Skip to content

Solving Trigonometric Equations

By the end of this section, you will be able to:

  • Solve linear trigonometric equations in sine and cosine
  • Solve equations involving a single trigonometric function
  • Solve trigonometric equations using a calculator
  • Solve trigonometric equations that are quadratic in form
  • Solve trigonometric equations using fundamental identities
  • Solve trigonometric equations with multiple angles
  • Solve right triangle problems

Thales of Miletus (circa 625–547 BC) is known as the founder of geometry. The legend is that he calculated the height of the Great Pyramid of Giza in Egypt using the theory of similar triangles, which he developed by measuring the shadow of his staff. Based on proportions, this theory has applications in a number of areas, including fractal geometry, engineering, and architecture. Often, the angle of elevation and the angle of depression are found using similar triangles.

In earlier sections of this chapter, we looked at trigonometric identities. Identities are true for all values in the domain of the variable. In this section, we begin our study of trigonometric equations to study real-world scenarios such as finding the dimensions of the pyramids.

Solving Linear Trigonometric Equations in Sine and Cosine

Trigonometric equations are, as the name implies, equations that involve trigonometric functions. Similar in many ways to solving polynomial equations or rational equations, only specific values of the variable will be solutions, if there are solutions at all. Often we will solve a trigonometric equation over a specified interval. However, just as often, we will be asked to find all possible solutions, and as trigonometric functions are periodic, solutions are repeated within each period. In other words, trigonometric equations may have an infinite number of solutions. Additionally, like rational equations, the domain of the function must be considered before we assume that any solution is valid. The period of both the sine function and the cosine function is 2π2\pi. In other words, every 2π2\pi units, the yy-values repeat. If we need to find all possible solutions, then we must add 2πk2\pi k, where kk is an integer, to the initial solution. Recall the rule that gives the format for stating all possible solutions for a function where the period is 2π2\pi:

sinθ=sin(θ±2kπ)\sin\theta=\sin(\theta\pm2k\pi)

There are similar rules for indicating all possible solutions for the other trigonometric functions. Solving trigonometric equations requires the same techniques as solving algebraic equations. We read the equation from left to right, horizontally, like a sentence. We look for known patterns, factor, find common denominators, and substitute certain expressions with a variable to make solving a more straightforward process. However, with trigonometric equations, we also have the advantage of using the identities we developed in the previous sections.

Example. Find all possible exact solutions for the equation cosθ=12\cos\theta=\tfrac12.

Solution. From the unit circle, we know that

cosθ=12θ=π3,5π3 \begin{array}{lrcl} & \cos\theta &=& \tfrac12 \\[4pt] & \theta &=& \tfrac{\pi}{3},\tfrac{5\pi}{3} \end{array}

These are the solutions in the interval [0,2π][0,2\pi]. All possible solutions are given by

π3±2kπ and 5π3±2kπ\tfrac{\pi}{3}\pm2k\pi\ \text{and}\ \tfrac{5\pi}{3}\pm2k\pi

where kk is an integer.

Example. Find all possible exact solutions for the equation sint=12\sin t=\tfrac12.

Solution. Solving for all possible values of tt means that solutions include angles beyond the period of 2π2\pi. From the unit circle, we can see that the solutions are π6\tfrac{\pi}{6} and 5π6\tfrac{5\pi}{6}. But the problem is asking for all possible values that solve the equation. Therefore, the answer is

π6±2πk and 5π6±2πk\tfrac{\pi}{6}\pm2\pi k\ \text{and}\ \tfrac{5\pi}{6}\pm2\pi k

where kk is an integer.

How to: given a trigonometric equation, solve using algebra.

  1. Look for a pattern that suggests an algebraic property, such as the difference of squares or a factoring opportunity.
  2. Substitute the trigonometric expression with a single variable, such as xx or uu.
  3. Solve the equation the same way an algebraic equation would be solved.
  4. Substitute the trigonometric expression back in for the variable in the resulting expressions.
  5. Solve for the angle.

Example. Solve the equation exactly: 2cosθ3=5, 0θ<2π2\cos\theta-3=-5,\ 0\le\theta<2\pi.

Solution. Use algebraic techniques to solve the equation.

2cosθ3=52cosθ=2cosθ=1θ=π \begin{array}{lrcl} & 2\cos\theta-3 &=& -5 \\[4pt] & 2\cos\theta &=& -2 \\[4pt] & \cos\theta &=& -1 \\[4pt] & \theta &=& \pi \end{array}

Solve exactly the following linear equation on the interval[0,2π)[0,2\pi):2sinx+1=02\sin x+1=0.

Solving Equations Involving a Single Trigonometric Function

When we are given equations that involve only one of the six trigonometric functions, their solutions involve using algebraic techniques and the unit circle. We need to make several considerations when the equation involves trigonometric functions other than sine and cosine. Problems involving the reciprocals of the primary trigonometric functions need to be viewed from an algebraic perspective. In other words, we will write the reciprocal function, and solve for the angles using the function. Also, an equation involving the tangent function is slightly different from one containing a sine or cosine function. First, as we know, the period of tangent is π\pi, not 2π2\pi. Further, the domain of tangent is all real numbers with the exception of odd integer multiples of π2\tfrac{\pi}{2}, unless, of course, a problem places its own restrictions on the domain.

Example. Solve the problem exactly: 2sin2θ1=0, 0θ<2π2\sin^2\theta-1=0,\ 0\le\theta<2\pi.

Solution. As this problem is not easily factored, we will solve using the square root property. First, we use algebra to isolate sinθ\sin\theta. Then we will find the angles.

2sin2θ1=02sin2θ=1sin2θ=12sin2θ=±12sinθ=±12=±22θ=π4,3π4,5π4,7π4 \begin{array}{lrcl} & 2\sin^2\theta-1 &=& 0 \\[4pt] & 2\sin^2\theta &=& 1 \\[4pt] & \sin^2\theta &=& \tfrac12 \\[4pt] & \sqrt{\sin^2\theta} &=& \pm\sqrt{\tfrac12} \\[4pt] & \sin\theta &=& \pm\tfrac{1}{\sqrt2}=\pm\tfrac{\sqrt2}{2} \\[4pt] & \theta &=& \tfrac{\pi}{4},\tfrac{3\pi}{4},\tfrac{5\pi}{4},\tfrac{7\pi}{4} \end{array}

Example. Solve the following equation exactly: cscθ=2, 0θ<4π\csc\theta=-2,\ 0\le\theta<4\pi.

Solution. We want all values of θ\theta for which cscθ=2\csc\theta=-2 over the interval 0θ<4π0\le\theta<4\pi.

cscθ=21sinθ=2sinθ=12θ=7π6,11π6,19π6,23π6 \begin{array}{lrcl} & \csc\theta &=& -2 \\[4pt] & \tfrac{1}{\sin\theta} &=& -2 \\[4pt] & \sin\theta &=& -\tfrac12 \\[4pt] & \theta &=& \tfrac{7\pi}{6},\tfrac{11\pi}{6},\tfrac{19\pi}{6},\tfrac{23\pi}{6} \end{array}

Analysis. As sinθ=12\sin\theta=-\tfrac12, notice that all four solutions are in the third and fourth quadrants.

Example. Solve the equation exactly: tan(θπ2)=1, 0θ<2π\tan\left(\theta-\tfrac{\pi}{2}\right)=1,\ 0\le\theta<2\pi.

Solution. Recall that the tangent function has a period of π\pi. On the interval [0,π)[0,\pi), and at the angle of π4\tfrac{\pi}{4}, the tangent has a value of 11. However, the angle we want is (θπ2)\left(\theta-\tfrac{\pi}{2}\right). Thus, if tan(π4)=1\tan\left(\tfrac{\pi}{4}\right)=1, then

θπ2=π4θ=3π4±kπ \begin{array}{lrcl} & \theta-\tfrac{\pi}{2} &=& \tfrac{\pi}{4} \\[4pt] & \theta &=& \tfrac{3\pi}{4}\pm k\pi \end{array}

Over the interval [0,2π)[0,2\pi), we have two solutions:

3π4 and 3π4+π=7π4\tfrac{3\pi}{4}\ \text{and}\ \tfrac{3\pi}{4}+\pi=\tfrac{7\pi}{4}

Find all solutions fortanx=3\tan x=\sqrt3, usingkkfor any integer and the representative angle in(π2,π2)\left(-\tfrac{\pi}{2},\tfrac{\pi}{2}\right).

Example. Identify all exact solutions to the equation 2(tanx+3)=5+tanx, 0x<2π2(\tan x+3)=5+\tan x,\ 0\le x<2\pi.

Solution. We can solve this equation using only algebra. Isolate the expression tanx\tan x on the left side of the equals sign.

2(tanx)+2(3)=5+tanx2tanx+6=5+tanx2tanxtanx=56tanx=1 \begin{array}{lrcl} & 2(\tan x)+2(3) &=& 5+\tan x \\[4pt] & 2\tan x+6 &=& 5+\tan x \\[4pt] & 2\tan x-\tan x &=& 5-6 \\[4pt] & \tan x &=& -1 \end{array}

There are two angles on the unit circle that have a tangent value of 1-1: θ=3π4\theta=\tfrac{3\pi}{4} and θ=7π4\theta=\tfrac{7\pi}{4}.

Solve Trigonometric Equations Using a Calculator

Not all functions can be solved exactly using only the unit circle. When we must solve an equation involving an angle other than one of the special angles, we will need to use a calculator. Make sure it is set to the proper mode, either degrees or radians, depending on the criteria of the given problem.

Example. Use a calculator to solve the equation sinθ=0.8\sin\theta=0.8, where θ\theta is in radians.

Solution. Make sure mode is set to radians. To find θ\theta, use the inverse sine function. On most calculators, you will need to push the 2ND button and then the SIN button to bring up the sin1\sin^{-1} function. What is shown on the screen is sin1(\sin^{-1}(. The calculator is ready for the input within the parentheses. For this problem, we enter sin1(0.8)\sin^{-1}(0.8), and press ENTER. Thus, to four decimal places,

sin1(0.8)0.9273\sin^{-1}(0.8)\approx0.9273

The solution is

0.9273±2πk0.9273\pm2\pi k

The angle measurement in degrees is

θ53.1θ18053.1126.9 \begin{array}{lrcl} & \theta &\approx& 53.1^\circ \\[4pt] & \theta &\approx& 180^\circ-53.1^\circ \\[4pt] & &\approx& 126.9^\circ \end{array}

Analysis. Note that a calculator will only return an angle in quadrants I or IV for the sine function, since that is the range of the inverse sine. The other angle is obtained by using πθ\pi-\theta.

Example. Use a calculator to solve the equation secθ=4\sec\theta=-4, giving your answer in radians.

Solution. We can begin with some algebra.

secθ=41cosθ=4cosθ=14 \begin{array}{lrcl} & \sec\theta &=& -4 \\[4pt] & \tfrac{1}{\cos\theta} &=& -4 \\[4pt] & \cos\theta &=& -\tfrac14 \end{array}

Check that the MODE is in radians. Now use the inverse cosine function.

cos1(14)1.8235θ1.8235+2πk \begin{array}{lrcl} & \cos^{-1}\left(-\tfrac14\right) &\approx& 1.8235 \\[4pt] & \theta &\approx& 1.8235+2\pi k \end{array}

Since π21.57\tfrac{\pi}{2}\approx1.57 and π3.14\pi\approx3.14, 1.82351.8235 is between these two numbers, thus θ1.8235\theta\approx1.8235 is in quadrant II. Cosine is also negative in quadrant III. Note that a calculator will only return an angle in quadrants I or II for the cosine function, since that is the range of the inverse cosine, as shown below.

So, we also need to find the measure of the angle in quadrant III. In quadrant III, the reference angle is θπ1.82351.3181\theta'\approx\pi-1.8235\approx1.3181. The other solution in quadrant III is π+1.31814.4597\pi+1.3181\approx4.4597.

The solutions are 1.8235±2πk1.8235\pm2\pi k and 4.4597±2πk4.4597\pm2\pi k.

Solvecosθ=0.2\cos\theta=-0.2, giving each family of solutions to four decimal places, usingkkfor any integer and representative angles in[0,2π)[0,2\pi).

Solving Trigonometric Equations in Quadratic Form

Solving a quadratic equation may be more complicated, but once again, we can use algebra as we would for any quadratic equation. Look at the pattern of the equation. Is there more than one trigonometric function in the equation, or is there only one? Which trigonometric function is squared? If there is only one function represented and one of the terms is squared, think about the standard form of a quadratic. Replace the trigonometric function with a variable such as xx or uu. If substitution makes the equation look like a quadratic equation, then we can use the same methods for solving quadratics to solve the trigonometric equations.

Example. Solve the equation exactly: cos2θ+3cosθ1=0, 0θ<2π\cos^2\theta+3\cos\theta-1=0,\ 0\le\theta<2\pi.

Solution. We begin by using substitution and replacing cosθ\cos\theta with xx. It is not necessary to use substitution, but it may make the problem easier to solve visually. Let cosθ=x\cos\theta=x. We have

x2+3x1=0x^2+3x-1=0

The equation cannot be factored, so we will use the quadratic formula x=b±b24ac2ax=\tfrac{-b\pm\sqrt{b^2-4ac}}{2a}.

x=3±(3)24(1)(1)2=3±132 \begin{array}{lrcl} & x &=& \tfrac{-3\pm\sqrt{(3)^2-4(1)(-1)}}{2} \\[4pt] & &=& \tfrac{-3\pm\sqrt{13}}{2} \end{array}

Replace xx with cosθ\cos\theta, and solve. Thus,

cosθ=3±132θ=cos1(3+132) \begin{array}{lrcl} & \cos\theta &=& \tfrac{-3\pm\sqrt{13}}{2} \\[4pt] & \theta &=& \cos^{-1}\left(\tfrac{-3+\sqrt{13}}{2}\right) \end{array}

Note that only the ++ sign is used. This is because we get an error when we solve θ=cos1(3132)\theta=\cos^{-1}\left(\tfrac{-3-\sqrt{13}}{2}\right) on a calculator, since the domain of the inverse cosine function is [1,1][-1,1]. However, there is a second solution:

cos1(3+132)1.26 \begin{array}{lrcl} & \cos^{-1}\left(\tfrac{-3+\sqrt{13}}{2}\right) \\[4pt] & \approx1.26 \end{array}

This terminal side of the angle lies in quadrant I. Since cosine is also positive in quadrant IV, the second solution is

2πcos1(3+132)5.02 \begin{array}{lrcl} & 2\pi-\cos^{-1}\left(\tfrac{-3+\sqrt{13}}{2}\right) \\[4pt] & \approx5.02 \end{array}

Example. Solve the equation exactly: 2sin2θ5sinθ+3=0, 0θ2π2\sin^2\theta-5\sin\theta+3=0,\ 0\le\theta\le2\pi.

Solution. Using grouping, this quadratic can be factored. Either make the real substitution, sinθ=u\sin\theta=u, or imagine it, as we factor:

2sin2θ5sinθ+3=0(2sinθ3)(sinθ1)=0 \begin{array}{lrcl} & 2\sin^2\theta-5\sin\theta+3 &=& 0 \\[4pt] & (2\sin\theta-3)(\sin\theta-1) &=& 0 \end{array}

Now set each factor equal to zero.

2sinθ3=02sinθ=3sinθ=32 \begin{array}{lrcl} & 2\sin\theta-3 &=& 0 \\[4pt] & 2\sin\theta &=& 3 \\[4pt] & \sin\theta &=& \tfrac32 \end{array} sinθ1=0sinθ=1 \begin{array}{lrcl} & \sin\theta-1 &=& 0 \\[4pt] & \sin\theta &=& 1 \end{array}

Next solve for θ\theta: sinθ32\sin\theta\ne\tfrac32, as the range of the sine function is [1,1][-1,1]. However, sinθ=1\sin\theta=1, giving the solution π2\tfrac{\pi}{2}.

Analysis. Make sure to check all solutions on the given domain as some factors have no solution.

Solvesin2θ=2cosθ+2\sin^2\theta=2\cos\theta+2on[0,2π][0,2\pi].

Example. Solve exactly:

2sin2θ+sinθ=0; 0θ<2π2\sin^2\theta+\sin\theta=0;\ 0\le\theta<2\pi

Solution. This problem should appear familiar as it is similar to a quadratic. Let sinθ=x\sin\theta=x. The equation becomes 2x2+x=02x^2+x=0. We begin by factoring:

2x2+x=0x(2x+1)=0 \begin{array}{lrcl} & 2x^2+x &=& 0 \\[4pt] & x(2x+1) &=& 0 \end{array}

Set each factor equal to zero.

x=0(2x+1)=0x=12 \begin{array}{lrcl} & x &=& 0 \\[4pt] & (2x+1) &=& 0 \\[4pt] & x &=& -\tfrac12 \end{array}

Then, substitute back into the equation the original expression sinθ\sin\theta for xx. Thus,

sinθ=0θ=0,π \begin{array}{lrcl} & \sin\theta &=& 0 \\[4pt] & \theta &=& 0,\pi \end{array} sinθ=12θ=7π6,11π6 \begin{array}{lrcl} & \sin\theta &=& -\tfrac12 \\[4pt] & \theta &=& \tfrac{7\pi}{6},\tfrac{11\pi}{6} \end{array}

The solutions within the domain 0θ<2π0\le\theta<2\pi are 0,π,7π6,11π60,\pi,\tfrac{7\pi}{6},\tfrac{11\pi}{6}.

If we prefer not to substitute, we can solve the equation by following the same pattern of factoring and setting each factor equal to zero.

2sin2θ+sinθ=0sinθ(2sinθ+1)=0sinθ=0θ=0,π \begin{array}{lrcl} & 2\sin^2\theta+\sin\theta &=& 0 \\[4pt] & \sin\theta(2\sin\theta+1) &=& 0 \\[4pt] & \sin\theta &=& 0 \\[4pt] & \theta &=& 0,\pi \end{array} 2sinθ+1=02sinθ=1sinθ=12θ=7π6,11π6 \begin{array}{lrcl} & 2\sin\theta+1 &=& 0 \\[4pt] & 2\sin\theta &=& -1 \\[4pt] & \sin\theta &=& -\tfrac12 \\[4pt] & \theta &=& \tfrac{7\pi}{6},\tfrac{11\pi}{6} \end{array}

Analysis. We can see the solutions on the graph below. On the interval 0θ<2π0\le\theta<2\pi, the graph crosses the xx-axis four times, at the solutions noted. Notice that trigonometric equations that are in quadratic form can yield up to four solutions instead of the expected two that are found with quadratic equations. In this example, each solution (angle) corresponding to a positive sine value will yield two angles that would result in that value.

We can verify the solutions on the unit circle as well.

Solve the quadratic equation2cos2θ+cosθ=02\cos^2\theta+\cos\theta=0on[0,2π)[0,2\pi).

Example. Solve the equation quadratic in form exactly: 2sin2θ3sinθ+1=0, 0θ<2π2\sin^2\theta-3\sin\theta+1=0,\ 0\le\theta<2\pi.

Solution. We can factor using grouping. Solution values of θ\theta can be found on the unit circle:

(2sinθ1)(sinθ1)=02sinθ1=0sinθ=12θ=π6,5π6 \begin{array}{lrcl} & (2\sin\theta-1)(\sin\theta-1) &=& 0 \\[4pt] & 2\sin\theta-1 &=& 0 \\[4pt] & \sin\theta &=& \tfrac12 \\[4pt] & \theta &=& \tfrac{\pi}{6},\tfrac{5\pi}{6} \end{array} sinθ=1θ=π2 \begin{array}{lrcl} & \sin\theta &=& 1 \\[4pt] & \theta &=& \tfrac{\pi}{2} \end{array}

Solving Trigonometric Equations Using Fundamental Identities

While algebra can be used to solve a number of trigonometric equations, we can also use the fundamental identities because they make solving equations simpler. Remember that the techniques we use for solving are not the same as those for verifying identities. The basic rules of algebra apply here, as opposed to rewriting one side of the identity to match the other side. In the next example, we use two identities to simplify the equation.

Example. Use identities to solve exactly the trigonometric equation over the interval 0x<2π0\le x<2\pi.

cosxcos(2x)+sinxsin(2x)=32\cos x\cos(2x)+\sin x\sin(2x)=\tfrac{\sqrt3}{2}

Solution. Notice that the left side of the equation is the difference formula for cosine.

Difference formula for cosine.cos(x2x)=32Use the negative angle identity.cos(x)=32cosx=32 \begin{array}{lrcl} \text{Difference formula for cosine.} & \cos(x-2x) &=& \tfrac{\sqrt3}{2} \\[4pt] \text{Use the negative angle identity.} & \cos(-x) &=& \tfrac{\sqrt3}{2} \\[4pt] & \cos x &=& \tfrac{\sqrt3}{2} \end{array}

From the unit circle, we see that cosx=32\cos x=\tfrac{\sqrt3}{2} when x=π6,11π6x=\tfrac{\pi}{6},\tfrac{11\pi}{6}.

Example. Solve the equation exactly using a double-angle formula: cos(2θ)=cosθ\cos(2\theta)=\cos\theta.

Solution. We have three choices of expressions to substitute for the double-angle of cosine. As it is simpler to solve for one trigonometric function at a time, we will choose the double-angle identity involving only cosine:

cos(2θ)=cosθ2cos2θ1=cosθ2cos2θcosθ1=0(2cosθ+1)(cosθ1)=0 \begin{array}{lrcl} & \cos(2\theta) &=& \cos\theta \\[4pt] & 2\cos^2\theta-1 &=& \cos\theta \\[4pt] & 2\cos^2\theta-\cos\theta-1 &=& 0 \\[4pt] & (2\cos\theta+1)(\cos\theta-1) &=& 0 \end{array} 2cosθ+1=0cosθ=12 \begin{array}{lrcl} & 2\cos\theta+1 &=& 0 \\[4pt] & \cos\theta &=& -\tfrac12 \end{array} cosθ1=0cosθ=1 \begin{array}{lrcl} & \cos\theta-1 &=& 0 \\[4pt] & \cos\theta &=& 1 \end{array}

So, if cosθ=12\cos\theta=-\tfrac12, then θ=2π3±2πk\theta=\tfrac{2\pi}{3}\pm2\pi k and θ=4π3±2πk\theta=\tfrac{4\pi}{3}\pm2\pi k; if cosθ=1\cos\theta=1, then θ=0±2πk\theta=0\pm2\pi k.

Example. Solve the equation exactly using an identity: 3cosθ+3=2sin2θ, 0θ<2π3\cos\theta+3=2\sin^2\theta,\ 0\le\theta<2\pi.

Solution. If we rewrite the right side, we can write the equation in terms of cosine:

3cosθ+3=2sin2θ3cosθ+3=2(1cos2θ)3cosθ+3=22cos2θ2cos2θ+3cosθ+1=0(2cosθ+1)(cosθ+1)=0 \begin{array}{lrcl} & 3\cos\theta+3 &=& 2\sin^2\theta \\[4pt] & 3\cos\theta+3 &=& 2(1-\cos^2\theta) \\[4pt] & 3\cos\theta+3 &=& 2-2\cos^2\theta \\[4pt] & 2\cos^2\theta+3\cos\theta+1 &=& 0 \\[4pt] & (2\cos\theta+1)(\cos\theta+1) &=& 0 \end{array} 2cosθ+1=0cosθ=12θ=2π3,4π3 \begin{array}{lrcl} & 2\cos\theta+1 &=& 0 \\[4pt] & \cos\theta &=& -\tfrac12 \\[4pt] & \theta &=& \tfrac{2\pi}{3},\tfrac{4\pi}{3} \end{array} cosθ+1=0cosθ=1θ=π \begin{array}{lrcl} & \cos\theta+1 &=& 0 \\[4pt] & \cos\theta &=& -1 \\[4pt] & \theta &=& \pi \end{array}

Our solutions are 2π3,4π3,π\tfrac{2\pi}{3},\tfrac{4\pi}{3},\pi.

Solving Trigonometric Equations with Multiple Angles

Sometimes it is not possible to solve a trigonometric equation with identities that have a multiple angle, such as sin(2x)\sin(2x) or cos(3x)\cos(3x). When confronted with these equations, recall that y=sin(2x)y=\sin(2x) is a horizontal compression by a factor of 22 of the function y=sinxy=\sin x. On an interval of 2π2\pi, we can graph two periods of y=sin(2x)y=\sin(2x), as opposed to one cycle of y=sinxy=\sin x. This compression of the graph leads us to believe there may be twice as many xx-intercepts or solutions to sin(2x)=0\sin(2x)=0 compared to sinx=0\sin x=0. This information will help us solve the equation.

Example. Solve exactly: cos(2x)=12\cos(2x)=\tfrac12 on [0,2π)[0,2\pi).

Solution. We can see that this equation is the standard equation with a multiple of an angle. If cos(α)=12\cos(\alpha)=\tfrac12, we know α\alpha is in quadrants I and IV. While θ=cos112\theta=\cos^{-1}\tfrac12 will only yield solutions in quadrants I and II, we recognize that the solutions to the equation cosθ=12\cos\theta=\tfrac12 will be in quadrants I and IV.

Therefore, the possible angles are θ=π3\theta=\tfrac{\pi}{3} and θ=5π3\theta=\tfrac{5\pi}{3}. So, 2x=π32x=\tfrac{\pi}{3} or 2x=5π32x=\tfrac{5\pi}{3}, which means that x=π6x=\tfrac{\pi}{6} or x=5π6x=\tfrac{5\pi}{6}. Does this make sense? Yes, because cos(2(π6))=cos(π3)=12\cos\left(2\left(\tfrac{\pi}{6}\right)\right)=\cos\left(\tfrac{\pi}{3}\right)=\tfrac12.

Are there any other possible answers? Let us return to our first step.

In quadrant I, 2x=π32x=\tfrac{\pi}{3}, so x=π6x=\tfrac{\pi}{6} as noted. Let us revolve around the circle again:

2x=π3+2π=π3+6π3=7π3 \begin{array}{lrcl} & 2x &=& \tfrac{\pi}{3}+2\pi \\[4pt] & &=& \tfrac{\pi}{3}+\tfrac{6\pi}{3} \\[4pt] & &=& \tfrac{7\pi}{3} \end{array}

so x=7π6x=\tfrac{7\pi}{6}.

One more rotation yields

2x=π3+4π=π3+12π3=13π3 \begin{array}{lrcl} & 2x &=& \tfrac{\pi}{3}+4\pi \\[4pt] & &=& \tfrac{\pi}{3}+\tfrac{12\pi}{3} \\[4pt] & &=& \tfrac{13\pi}{3} \end{array}

x=13π6>2πx=\tfrac{13\pi}{6}>2\pi, so this value for xx is larger than 2π2\pi, so it is not a solution on [0,2π)[0,2\pi).

In quadrant IV, 2x=5π32x=\tfrac{5\pi}{3}, so x=5π6x=\tfrac{5\pi}{6} as noted. Let us revolve around the circle again:

2x=5π3+2π=5π3+6π3=11π3 \begin{array}{lrcl} & 2x &=& \tfrac{5\pi}{3}+2\pi \\[4pt] & &=& \tfrac{5\pi}{3}+\tfrac{6\pi}{3} \\[4pt] & &=& \tfrac{11\pi}{3} \end{array}

so x=11π6x=\tfrac{11\pi}{6}.

One more rotation yields

2x=5π3+4π=5π3+12π3=17π3 \begin{array}{lrcl} & 2x &=& \tfrac{5\pi}{3}+4\pi \\[4pt] & &=& \tfrac{5\pi}{3}+\tfrac{12\pi}{3} \\[4pt] & &=& \tfrac{17\pi}{3} \end{array}

x=17π6>2πx=\tfrac{17\pi}{6}>2\pi, so this value for xx is larger than 2π2\pi, so it is not a solution on [0,2π)[0,2\pi).

Our solutions are π6,5π6,7π6,and 11π6\tfrac{\pi}{6},\tfrac{5\pi}{6},\tfrac{7\pi}{6},\text{and}\ \tfrac{11\pi}{6}. Note that whenever we solve a problem in the form of sin(nx)=c\sin(nx)=c, we must go around the unit circle nn times.

Solving Right Triangle Problems

We can now use all of the methods we have learned to solve problems that involve applying the properties of right triangles and the Pythagorean Theorem. We begin with the familiar Pythagorean Theorem, a2+b2=c2a^2+b^2=c^2, and model an equation to fit a situation.

Example. Use the Pythagorean Theorem, and the properties of right triangles to model an equation that fits the problem.

One of the cables that anchors the center of the London Eye Ferris wheel to the ground must be replaced. The center of the Ferris wheel is 69.569.5 meters above the ground, and the second anchor on the ground is 2323 meters from the base of the Ferris wheel. Approximately how long is the cable, and what is the angle of elevation (from ground up to the center of the Ferris wheel)? See the figure below.

Solution. Using the information given, we can draw a right triangle. We can find the length of the cable with the Pythagorean Theorem.

a2+b2=c2(23)2+(69.5)25,3595,35973.2 m \begin{array}{lrcl} & a^2+b^2 &=& c^2 \\[4pt] & (23)^2+(69.5)^2 &\approx& 5{,}359 \\[4pt] & \sqrt{5{,}359} &\approx& 73.2\ \text{m} \end{array}

The angle of elevation is θ\theta, formed by the second anchor on the ground and the cable reaching to the center of the wheel. We can use the tangent function to find its measure. Round to two decimal places.

tanθ=69.523tan1(69.523)1.252271.69 \begin{array}{lrcl} & \tan\theta &=& \tfrac{69.5}{23} \\[4pt] & \tan^{-1}\left(\tfrac{69.5}{23}\right) &\approx& 1.2522 \\[4pt] & &\approx& 71.69^\circ \end{array}

The angle of elevation is approximately 71.771.7^\circ, and the length of the cable is 73.273.2 meters.

Example. Use the Pythagorean Theorem, and the properties of right triangles to model an equation that fits the problem.

OSHA safety regulations require that the base of a ladder be placed 11 foot from the wall for every 44 feet of ladder length. Find the angle that a ladder of any length forms with the ground and the height at which the ladder touches the wall.

Solution. For any length of ladder, the base needs to be a distance from the wall equal to one fourth of the ladder’s length. Equivalently, if the base of the ladder is “aa” feet from the wall, the length of the ladder will be 4a4a feet. See the figure below.

The side adjacent to θ\theta is aa and the hypotenuse is 4a4a. Thus,

cosθ=a4a=14cos1(14)75.5 \begin{array}{lrcl} & \cos\theta &=& \tfrac{a}{4a}=\tfrac14 \\[4pt] & \cos^{-1}\left(\tfrac14\right) &\approx& 75.5^\circ \end{array}

The elevation of the ladder forms an angle of 75.575.5^\circ with the ground. The height at which the ladder touches the wall can be found using the Pythagorean Theorem:

a2+b2=(4a)2b2=(4a)2a2b2=16a2a2b2=15a2b=15a \begin{array}{lrcl} & a^2+b^2 &=& (4a)^2 \\[4pt] & b^2 &=& (4a)^2-a^2 \\[4pt] & b^2 &=& 16a^2-a^2 \\[4pt] & b^2 &=& 15a^2 \\[4pt] & b &=& \sqrt{15}\,a \end{array}

Thus, the ladder touches the wall at 15a\sqrt{15}\,a feet from the ground.

Key concepts

  • When solving linear trigonometric equations, we can use algebraic techniques just as we do solving algebraic equations. Look for patterns, like the difference of squares, quadratic form, or an expression that lends itself well to substitution.
  • Equations involving a single trigonometric function can be solved or verified using the unit circle.
  • We can also solve trigonometric equations using a graphing calculator.
  • Many equations appear quadratic in form. We can use substitution to make the equation appear simpler, and then use the same techniques we use solving an algebraic quadratic: factoring, the quadratic formula, etc.
  • We can also use the identities to solve trigonometric equations.
  • We can use substitution to solve a multiple-angle trigonometric equation, which is a compression of a standard trigonometric function. We will need to take the compression into account and verify that we have found all solutions on the given interval.
  • Real-world scenarios can be modeled and solved using the Pythagorean Theorem and trigonometric functions.

Practice

Solve linear trigonometric equations in sine and cosine

Find all exact solutions on[0,2π)[0,2\pi):2sinθ=32\sin\theta=\sqrt3.

Solve exactly on[0,2π)[0,2\pi):2cosθ=22\cos\theta=-\sqrt2.

Solve equations involving a single trigonometric function

Find all solutions exactly on[0,2π)[0,2\pi):4sin2x2=04\sin^2x-2=0.

Solve exactly on[0,2π)[0,2\pi):sec2x=1\sec^2x=1.

Solve trigonometric equations using a calculator

Use a calculator to find all solutions tosinx=0.27\sin x=0.27, to four decimal places, usingkkfor any integer and representative angles in[0,2π)[0,2\pi).

Use a calculator to find all solutions totanx=0.34\tan x=-0.34, to four decimal places, usingkkfor any integer and the representative angle in(π2,π2)\left(-\tfrac{\pi}{2},\tfrac{\pi}{2}\right).

Solve trigonometric equations that are quadratic in form

Find all exact solutions on[0,2π)[0,2\pi):tan2x3tanx=0\tan^2x-\sqrt3\tan x=0.

Solvesin2x2sinx4=0\sin^2x-2\sin x-4=0on[0,2π)[0,2\pi).

Solve trigonometric equations using fundamental identities

Find all exact solutions on[0,2π)[0,2\pi):cos3t=cost\cos^3t=\cos t.

Find all exact solutions on[0,2π)[0,2\pi):12sin2t+cost6=012\sin^2t+\cos t-6=0.

Solve trigonometric equations with multiple angles

Find all exact solutions on[0,2π)[0,2\pi):2sin(3θ)=12\sin(3\theta)=1.

Find all exact solutions on[0,2π)[0,2\pi):2cos(3θ)=22\cos(3\theta)=-\sqrt2.

Solve right triangle problems

An airplane has only enough gas to fly to a city200200miles northeast of its current location. If the pilot knows that the city is2525miles north, how many degrees north of east should the airplane fly? Round to the nearest tenth of a degree.

If a loading ramp is placed next to a truck, at a height of22feet, and the ramp is2020feet long, what angle does the ramp make with the ground? Round to the nearest tenth of a degree.


This section is adapted from Precalculus 2e, Section 7.5: Solving Trigonometric Equations by Jay Abramson and OpenStax, © OpenStax, licensed under CC BY-NC-SA 4.0. Access the original for free at openstax.org. Changes: omitted the decorative photo of the Egyptian pyramids (Figure 1), which carries no mathematics beyond the credit line; recreated the four instructional figures as accessible spec-first SVGs — the reference-angle diagram accompanying the calculator secant example (two terminal rays in standard position with their arcs, sampled from the exact solved angles); the graph of y=2sin2θ+sinθy=2\sin^2\theta+\sin\theta accompanying its Analysis, sampled as a dense polyline from the exact formula over [π6,13π6]\left[-\tfrac{\pi}{6},\tfrac{13\pi}{6}\right] (never a freehand curve) with the source’s own π6\tfrac{\pi}{6}-multiple tick labels; the Ferris wheel right triangle with the wheel drawn as a circle centered at the cable’s top vertex; and the generic ladder right triangle. Three sentences that cited a “unit circle” figure appearing elsewhere in the chapter (a different module’s figure, not this section’s own) are reworded to refer to the unit circle generically rather than point at a specific figure number, since that figure is outside this page’s scope. Every retained Try It became a real fillin component, each carrying the answerForm the printed subject demands to block a retype of the equation itself: radians on every interval-restricted list and general solution, with answerMode="unordered" on every list of two or more members (member order carries no meaning, and the engine grades a swapped order and an equation-wrapped restatement the same). Every general-solution question additionally names kk as the integer parameter, states the rounding its own printed key uses, and pins the representative angle’s range, since the grader compares one keyed representative strictly — instructions the source’s bare “find all solutions” wording leaves implicit. The Try It following Example 12 (a quadratic-in-form equation with no interval stated in the source, unlike every other equation in its subsection) is stated on [0,2π)[0,2\pi) to match the domain its own printed answer key assumes and the domain used by the surrounding worked examples. Adapted fourteen selected end-of-section exercises — two linear, two single-function, two calculator/general-solution, two quadratic-form (one the “no real solution” case recast as a multiplechoice, since a categorical non-existence claim has no free-response answer), one identity-based quadratic-form, one pure-identity, two multiple-angle, and two right-triangle word problems — into a closing Practice block, one group per objective, every item independently re-derived (including by running the arithmetic in Node) rather than read off the source key.