Sign In
| 11 Theory slides |
| 9 Exercises - Grade E - A |
| Each lesson is meant to take 1-2 classroom sessions |
Here are a few recommended readings before getting started with this lesson.
On Sunday, Magdalena and her younger sister Paulina went to the amusement park Adventurally with their father. They all had a lot of fun going on numerous rides, including a Ferris Wheel. When they first saw it close up, the girls were so amazed by its size that they asked one of the workers for more details about it.
There are functions that undo the trigonometric functions, so to speak. These functions are called inverse trigonometric functions.
The inverse trigonometric functions are the inverse functions of the trigonometric functions. For example, the inverse sine is the inverse function of the sine function. The main inverse trigonometric functions are shown in the table below.
Trigonometric Function | Inverse Trigonometric Function |
---|---|
f(x)=sinx | f-1(x)=sin-1x |
f(x)=cosx | f-1(x)=cos-1x |
f(x)=tanx | f-1(x)=tan-1x |
Inverse Trigonometric Function | Domain | Range |
---|---|---|
y=sin-1x | [-1,1] | -2π≤x≤2π |
y=cos-1x | [-1,1] | 0≤x≤π |
y=tan-1x | All real numbers | -2π≤x≤2π |
Contrary to trigonometric identities — which are true for all values of the variable for which both sides are defined — some equations involving trigonometric functions are true only for certain values of the variable. Now such equations will be presented.
To sum up, the following facts can be used to solve trigonometric equations. Note that n and m written below are integers.
Equation | Solutions |
---|---|
sinθ=sinα | θ=nπif n is odd, if n is even, +(-1)nα⇓θ=(2m+1)π−αθ=2mπ+α
|
cosθ=cosα | θ=2nπ±α |
tanθ=tanα | θ=nπ+α |
cos(2θ)=1−2sin2(θ)
LHS+2sin2θ=RHS+2sin2θ
LHS−1=RHS−1
Rearrange equation
Commutative Property of Addition
Rewrite 15sinθ as 14sinθ+sinθ
Distribute -1
LHS+1=RHS+1
LHS/2=RHS/2
sin-1(LHS)=sin-1(RHS)
f-1(f(x))=x
cos(2θ)=2cos2(θ)−1
LHS+3=RHS+3
Commutative Property of Addition
LHS/2=RHS/2
a2+2ab+b2=(a+b)2
LHS=RHS
LHS−1=RHS−1
sec2θ=1+tan2θ
LHS−tan2θ=RHS−tan2θ
LHS+1=RHS+1
LHS/2=RHS/2
LHS=RHS
The teacher gave the class a couple of exercises to solve for homework. She also warned that one of the equations has extraneous solutions and that the students should identify them. To make things interesting, Magdalena and Davontay decided to make a bet about which equation has extraneous solutions.
After each chose an equation, they started solving them to see who guessed correctly. The winner will get the last piece of cake left in the fridge. To solve the equations, they must write all the solutions in radians such that 0≤θ≤2π.
cos2θ=1−sin2θ
Distribute 2
Commutative Property of Addition
LHS−3=RHS−3
LHS⋅(-1)=RHS⋅(-1)
Rewrite 3sinθ as 2sinθ+sinθ
Distribute -1
Factor out 2sinθ
Factor out -1
Factor out sinθ−1
(I), (II): LHS+1=RHS+1
(I): LHS/2=RHS/2
θ=6π
(ba)m=bmam
a⋅cb=ca⋅b
ba=b/2a/2
Add fractions
Solution | Substitute | Evaluate | True or False |
---|---|---|---|
θ=6π | 2cos2(6π)+3sin(6π)=?3 | 2(23)2+3(21)=?3 | 3=3 ✓ |
θ=65π | 2cos2(65π)+3sin(65π)=?3 | 2(-23)2+3(21)=?3 | 3=3 ✓ |
θ=2π | 2cos2(2π)+3sin(2π)=?3 | 2(0)2+3(1)=?3 | 3=3 ✓ |
Therefore, there are three solutions to the equation and none of them are extraneous.
cos2θ=1−sin2θ
LHS+sin2θ=RHS+sin2θ
LHS/2=RHS/2
LHS=RHS
ba=ba
ba=b⋅2a⋅2
Solution | Substitute | Evaluate | True or False |
---|---|---|---|
θ1=4π | sin(4π)−cos(4π)=?0 | 22−22=?0 | 0=0 ✓ |
θ2=43π | sin(43π)−cos(43π)=?0 | 22−(-22)=?0 | 2=0 × |
θ3=45π | sin(45π)−cos(45π)=?0 | -22−(-22)=?0 | 0=0 ✓ |
θ4=47π | sin(47π)−cos(47π)=?0 | -22−22=?0 | -2=0 × |
It can be concluded that θ=43π and θ=47π are extraneous solutions. Therefore, only θ=4π and θ=45π are solutions to the equation. This means that Davontay bet on the right equation and he will get the last piece of the cake!
Magdalena's math teacher designed a labyrinth in the school athletics field for her students. To determine which direction to go at each crossroad, she made signs with certain clues. At one of the crossroads, the clue said to follow the direction that is not a solution to either of the two given trigonometric equations.
The clue also advised to graph the solutions on a unit circle. Write all the possible solutions in the form of general equations where n is an integer number.
cot(θ)=sin(θ)cos(θ)
a⋅cb=ca⋅b
ba=b/sinθa/sinθ
Factor out cosθ
As shown on the unit circle, the solutions are located at two out of the four cardinal directions, north and south. Therefore, these are the directions the students should not choose.
sec2θ=1+tan2θ
Distribute -1
Subtract term
Rearrange equation
The solution is located in the western direction, which means that students should not choose it. Considering the solutions to the first equation, the only direction left is east, so the students should turn east at the crossroad.
sin(2θ)=2sin(θ)cos(θ)
LHS−(3sinθ+cosθ)=RHS−(3sinθ+cosθ)
Distribute -1
Commutative Property of Addition
(I): LHS+1=RHS+1
(I): LHS/2=RHS/2
(II): LHS+23=RHS+23
cos(2π−θ)=sin(θ)
csc(θ)=sin(θ)1
LHS⋅sinθ=RHS⋅sinθ
LHS=RHS
It was finally the weekend and Madgalena and her family went on a boat ride on the local river. A man who worked there said that there was a very high tide recently.
When Magdalena asked how they measure the height of the tide, the worker said that, in addition to sensors, they also use a formula to determine the height of the tide.10:40 PM and 1:20 AM
h=4
LHS/5=RHS/5
cos-1(LHS)=cos-1(RHS)
f-1(f(x))=x
Rearrange equation
LHS⋅2π13=RHS⋅2π13
Use a calculator
Round to 2 decimal place(s)
It was previously stated that when Magdalena and Paulina were at the amusement park Adventurally, they were so amazed by the size of the Ferris wheel that they asked a worker about how large it is.
h=34
LHS−23=RHS−23
LHS/(-22)=RHS/(-22)
Put minus sign in front of fraction
ba=b/11a/11
Rearrange equation
ca⋅b=ca⋅b
Multiply fractions
ba=b/3 mina/3 min
Multiply
Calculate quotient
Round to 1 decimal place(s)
t=3.5
Multiply
Use a calculator
Subtract term
We know that the number d hours of daylight in Mackinaw City, MI, can be approximated by the following equation, where t is the number of days after March 21^(st). d = 4sin 2π365t+12 We want to find the days when Mackinaw City has exactly 10 hours of sunlight. Let's write an equation for the values of t that correspond to d = 10. d = 4sin 2π365t+12 ⇓ 10= 4sin 2π365t+12 To solve the given equation, we will first isolate sin 2π365t in the equation. Then we will use the unit circle to find the exact values of t that satisfy the equation. Let's solve the equation for sin 2π365t.
The value of sin 2π365t that corresponds to d = 10 is - 12. The sine of an angle in standard position is the y-coordinate of the point of intersection P of its terminal side and the unit circle. P(x,y)=(cosθ,sinθ) To solve the equation sin 2π365t =- 12, we need to consider the points on the unit circle that have a y-coordinate of - 12. Recall that sine is negative in Quadrants III and IV.
We can now draw two congruent right triangles, each with a leg on the x-axis. Since the radius of the unit circle is 1, the hypotenuse of each triangle is also 1. Furthermore, since the y-coordinate of both points is - 12, the length of the leg which is not on the x-axis of each triangle is 12.
For both triangles one of the legs is half the hypotenuse, so they are 30^(∘)-60^(∘)-90^(∘) triangles. In this type of triangle, the smaller angle measures 30^(∘) or π6 radians. Knowing that a half turn is π radians and a full turn measures 2π radians, we can calculate the desired angle measures. We will add π6 to π, and subtract π6 from 2π.
We found two solutions for the equation sin 2π365t =- 12. 2π365t= 7π6 and 2π365t= 11π6 This gives us two equations for t. Let's solve them one by one, starting with 2π365t= 7π6.
One of the days when Mackinaw City will have exactly 10 hours of daylight is 213 days from March 21^(st). To find the second day, let's solve the second equation!
The two days when Mackinaw City will have exactly 10 hours of daylight are 213 and 335 days from March 21^(st).
We want to use the information from Part A to find which days of the year have less than 10 hours of daylight. We know that the city gets exactly 10 hours of daylight on the 213^(rd) and 335^(th) day after March 21^(st). Furthermore, the number of hours of daylight each day is modeled by the equation d = 4sin 2π365t+12. Let's graph this equation.
From the graph we can say that the days between the 213^(th) and 335^(th) days get no more than 10 hours of daylight. Note that the shortest day in a year occurs around December 21^(st). That is, the number of hours of daylight must fall from 213^(rd) day to December 21^(st) and rise from December 21^(st) to the 335^(th) day.
We will suppose that the outside temperature is modeled by the given function. f(t) = 26-6cos( π12t) We are told that an air conditioner cools Tadeo's house when the outside temperature is above 24 degrees Celcius. Let's set f(t) as 24 and solve it for t. By doing this, we will find times when it is 24^(∘)C outside.
The air conditioner is turned on about 4.7 hours after midnight. Note that 0.7 hours is 42 minutes. In other words, the air conditioner starts to work at 4:42AM. Let's now consider the graph of the function.
We can see that the graph is symmetric about the line x=12. Since the difference between 12 and 4.7 is 7.3, we can determine the time when the air condition is turned off by adding 7.3 to 12. This is equal to 19.3.
About 19.3 hours after midnight the air conditioner is turned off. Since 0.3 hours is 18 minutes, the air conditioner stops at 19:18, or 7:18PM. As a result, the air conditioner runs from 4:42AM to 7:18PM.
Let's first rewrite the given trigonometric equation.
We can now factor the equation and use the Zero Product Property to solve for sinθ and tan θ. Then we will use the unit circle to find the exact values of θ that satisfy the equation.
Let's start by factoring the expression on the left-hand side. Then, let's use the Zero Product Property to solve the equation for sin θ and tan θ.
Now, let's solve the obtained equations for θ.
To solve the equation tan θ = 0, recall the graph of the tangent function. Let's also draw the line y = 0 to see for which values of θ we have tan θ = 0.
We see that the first non-negative solution to the equation is θ = 0^(∘). We also see that solutions repeat every 180^(∘). With this information, we can write the general form for all the solutions to the equation tan θ = 0. 0^(∘) + k * 180^(∘) Here, k is any integer number.
To solve the equation sin θ = 1, recall the graph of the sine function. Let's also draw the line y = 1 to see for which values of θ we have sin θ = 1.
We see that the first positive solution to the equation is θ = 90^(∘). We also see that solutions repeat every 360^(∘). With this information, we can write the general form for all the solutions to the equation sin θ = 1. 90^(∘) + k * 360^(∘) Here, again, k is any integer number.
While solving equations tan θ =0 and sin θ = 1, we have found the following solutions.
Equations | Solutions |
---|---|
tanθ =0 | 0^(∘)+k * 180^(∘) |
sinθ = 1 | 90^(∘) + k * 360^(∘) |
These are also all the values that could be the solutions to our original equation. However, we need to check whether there are no extraneous solutions.
Since we only have two trigonometric functions in the original equation, and out of them only cos θ makes the equation undefined for some values of θ. The cosine function is the only possible source of extraneous solutions. Let's recall its graph and plot the solutions of the form 90^(∘)+k* 360^(∘).
We see that for every solution of the form 90^(∘)+k* 360^(∘), the cosine function is zero, and therefore makes the original equation undefined. Therefore, these solutions are extraneous solutions to our original equation. This means that all solutions to the original equation are multiples of 180^(∘). 0^(∘)+k * 180^(∘)
Alternatively, we can start by multiplying the equation by cos θ. After solving the resulting equation for θ, we exclude the values of θ that make cos θ equal to zero. This is because cos θ is the denominator of the original equation. Let's find the solutions using this strategy.
We can now use the Zero Product Property to solve for sin θ.
Now, let's solve the obtained equations for θ. To solve the equation sin θ = 0, recall the graph of the sine function. Let's also draw the line y = 0 to see for which values of θ we have sin θ = 0.
We see that the first non-negative solution to the equation is θ = 0^(∘). We also see that solutions repeat every 180^(∘). 0^(∘) + k * 180^(∘), where k ∈ Z Earlier, we found the general form for all the solutions to the equation sin θ = 1 to be the following. 90^(∘) + k * 360^(∘), where k ∈ Z We found the following solutions.
Equations | Solutions |
---|---|
sinθ =0 | 0^(∘)+k * 180^(∘) |
sinθ = 1 | 90^(∘) + k * 360^(∘) |
These are also all the values that could be the solutions to our original equation. Recall that cos θ cannot be zero. We have shown that for every solution of the form 90^(∘)+k* 360^(∘), the cosine function is zero, and therefore they are extraneous solutions to our original equation. We found the same set of solutions for θ. 0^(∘)+k * 180^(∘)
We are given the following equation. 2sqrt(2)sin^2θ+ (2-sqrt(2))sin θ = 1 We will first solve the above equation for sin θ. Then, we will find the exact values of θ which solve our equation. Let's do these things one at a time.
We will start by writing all the terms on the left-hand side of the equation. Then, we will solve the obtained equation by factoring and using the Zero Product Property.
Let's solve these equations for θ.
To solve the equation sin θ = 12, let's recall the graph of the sine function. Let's also draw the line y = 12 to see for which values of θ we have sin θ = 12.
We see that the first two positive solutions to the equation are θ = π6 and θ= 5π6. We also see that the solutions repeat every 2π radians. With this information, we can write the general form for all the solutions to the equation sin θ = 12. π/6 + 2π k and 5π/6 + 2π k Here, k is any integer number.
To solve the equation sin θ = - sqrt(2)2, recall the graph of the sine function again. This time we will draw the line y = - sqrt(2)2 to see for which values of θ we have sin θ = - sqrt(2)2.
We see that sin θ = - sqrt(2)2 at θ = 5π4 and at θ = 7π4. We also see that the solutions appear every 2π radians. With this information, we can write the general form for the solutions to our equation. 5π/4 + 2 π k and 7π/4 + 2 π k Here, again, k is any integer number.
While solving equations sin θ =- sqrt(2)2 and sin θ = 12, we have found the following solutions.
2sqrt(2)sin^2θ+ (2-sqrt(2))sin θ = 1 | |
---|---|
sinθ = 1/2 | sinθ = - sqrt(2)/2 |
π/6 + 2 π k and 5π/6 + 2 π k | 5π/4 + 2 π k and 7π/4 + 2 π k |
These are also all the solutions to our original equation.