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Topic 3.10A

Trigonometric Equations and Inequalities

In 3.9 an inverse trig function gave us one angle. But a trig equation usually has more solutions than that: two in every cycle, and infinitely many overall. This note (Part A) shows how to find all of them. Part B uses the same ideas to solve inequalities.

9 MIN READ5 IDEAS33 PROBLEMS10 flashcards

01

Two Solutions per Cycle

Every trig equation is solved in the same order: first isolate the trig function, then find the angles.

Worked example

Example 1. Solve 3−2sin⁡θ=43 - 2 \sin \theta = 4 for 0≤θ<2π0 \le \theta < 2\pi. Then give all solutions.

  1. 01

    Isolate sin⁡θ\sin \theta, as you would isolate xx: −2sin⁡θ=1-2 \sin \theta = 1, so sin⁡θ=−1/2\sin \theta = -1/2.

  2. 02

    Find the reference angle: sin⁡(π/6)=1/2\sin (\pi /6) = 1/2, so the reference angle is π/6\pi /6.

  3. 03

    Sine is the y-coordinate, and it is negative in Quadrants III and IV. The angles with reference angle π/6\pi /6 there are π+π/6=7π/6\pi + \pi /6 = 7\pi /6 and 2π−π/6=11π/62\pi - \pi /6 = 11\pi /6.

  4. 04

    Both lie in [0,2π)[0, 2\pi ), so the solutions are θ=7π/6\theta = 7\pi /6 and θ=11π/6\theta = 11\pi /6.

    2026-09-19T23:12:40.421147 image/svg+xml Matplotlib v3.10.8, https://matplotlib.org/

    The horizontal line y=−1/2y = -1/2 meets the unit circle, and one cycle of the sine graph, exactly twice.

    Because sine repeats every 2π2\pi, adding any whole number of full turns gives another solution. The complete solution set is:

    θ=7π6+2πkorθ=11π6+2πk\theta=\frac{7\pi}{6}+2\pi k\quad\mathrm{or}\quad\theta=\frac{11\pi}{6}+2\pi k

    where kk is any integer. Graphically, the line y=−1/2y = -1/2 crosses the sine graph twice in every cycle, and each crossing repeats every 2π2\pi.

COMMON MISTAKE

"sin⁡θ=−1/2\sin \theta = -1/2, so θ=arcsin⁡(−1/2)=−π/6\theta = \arcsin (-1/2) = -\pi /6. Done."

arcsin⁡\arcsin returns only ONE angle, the one in [−π/2,π/2][-\pi /2, \pi /2] (3.9). −π/6-\pi /6 is a correct solution, but it is not in [0,2π)[0, 2\pi ), and it is only one of the two solutions per cycle.

From −π/6-\pi /6 you can reach both answers: add 2π2\pi to get 11π/611\pi /6, and use symmetry (π−(−π/6))(\pi - (-\pi /6)) to get 7π/67\pi /6. Either way, always look for the second angle.

Quick check

Solve 2cos⁡θ=12\cos\theta = 1 for 0≤θ<2π0 \le \theta < 2\pi.

02

Using Inverse Trig Functions

When the value is not a special one, use a calculator in RADIAN mode. The inverse function gives the first angle; symmetry gives the second.

CONCEPT

Finding both angles in one cycle

sin⁡θ=k\sin \theta = k: θ=arcsin⁡k\theta = \arcsin k or θ=π−arcsin⁡k\theta = \pi - \arcsin k (the two angles are symmetric about π/2\pi /2).

cos⁡θ=k\cos \theta = k: θ=arccos⁡k\theta = \arccos k or θ=−arccos⁡k\theta = -\arccos k (symmetric about the x-axis); add 2π2\pi to bring −arccos⁡k-\arccos k into [0,2π)[0, 2\pi ).

tan⁡θ=k\tan \theta = k: θ=arctan⁡k\theta = \arctan k, and then every π\pi after it (tangent has period π\pi, 3.8).

Worked example

Example 2. Solve 5cos⁡θ−1=25 \cos \theta - 1 = 2 for 0≤θ<2π0 \le \theta < 2\pi. Round to three decimal places.

  1. 01

    Isolate: 5cos⁡θ=35 \cos \theta = 3, so cos⁡θ=3/5=0.6\cos \theta = 3/5 = 0.6.

  2. 02

    First angle: θ=arccos⁡(0.6)≈0.927\theta = \arccos (0.6) \approx 0.927.

  3. 03

    Cosine is the x-coordinate. The other point on the unit circle with x=0.6x = 0.6 is the mirror image below the x-axis, at −0.927. In [0,2π)[0, 2\pi ) that is 2π−0.927≈5.3562\pi - 0.927 \approx 5.356.

    2026-09-19T23:12:40.685846 image/svg+xml Matplotlib v3.10.8, https://matplotlib.org/

    The vertical line x=0.6x = 0.6 meets the unit circle at two angles, symmetric about the x-axis.

COMMON MISTAKE

"The second solution of cos⁡θ=0.6\cos \theta = 0.6 is π−0.927≈2.214\pi - 0.927 \approx 2.214."

π−θ\pi - \theta is the partner angle for SINE, because it keeps the y-coordinate. It flips the x-coordinate: cos⁡(2.214)≈−0.6\cos (2.214) \approx -0.6, not 0.6.

Cosine keeps the x-coordinate, so its partner is the reflection over the x-axis: −θ-\theta, or 2π−θ2\pi - \theta.

Worked example

Example 3. Solve 2tan⁡θ+5=02 \tan \theta + 5 = 0 for 0≤θ<2π0 \le \theta < 2\pi.

  1. 01

    Isolate: tan⁡θ=−2.5\tan \theta = -2.5. Then arctan⁡(−2.5)≈−1.190\arctan (-2.5) \approx -1.190, which is not in [0,2π)[0, 2\pi ).

  2. 02

    Tangent repeats every π\pi, so add π\pi until the angles land in the interval: −1.190+π≈1.951-1.190 + \pi \approx 1.951 and −1.190+2π≈5.093-1.190 + 2\pi \approx 5.093.

  3. 03

    Check: tan⁡θ\tan \theta is negative in Quadrants II and IV, and 1.951 (between π/2\pi /2 and π\pi) and 5.093 (between 3π/23\pi /2 and 2π2\pi) are in exactly those quadrants ✓.

03

Equations That Factor

Sometimes the trig function appears squared, or more than once. Treat the trig function like a single variable and factor, just like a quadratic from Unit 1.

Worked example

Example 4. Solve 2cos⁡2θ+cos⁡θ−1=02 \cos ^{2} \theta + \cos \theta - 1 = 0 for 0≤θ<2π0 \le \theta < 2\pi.

  1. 01

    Think of cos⁡θ\cos \theta as cc: 2c2+c−1=(2c−1)(c+1)2c^{2} + c - 1 = (2c - 1)(c + 1). So (2cos⁡θ−1)(cos⁡θ+1)=0(2 \cos \theta - 1)(\cos \theta + 1) = 0.

  2. 02

    Zero product property: cos⁡θ=1/2\cos \theta = 1/2 or cos⁡θ=−1\cos \theta = -1.

  3. 03

    cos⁡θ=1/2\cos \theta = 1/2 gives θ=π/3\theta = \pi /3 and 5π/35\pi /3. cos⁡θ=−1\cos \theta = -1 gives only θ=π\theta = \pi (the one point (−1,0)(-1, 0)).

  4. 04

    Solutions: θ=π/3\theta = \pi /3, π\pi, and 5π/35\pi /3.

COMMON MISTAKE

Solving 3sin⁡θcos⁡θ=sin⁡θ3 \sin \theta \cos \theta = \sin \theta by dividing both sides by sin⁡θ\sin \theta to get cos⁡θ=1/3\cos \theta = 1/3.

Dividing by sin⁡θ\sin \theta is only allowed when sin⁡θ≠0\sin \theta \ne 0, so this throws away every solution with sin⁡θ=0\sin \theta = 0.

Instead, move everything to one side and factor: sin⁡θ\sin \theta (3cos⁡θ−1)=0(3 \cos \theta - 1) = 0. Now sin⁡θ=0\sin \theta = 0 gives θ=0\theta = 0 and π\pi, and cos⁡θ=1/3\cos \theta = 1/3 gives θ≈1.231\theta \approx 1.231 and 5.052. That is four solutions, not two.

04

When the Period Changes

If the input is bθb\theta instead of θ\theta, the graph completes more cycles in [0,2π)[0, 2\pi ), so there are more solutions. Remember from 3.6A: y=sin⁡2θy = \sin 2\theta has period π\pi, so it fits two full cycles into [0,2π)[0, 2\pi ).

Worked example

Example 5. Solve 2sin⁡2 \sin 2θ=32\theta = \sqrt{3} for 0≤θ<2π0 \le \theta < 2\pi.

  1. 01

    Isolate: sin⁡\sin 2θ=3/22\theta = \sqrt{3}/2. Let u=2θu = 2\theta. Because 0≤θ<2π0 \le \theta < 2\pi, the new variable runs over 0≤u<4π0 \le u < 4\pi: two full turns.

  2. 02

    In the first turn, sin⁡u=3/2\sin u = \sqrt{3}/2 at u=π/3u = \pi /3 and 2π/32\pi /3. Add 2π2\pi for the second turn: u=7π/3u = 7\pi /3 and 8π/38\pi /3.

  3. 03

    Divide every uu by 2: θ=π/6\theta = \pi /6, π/3\pi /3, 7π/67\pi /6, and 4π/34\pi /3.

    2026-09-19T23:12:40.881708 image/svg+xml Matplotlib v3.10.8, https://matplotlib.org/

    sin⁡θ\sin \theta reaches 3/2\sqrt{3}/2 twice in [0,2π)[0, 2\pi ), but sin⁡2θ\sin 2\theta does it four times.

COMMON MISTAKE

"sin⁡\sin 2θ=3/22\theta = \sqrt{3}/2, so 2θ=π/32\theta = \pi /3 or 2π/32\pi /3, and θ=π/6\theta = \pi /6 or π/3\pi /3."

That solves only the first of the two cycles. The interval for u=2θu = 2\theta is twice as long as the interval for θ\theta, so you must collect u-values from [0,4π)[0, 4\pi ) BEFORE dividing by 2. Check with the graph: the curve y=sin⁡2θy = \sin 2\theta clearly meets the line four times.

REAL-LIFE EXAMPLE

Every time the pedal is at 40 cm

Remember from 3.9: h(t)=−17cos⁡(5πt/3)+28=40h(t) = -17 \cos (5\pi t/3) + 28 = 40 led to cos⁡(5πt/3)=−12/17\cos (5\pi t/3) = -12/17, and arccos⁡\arccos gave the first time, t≈0.45t \approx 0.45 s. Now we can find them all.

Let u=5πt/3u = 5\pi t/3. cos⁡u=−12/17\cos u = -12/17 gives u=arccos⁡(−12/17)≈2.354u = \arccos (-12/17) \approx 2.354 and u=2π−2.354≈3.929u = 2\pi - 2.354 \approx 3.929. Then t=3u/(5π)t = 3u/(5\pi ): t≈0.45t \approx 0.45 s (on the way up) and t≈0.75t \approx 0.75 s (on the way down).

One rotation takes 1.2 s, so all the times are t≈0.45+1.2kt \approx 0.45 + 1.2k and t≈0.75+1.2kt \approx 0.75 + 1.2k for k=0k = 0, 1, 2, …

Check with symmetry: the top of the rotation is at t=0.6t = 0.6, and 0.45 and 0.75 are both 0.15 s away from it ✓.

2026-09-19T23:12:41.159154 image/svg+xml Matplotlib v3.10.8, https://matplotlib.org/

The pedal passes 40 cm twice per rotation: once rising, once falling.

Quick check

How many solutions does sin⁡(2θ)=0\sin(2\theta) = 0 have on 0≤θ<2π0 \le \theta < 2\pi?

Common slips

  • "sin⁡θ=−1/2\sin \theta = -1/2, so θ=arcsin⁡(−1/2)=−π/6\theta = \arcsin (-1/2) = -\pi /6. Done."

    arcsin⁡\arcsin returns only one angle, the one in [−π/2,π/2][-\pi /2, \pi /2] (3.9). −π/6-\pi /6 is a correct solution, but it is not in [0,2π)[0, 2\pi ), and it is only one of the two solutions per cycle.

    From −π/6-\pi /6 you can reach both answers: add 2π2\pi to get 11π/611\pi /6, and use symmetry (π−(−π/6))(\pi - (-\pi /6)) to get 7π/67\pi /6. Either way, always look for the second angle.

  • "The second solution of cos⁡θ=0.6\cos \theta = 0.6 is π−0.927≈2.214\pi - 0.927 \approx 2.214."

    π−θ\pi - \theta is the partner angle for sine, because it keeps the y-coordinate. It flips the x-coordinate: cos⁡(2.214)≈−0.6\cos (2.214) \approx -0.6, not 0.6.

    Cosine keeps the x-coordinate, so its partner is the reflection over the x-axis: −θ-\theta, or 2π−θ2\pi - \theta.

  • Solving 3sin⁡θcos⁡θ=sin⁡θ3 \sin \theta \cos \theta = \sin \theta by dividing both sides by sin⁡θ\sin \theta to get cos⁡θ=1/3\cos \theta = 1/3.

    Dividing by sin⁡θ\sin \theta is only allowed when sin⁡θ≠0\sin \theta \ne 0, so this throws away every solution with sin⁡θ=0\sin \theta = 0.

    Instead, move everything to one side and factor: sin⁡θ\sin \theta (3cos⁡θ−1)=0(3 \cos \theta - 1) = 0. Now sin⁡θ=0\sin \theta = 0 gives θ=0\theta = 0 and π\pi, and cos⁡θ=1/3\cos \theta = 1/3 gives θ≈1.231\theta \approx 1.231 and 5.052. That is four solutions, not two.

  • "sin⁡\sin 2θ=3/22\theta = \sqrt{3}/2, so 2θ=π/32\theta = \pi /3 or 2π/32\pi /3, and θ=π/6\theta = \pi /6 or π/3\pi /3."

    That solves only the first of the two cycles. The interval for u=2θu = 2\theta is twice as long as the interval for θ\theta, so you must collect u-values from [0,4π)[0, 4\pi ) Before dividing by 2. Check with the graph: the curve y=sin⁡2θy = \sin 2\theta clearly meets the line four times.

Lock it in

Try the flashcards

10 cards · Inverse trig and equations

Start

Recap card

6 lines to re-read the night before.

  1. 01

    Isolate the trig function first, then find the angles.

  2. 02

    Most equations have two solutions per cycle. For sine the partner of θ\theta is π−θ\pi - \theta; for cosine it is −θ-\theta (or 2π−θ2\pi - \theta). Tangent repeats every π\pi.

  3. 03

    An inverse trig function gives only one angle. Use symmetry and periodicity to find the rest.

  4. 04

    All solutions: add 2πk2\pi k (or πk\pi k for tangent), where kk is any integer.

  5. 05

    Factor instead of dividing by a trig function, so no solutions are lost.

  6. 06

    With input bθb\theta, collect solutions over the stretched interval first, then divide by bb.

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