⁡−1(0.4)\sin^{-1}(0.4) is about 23.5823.58 in degrees but 0.41150.4115 in radians. Every answer on this page is in radians.

Taking the inverse of a negative value and stopping. sin⁡−1(−0.4)≈−0.4115\sin^{-1}(-0.4) \approx -0.4115 isn’t in the interval, and it’s only one solution anyway. Find the related angle from the positive value, then use CAST.

Finding only one solution. Most values of sine or cosine occur twice in one turn. Always ask “which two quadrants?”

Dividing by k too early. In cos⁡2x=12\cos 2x = \dfrac{1}{2}, finding x=π6x = \dfrac{\pi}{6} and 5π6\dfrac{5\pi}{6} and stopping misses half the answers. Extend the interval for u=2xu = 2x to 0≤u≤4π0 \le u \le 4\pi first, find all values of uu, then divide.

Missing the endpoints. For 0≤x≤2π0 \le x \le 2\pi, both 00 and 2π2\pi are included. sin⁡x=0\sin x = 0 has three solutions: 00, π\pi and 2π2\pi.

Not noticing there’s no solution. If you get a value of sin⁡x\sin x or cos⁡x\cos x that is less than −1-1 or greater than 11, stop: there is no solution. Your calculator will show an error, and that’s the reason.

1. (Warm-up) Solve each equation for 0≤x≤2π0 \le x \le 2\pi.

  • (a) sin⁡x=−22\sin x = -\dfrac{\sqrt{2}}{2}
  • (b) cos⁡x=−1\cos x = -1
  • (c) sin⁡x=0\sin x = 0
Solution

(a) Related angle π4\dfrac{\pi}{4}. Sine is negative in quadrants 3 and 4: x=π+π4=5π4x = \pi + \dfrac{\pi}{4} = \dfrac{5\pi}{4} or x=2π−π4=7π4x = 2\pi - \dfrac{\pi}{4} = \dfrac{7\pi}{4}.

(b) The point (−1,0)(-1, 0) on the unit circle: x=πx = \pi.

(c) The points (1,0)(1, 0) and (−1,0)(-1, 0): x=0x = 0, π\pi, 2π2\pi.

2. (Warm-up) Solve 2cos⁡x−1=02\cos x - 1 = 0 for 0≤x≤2π0 \le x \le 2\pi.

Solution

cos⁡x=12\cos x = \dfrac{1}{2}. Related angle π3\dfrac{\pi}{3}; cosine is positive in quadrants 1 and 4:

x=π3orx=2π−π3=5π3x = \frac{\pi}{3} \qquad\text{or}\qquad x = 2\pi - \frac{\pi}{3} = \frac{5\pi}{3}

3. (Core) Solve 3tan⁡x+1=0\sqrt{3}\tan x + 1 = 0 for 0≤x≤2π0 \le x \le 2\pi.

Solution

tan⁡x=−13\tan x = -\dfrac{1}{\sqrt{3}}. The related angle is π6\dfrac{\pi}{6} (since tan⁡π6=13\tan\dfrac{\pi}{6} = \dfrac{1}{\sqrt{3}}). Tangent is negative in quadrants 2 and 4:

x=π−π6=5π6orx=2π−π6=11π6x = \pi - \frac{\pi}{6} = \frac{5\pi}{6} \qquad\text{or}\qquad x = 2\pi - \frac{\pi}{6} = \frac{11\pi}{6}

Check: tan⁡11π6=−13\tan\dfrac{11\pi}{6} = -\dfrac{1}{\sqrt{3}}, so 3(−13)+1=0\sqrt{3}\left(-\dfrac{1}{\sqrt{3}}\right) + 1 = 0. ✓

4. (Core) Solve 3cos⁡x−1=03\cos x - 1 = 0 for 0≤x≤2π0 \le x \le 2\pi. Round to three decimal places.

Solution

cos⁡x=13\cos x = \dfrac{1}{3}. In radian mode, θr=cos⁡−1(13)≈1.2310\theta_r = \cos^{-1}\left(\dfrac{1}{3}\right) \approx 1.2310. Cosine is positive in quadrants 1 and 4:

x≈1.231orx≈2π−1.2310≈5.052x \approx 1.231 \qquad\text{or}\qquad x \approx 2\pi - 1.2310 \approx 5.052

5. (Core) Explain why 4sin⁡x+7=24\sin x + 7 = 2 has no solution.

Solution

Isolating gives 4sin⁡x=−54\sin x = -5, so sin⁡x=−54=−1.25\sin x = -\dfrac{5}{4} = -1.25. But sin⁡x\sin x is always between −1-1 and 11, so no angle has a sine of −1.25-1.25. (On a graph, the line y=−1.25y = -1.25 never meets y=sin⁡xy = \sin x.)

6. (Core) Solve 2sin⁡2x+3=02\sin 2x + \sqrt{3} = 0 for 0≤x≤2π0 \le x \le 2\pi.

Solution

sin⁡2x=−32\sin 2x = -\dfrac{\sqrt{3}}{2}. Let u=2xu = 2x, with 0≤u≤4π0 \le u \le 4\pi.

Related angle π3\dfrac{\pi}{3}. Sine is negative in quadrants 3 and 4, so in the first turn u=π+π3=4π3u = \pi + \dfrac{\pi}{3} = \dfrac{4\pi}{3} and u=2π−π3=5π3u = 2\pi - \dfrac{\pi}{3} = \dfrac{5\pi}{3}. Adding 2π2\pi: u=10π3u = \dfrac{10\pi}{3} and 11π3\dfrac{11\pi}{3}.

Divide by 22:

x=2π3, 5π6, 5π3, 11π6x = \frac{2\pi}{3},\ \frac{5\pi}{6},\ \frac{5\pi}{3},\ \frac{11\pi}{6}

7. (Core) A Ferris wheel at the CNE turns once every 6060 s. A rider’s height above the ground, in metres, tt seconds after boarding is

h(t)=−9cos⁡(πt30)+11h(t) = -9\cos\left(\frac{\pi t}{30}\right) + 11

During the first turn (0≤t≤600 \le t \le 60), when is the rider 15.515.5 m above the ground?

Solution−9cos⁡(πt30)+11=15.5⇒−9cos⁡(πt30)=4.5⇒cos⁡(πt30)=−12-9\cos\left(\frac{\pi t}{30}\right) + 11 = 15.5 \quad\Rightarrow\quad -9\cos\left(\frac{\pi t}{30}\right) = 4.5 \quad\Rightarrow\quad \cos\left(\frac{\pi t}{30}\right) = -\frac{1}{2}

Let u=πt30u = \dfrac{\pi t}{30}. For 0≤t≤600 \le t \le 60, 0≤u≤2π0 \le u \le 2\pi. Cosine is negative in quadrants 2 and 3, with related angle π3\dfrac{\pi}{3}:

u=2π3oru=4π3u = \frac{2\pi}{3} \quad\text{or}\quad u = \frac{4\pi}{3}

Solve πt30=u\dfrac{\pi t}{30} = u for tt, so t=30uπt = \dfrac{30u}{\pi}:

t=30π⋅2π3=20ort=30π⋅4π3=40t = \frac{30}{\pi}\cdot\frac{2\pi}{3} = 20 \qquad\text{or}\qquad t = \frac{30}{\pi}\cdot\frac{4\pi}{3} = 40

The rider is 15.515.5 m up at 2020 s (on the way up) and 4040 s (on the way down).

Check: h(20)=−9cos⁡2π3+11=−9(−12)+11=15.5h(20) = -9\cos\dfrac{2\pi}{3} + 11 = -9\left(-\dfrac{1}{2}\right) + 11 = 15.5. ✓

8. (Challenge) Solve sin⁡3x=12\sin 3x = \dfrac{1}{2} for 0≤x≤2π0 \le x \le 2\pi. How many solutions are there, and why?

Solution

Let u=3xu = 3x, with 0≤u≤6π0 \le u \le 6\pi (three full turns).

In the first turn, sin⁡u=12\sin u = \dfrac{1}{2} at u=π6u = \dfrac{\pi}{6} and u=5π6u = \dfrac{5\pi}{6}. Add 2π=12π62\pi = \dfrac{12\pi}{6} and 4π=24π64\pi = \dfrac{24\pi}{6}:

u=π6, 5π6, 13π6, 17π6, 25π6, 29π6u = \frac{\pi}{6},\ \frac{5\pi}{6},\ \frac{13\pi}{6},\ \frac{17\pi}{6},\ \frac{25\pi}{6},\ \frac{29\pi}{6}

Divide by 33:

x=π18, 5π18, 13π18, 17π18, 25π18, 29π18x = \frac{\pi}{18},\ \frac{5\pi}{18},\ \frac{13\pi}{18},\ \frac{17\pi}{18},\ \frac{25\pi}{18},\ \frac{29\pi}{18}

There are 66 solutions: y=sin⁡3xy = \sin 3x completes 33 cycles in 0≤x≤2π0 \le x \le 2\pi, and it reaches 12\dfrac{1}{2} twice in each cycle.

9. (Challenge) Solve 2cos⁡(x−π6)+2=02\cos\left(x - \dfrac{\pi}{6}\right) + \sqrt{2} = 0 for 0≤x≤2π0 \le x \le 2\pi.

Solution

cos⁡(x−π6)=−22\cos\left(x - \dfrac{\pi}{6}\right) = -\dfrac{\sqrt{2}}{2}. Let u=x−π6u = x - \dfrac{\pi}{6}. Since 0≤x≤2π0 \le x \le 2\pi, the interval for uu is −π6≤u≤11π6-\dfrac{\pi}{6} \le u \le \dfrac{11\pi}{6}.

Related angle π4\dfrac{\pi}{4}; cosine is negative in quadrants 2 and 3:

u=π−π4=3π4oru=π+π4=5π4u = \pi - \frac{\pi}{4} = \frac{3\pi}{4} \qquad\text{or}\qquad u = \pi + \frac{\pi}{4} = \frac{5\pi}{4}

Both are in the interval for uu (and no others are: adding or subtracting 2π2\pi takes them outside it). Add π6\dfrac{\pi}{6} to get xx:

x=3π4+π6=9π+2π12=11π12orx=5π4+π6=15π+2π12=17π12x = \frac{3\pi}{4} + \frac{\pi}{6} = \frac{9\pi + 2\pi}{12} = \frac{11\pi}{12} \qquad\text{or}\qquad x = \frac{5\pi}{4} + \frac{\pi}{6} = \frac{15\pi + 2\pi}{12} = \frac{17\pi}{12}