7.1 solutions to exercises

21
Last edited 11/13/14 7.1 Solutions to Exercises 1. Dividing both sides by 2, we have sin = βˆ’ 1 2 . Since sin is negative only in quadrants III and IV, using our knowledge of special angles, = 7 6 or = 11 6 . 3. Dividing both sides by 2, cos = 1 2 . Using our knowledge of quadrants, this occurs in quadrants I and IV. In quadrant I, = 3 ; in quadrant IV, = 5 3 . 5. Start by dividing both sides by 2 to get sin ( 4 ) = 1 2 . We know that sin = 1 2 for = 6 + 2 and = 5 6 + for any integer . Therefore, 4 = 6 + 2 and 4 = 5 6 + 2. Solving the first equation by multiplying both sides by 4 (the reciprocal of 4 ) and distributing, we get = 4 6 + 8, or = 2 3 + 8. The second equation is solved in exactly the same way to arrive at = 10 3 + 8. 7. Divide both sides by 2 to arrive at cos 2 = βˆ’ √3 2 . Since cos = βˆ’ √3 2 when = 5 6 + 2 and when = 7 6 + 2. Thus, 2 = 5 6 + 2 and 2 = 7 6 + 2. Solving these equations for results in = 5 12 + and = 7 12 + . 9. Divide both sides by 3; then, cos ( 5 ) = 2 3 . Since 2 3 is not the cosine of any special angle we know, we must first determine the angles in the interval [0, 2) that have a cosine of 2 3 . Your calculator will calculate cos βˆ’1 ( 2 3 ) as approximately 0.8411. But remember that, by definition, cos βˆ’1 will always have a value in the interval [0, ] -- and that there will be another angle in (, 2) that has the same cosine value. In this case, 0.8411 is in quadrant I, so the other angle must be in quadrant IV: 2 βˆ’ 0.8411 β‰ˆ 5.4421. Therefore, 5 = 0.8411 + 2 and 5 = 5.442 + 2. Multiplying both sides of both equations by 5 gives us = 1.3387 + 10 and = 8.6612 + 10.

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Page 1: 7.1 Solutions to Exercises

Last edited 11/13/14

7.1 Solutions to Exercises

1. Dividing both sides by 2, we have sin πœƒ = βˆ’1

2. Since sin πœƒ is negative only in quadrants III

and IV, using our knowledge of special angles, πœƒ =7πœ‹

6 or πœƒ =

11πœ‹

6.

3. Dividing both sides by 2, cos πœƒ =1

2. Using our knowledge of quadrants, this occurs in

quadrants I and IV. In quadrant I, πœƒ =πœ‹

3; in quadrant IV, πœƒ =

5πœ‹

3.

5. Start by dividing both sides by 2 to get sin (πœ‹

4π‘₯) =

1

2. We know that sin πœƒ =

1

2 for πœƒ =

πœ‹

6+

2π‘˜πœ‹ and πœƒ =5πœ‹

6+ π‘˜πœ‹ for any integer π‘˜. Therefore,

πœ‹

4π‘₯ =

πœ‹

6+ 2π‘˜πœ‹ and

πœ‹

4π‘₯ =

5πœ‹

6+ 2π‘˜πœ‹. Solving

the first equation by multiplying both sides by 4

πœ‹ (the reciprocal of

πœ‹

4) and distributing, we get

π‘₯ =4

6+ 8π‘˜, or π‘₯ =

2

3+ 8π‘˜. The second equation is solved in exactly the same way to arrive at

π‘₯ =10

3+ 8π‘˜.

7. Divide both sides by 2 to arrive at cos 2𝑑 = βˆ’βˆš3

2. Since cos πœƒ = βˆ’

√3

2 when πœƒ =

5πœ‹

6+ 2π‘˜πœ‹ and

when πœƒ =7πœ‹

6+ 2π‘˜πœ‹. Thus, 2𝑑 =

5πœ‹

6+ 2π‘˜πœ‹ and 2𝑑 =

7πœ‹

6+ 2π‘˜πœ‹. Solving these equations for 𝑑

results in 𝑑 =5πœ‹

12+ π‘˜πœ‹ and 𝑑 =

7πœ‹

12+ π‘˜πœ‹.

9. Divide both sides by 3; then, cos (πœ‹

5π‘₯) =

2

3. Since

2

3 is not the cosine of any special angle we

know, we must first determine the angles in the interval [0, 2πœ‹) that have a cosine of 2

3. Your

calculator will calculate cosβˆ’1 (2

3) as approximately 0.8411. But remember that, by definition,

cosβˆ’1 πœƒ will always have a value in the interval [0, πœ‹] -- and that there will be another angle in

(πœ‹, 2πœ‹) that has the same cosine value. In this case, 0.8411 is in quadrant I, so the other angle

must be in quadrant IV: 2πœ‹ βˆ’ 0.8411 β‰ˆ 5.4421. Therefore, πœ‹

5π‘₯ = 0.8411 + 2π‘˜πœ‹ and

πœ‹

5π‘₯ =

5.442 + 2π‘˜πœ‹. Multiplying both sides of both equations by 5

πœ‹ gives us π‘₯ = 1.3387 + 10π‘˜ and

π‘₯ = 8.6612 + 10π‘˜.

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11. Divide both sides by 7: sin 3𝑑 = βˆ’2

7. We need to know the values of πœƒ that give us sin πœƒ =

βˆ’2

7. Your calculator provides one answer: sinβˆ’1 (βˆ’

2

7) β‰ˆ βˆ’0.2898. However, sinβˆ’1 πœƒ has a

range of [βˆ’πœ‹

2,

πœ‹

2], which only covers quadrants I and IV. There is another angle in the interval

(πœ‹

2,

3πœ‹

2) with the same sine value; in this case, in quadrant III: πœ‹ + 0.2898 β‰ˆ 3.4314. Therefore,

3𝑑 = βˆ’0.2898 + 2π‘˜πœ‹ and 3𝑑 = 3.4314 + 2π‘˜πœ‹. Dividing both sides of both equations by 3 gives

us 𝑑 = 1.1438 +2πœ‹

3π‘˜ and 𝑑 = βˆ’0.0966 +

2πœ‹

3π‘˜.

13. Resist the urge to divide both sides by cos π‘₯ -- although you can do this, you then have to

separately consider the case where cos π‘₯ = 0. Instead, regroup all expressions onto one side of

the equation:

10 sin π‘₯ cos π‘₯ βˆ’ 6 cos π‘₯ = 0

Now factor cos π‘₯:

cos π‘₯ (10 sin π‘₯ βˆ’ 6) = 0

So either cos π‘₯ = 0 or 10 sin π‘₯ βˆ’ 6 = 0. On the interval [0, 2πœ‹), cos π‘₯ = 0 at π‘₯ =πœ‹

2 and π‘₯ =

3πœ‹

2,

which provides us with two solutions. If 10 sin π‘₯ βˆ’ 6 = 0, then 10 sin π‘₯ = 6 and sin π‘₯ =6

10.

Using a calculator or computer to calculate sinβˆ’1 6

10 gives us approximately 0.644, which is in

quadrant I. We know there is another value for π‘₯ in the interval [0, 2πœ‹): in quadrant II at

πœ‹ βˆ’ 0.644 β‰ˆ 2.498. Our solutions are πœ‹

2,

3πœ‹

2, 0.644 and 2.498.

15. Add 9 to both sides to get csc 2π‘₯ = 9. If we rewrite this as 1

sin 2π‘₯= 9, we have 9 sin 2π‘₯ = 1

and sin 2π‘₯ =1

9. sin πœƒ =

1

9 at πœƒ β‰ˆ 0.1113 (the value from a calculator) and πœƒ β‰ˆ 3.0303 (using the

reference angle in quadrant II). Therefore, 2π‘₯ = 0.1113 + 2π‘˜πœ‹ and 2π‘₯ = 3.0303 + 2π‘˜πœ‹.

Solving these equations gives us π‘₯ = 0.056 + π‘˜πœ‹ and π‘₯ = 1.515 + π‘˜πœ‹ for integral π‘˜. We choose

π‘˜ = 0 and π‘˜ = 1 for both equations to get four values: 0.056, 1.515, 3.198 and 4.657; these are

the only values that lie in the interval [0, 2πœ‹).

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17. Factoring sin π‘₯, we get sin π‘₯ (sec π‘₯ βˆ’ 2) = 0. Therefore, either sin π‘₯ = 0 or sec π‘₯ βˆ’ 2 = 0.

On the interval [0, 2πœ‹), sin π‘₯ = 0 at π‘₯ = 0 and π‘₯ = πœ‹, so these are our first two answers.

If sec π‘₯ βˆ’ 2 = 0, then sec π‘₯ = 2 and 1

cos π‘₯= 2. This leads us to 2 cos π‘₯ = 1 and cos π‘₯ =

1

2.

Recognizing this as a well-known angle, we conclude that (again, on the interval [0, 2πœ‹)), π‘₯ =πœ‹

3

and π‘₯ =5πœ‹

3.

19. If sin2(π‘₯) =1

4, then sin π‘₯ = Β±

1

2. On the interval [0, 2πœ‹), this occurs at π‘₯ =

πœ‹

6, π‘₯ =

5πœ‹

6,

π‘₯ =7πœ‹

6 and π‘₯ =

11πœ‹

6.

21. If sec2 π‘₯ = 7, then sec π‘₯ = ±√7, 1

cos π‘₯= ±√7, and cos π‘₯ = Β±

1

√7= ±

√7

7.

Using a calculator for cosβˆ’1 (√7

7), we get π‘₯ β‰ˆ 1.183. There is another angle on the interval

[0, 2πœ‹) whose cosine is 1

7, in quadrant IV: π‘₯ = 2πœ‹ βˆ’ 1.183 β‰ˆ 5.1. The two angles where

cos π‘₯ = βˆ’βˆš7

7 must lie in quadrants III and IV at π‘₯ = πœ‹ βˆ’ 1.183 β‰ˆ 1.959 and π‘₯ = πœ‹ + 1.183 β‰ˆ

4.325.

23. This is quadratic in sin 𝑀: think of it as 2π‘₯2 + 3π‘₯ + 1 = 0, where π‘₯ = sin 𝑀. This is simple

enough to factor:

2π‘₯2 + 3π‘₯ + 1 = (2π‘₯ + 1)(π‘₯ + 1) = 0

This means that either 2π‘₯ + 1 = 0 and π‘₯ = βˆ’1

2, or π‘₯ + 1 = 0 and π‘₯ = βˆ’1. Therefore, either

sin 𝑀 = βˆ’1

2 or sin 𝑀 = βˆ’1. We know these special angles: these occur on the interval [0, 2πœ‹)

when 𝑀 =7πœ‹

6 or 𝑀 =

11πœ‹

6 (for sin 𝑀 = βˆ’

1

2) or when 𝑀 =

3πœ‹

2 (for sin 𝑀 = βˆ’1).

25. If we subtract 1 from both sides, we can see that this is quadratic in cos 𝑑:

2(cos2 𝑑 + cos 𝑑 βˆ’ 1 = 0

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If we let π‘₯ = cos 𝑑, we have:

2π‘₯2 + π‘₯ βˆ’ 1 = (2π‘₯ βˆ’ 1)(π‘₯ + 1) = 0

Either 2π‘₯ βˆ’ 1 = 0 and π‘₯ =1

2, or π‘₯ + 1 = 0 and π‘₯ = βˆ’1. Therefore, cos 𝑑 =

1

2 or cos 𝑑 = βˆ’1. On

the interval [0, 2πœ‹), these are true when 𝑑 =πœ‹

3 or 𝑑 =

5πœ‹

3 (for cos 𝑑 =

1

2) or when 𝑑 = πœ‹ (for

cos 𝑑 = βˆ’1).

27. If we rearrange the equation, it is quadratic in cos π‘₯:

4 cos2 π‘₯ βˆ’ 15 cos π‘₯ βˆ’ 4 = 0

If we let 𝑒 = cos π‘₯, we can write this as:

4𝑒2 βˆ’ 15𝑒 βˆ’ 4 = 0

This factors as:

(4𝑒 + 1)(𝑒 βˆ’ 4) = 0

Therefore, either 4𝑒 + 1 = 0 and 𝑒 = βˆ’1

4, or 𝑒 βˆ’ 4 = 0 and 𝑒 = 4. Substituting back, we have:

cos π‘₯ = βˆ’1

4

We reject the other possibility that cos π‘₯ = 4 since cos π‘₯ is always in the interval [βˆ’1, 1].

Your calculator will tell you that cosβˆ’1 (βˆ’1

4) β‰ˆ 1.823. This is in quadrant II, and the cosine is

negative, so the other value must lie in quadrant III. The reference angle is πœ‹ βˆ’ 1.823, so the

other angle is at πœ‹ + (πœ‹ βˆ’ 1.823) = 2πœ‹ βˆ’ 1.823 β‰ˆ 4.460.

29. If we substitute 1 βˆ’ cos2 𝑑 for sin2 𝑑, we can see that this is quadratic in cos 𝑑:

12 sin2 𝑑 + cos 𝑑 βˆ’ 6 = 12(1 βˆ’ cos2 𝑑) + cos 𝑑 βˆ’ 6 = βˆ’12 cos2 𝑑 + cos 𝑑 + 6 = 0

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Setting 𝑒 = cos 𝑑:

βˆ’12𝑒2 + 𝑒 + 6 = (βˆ’4𝑒 + 3)(3𝑒 + 2) = 0

This leads us to βˆ’4𝑒 + 3 = 0 or 3𝑒 + 2 = 0, so either 𝑒 =3

4 or 𝑒 = βˆ’

2

3.

Substituting back, cos 𝑑 =3

4 gives us (via a calculator) 𝑑 β‰ˆ 0.7227. This is in quadrant I, so the

corresponding angle must lie in quadrant IV at 𝑑 = 2πœ‹ βˆ’ 0.7227 β‰ˆ 5.5605.

Similarly, cos 𝑑 = βˆ’2

3 gives us 𝑑 β‰ˆ 2.3005. This is in quadrant II; the corresponding angle with

the same cosine value must be in quadrant III at 𝑑 = 2πœ‹ βˆ’ 2.3005 β‰ˆ 3.9827.

31. Substitute 1 βˆ’ sin2 πœ™ for cos2 πœ™:

1 βˆ’ sin2 πœ™ = βˆ’6 sin πœ™

βˆ’ sin2 πœ™ + 6 sin πœ™ + 1 = 0

This is quadratic in sin πœ™, so set 𝑒 = sin πœ™ and we have:

βˆ’π‘’2 + 6𝑒 + 1 = 0

This does not factor easily, but the quadratic equation gives us:

𝑒 =βˆ’6 Β± √36 βˆ’ 4(βˆ’1)(1)

2(βˆ’1)=

βˆ’6 Β± √40

βˆ’2=

βˆ’6 Β± 2√10

βˆ’2= 3 Β± √10

Thus, 𝑒 β‰ˆ 6.1623 and 𝑒 β‰ˆ βˆ’0.1623. Substituting back, we have sin πœ™ = βˆ’0.1623. We reject

sin πœ™ = 6.1623 since sin πœ™ is always between -1 and 1. Using a calculator to calculate

sinβˆ’1(βˆ’0.1623), we get πœ™ β‰ˆ βˆ’.1630. Unfortunately, this is not in the required interval [0, 2πœ‹),

so we add 2πœ‹ to get πœ™ β‰ˆ 6.1202. This is in quadrant IV; the corresponding angle with the same

sine value must be in quadrant III at πœ‹ + 0.1630 β‰ˆ 3.3046.

33. If we immediately substitute 𝑣 = tan π‘₯, we can write:

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𝑣3 = 3𝑣

𝑣3 βˆ’ 3𝑣 = 0

𝑣(𝑣2 βˆ’ 3) = 0

Thus, either 𝑣 = 0 or 𝑣2 βˆ’ 3 = 0, meaning 𝑣2 = 3 and 𝑣 = ±√3.

Substituting back, tan π‘₯ = 0 at π‘₯ = 0 and π‘₯ = πœ‹. Similarly, tan π‘₯ = √3 at π‘₯ =πœ‹

3 and π‘₯ =

4πœ‹

3 and

tan π‘₯ = βˆ’βˆš3 at π‘₯ =2πœ‹

3 and π‘₯ =

5πœ‹

3.

35. Substitute 𝑣 = tan π‘₯ so that:

𝑣5 = 𝑣

𝑣5 βˆ’ 𝑣 = 0

𝑣(𝑣4 βˆ’ 1) = 0

Either 𝑣 = 0 or 𝑣4 βˆ’ 1 = 0 and 𝑣4 = 1 and 𝑣 = Β±1. Substituting back, tan π‘₯ = 0 at π‘₯ = 0 and

π‘₯ = πœ‹. Similarly, tan π‘₯ = 1 at π‘₯ =πœ‹

4 and π‘₯ =

5πœ‹

4. Finally, tan π‘₯ = βˆ’1 for π‘₯ =

3πœ‹

4 and π‘₯ =

7πœ‹

4.

37. The structure of the equation is not immediately apparent.

Substitute 𝑒 = sin π‘₯ and 𝑣 = cos π‘₯, and we have:

4𝑒𝑣 + 2𝑒 βˆ’ 2𝑣 βˆ’ 1 = 0

The structure is now reminiscent of the result of multiplying two binomials in different variables.

For example, (π‘₯ + 1)(𝑦 + 1) = π‘₯𝑦 + π‘₯ + 𝑦 + 1. In fact, our equation factors as:

(2𝑒 βˆ’ 1)(2𝑣 + 1) = 0

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Therefore, either 2𝑒 βˆ’ 1 = 0 (and 𝑒 =1

2) or 2𝑣 + 1 = 0 (and 𝑣 = βˆ’

1

2). Substituting back,

sin π‘₯ =1

2 or cos π‘₯ = βˆ’

1

2. This leads to π‘₯ =

πœ‹

6, π‘₯ =

5πœ‹

6 (for sin π‘₯ =

1

2) and π‘₯ =

2πœ‹

3, π‘₯ =

4πœ‹

3 (for

cos π‘₯ = βˆ’1

2

39. Rewrite tan π‘₯ as sin π‘₯

cos π‘₯ to give:

sin π‘₯

cos π‘₯βˆ’ 3 sin π‘₯ = 0

Using a common denominator of cos π‘₯, we have:

sin π‘₯

cos π‘₯βˆ’

3 sin π‘₯ cos π‘₯

cos π‘₯= 0

and

sin π‘₯ βˆ’ 3 sin π‘₯ cos π‘₯

cos π‘₯= 0

sin π‘₯ βˆ’ 3 sin π‘₯ cos π‘₯ = 0

sin π‘₯ (1 βˆ’ 3 cos π‘₯) = 0

Therefore, either sin π‘₯ = 0 or 1 βˆ’ 3 cos π‘₯ = 0, which means cos π‘₯ =1

3.

For sin π‘₯ = 0, we have π‘₯ = 0 and π‘₯ = πœ‹ on the interval [0, 2πœ‹). For cos π‘₯ =1

3, we need

cosβˆ’1 (1

3), which a calculator will indicate is approximately 1.231. This is in quadrant I, so the

corresponding angle with a cosine of 1

3 is in quadrant IV at 2πœ‹ βˆ’ 1.231 β‰ˆ 5.052.

41. Rewrite both tan 𝑑 and sec 𝑑 in terms of sin 𝑑 and cos 𝑑:

2sin2 𝑑

cos2 𝑑= 3

1

cos 𝑑

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We can multiply both sides by cos2 𝑑:

2 sin2 𝑑 = 3 cos 𝑑

Now, substitute 1 βˆ’ cos2 𝑑 for sin2 𝑑 to yield:

2(1 βˆ’ cos2 𝑑) βˆ’ 3 cos 𝑑 = 0

This is beginning to look quadratic in cos 𝑑. Distributing and rearranging, we get:

βˆ’2 cos2 𝑑 βˆ’ 3 cos 𝑑 + 2 = 0

Substitute 𝑒 = cos 𝑑:

βˆ’2𝑒2 βˆ’ 3𝑒 + 2 = 0

(βˆ’2𝑒 + 1)(𝑒 + 2) = 0

Therefore, either βˆ’2𝑒 + 1 = 0 (and 𝑒 =1

2) or 𝑒 + 2 = 0 (and 𝑒 = βˆ’2). Since 𝑒 = cos 𝑑 will

never have a value of -2, we reject the second solution.

cos 𝑑 =1

2 at 𝑑 =

πœ‹

3 and 𝑑 =

5πœ‹

3 on the interval [0, 2πœ‹).

7.2 Solutions to Exercises

1. sin(75°) = sin(45°+30°) = sin(45°)cos(30°)+cos(45°)sin(30°) = √2

2βˆ™

√3

2+

√2

2βˆ™

1

2=

√6+√2

4

3. cos(165Β°) = cos(120Β° + 45Β°) = cos(120Β°)cos(45Β°)-sin(120Β°)sin(45Β°) = βˆ’(√6+√2)

4

5. cos (7πœ‹

12) = cos (

πœ‹

4+

πœ‹

3) = cos (

πœ‹

4) cos (

πœ‹

3) βˆ’ sin (

πœ‹

4) sin (

πœ‹

3) =

√2βˆ’βˆš6

4

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7. sin (5πœ‹

12) = sin (

πœ‹

6+

πœ‹

4) = sin (

πœ‹

6) cos (

πœ‹

4) + cos (

πœ‹

6) sin (

πœ‹

4) =

√6+√2

4

9. sin (π‘₯ +11πœ‹

6) = sin(π‘₯) cos (

11πœ‹

6) + cos(π‘₯) sin (

11πœ‹

6) =

√3

2sin(π‘₯) βˆ’

1

2cos(π‘₯)

11. cos (π‘₯ βˆ’5πœ‹

6) = cos(π‘₯) cos (

5πœ‹

6) + sin(π‘₯) sin (

5πœ‹

6) = βˆ’

√3

2cos(π‘₯) +

1

2sin(π‘₯)

13. csc (πœ‹

2βˆ’ 𝑑) =

1

sin(πœ‹

2βˆ’π‘‘)

=1

sin(πœ‹

2) cos(𝑑)βˆ’cos(

πœ‹

2) sin(𝑑)

=1

cos(𝑑)= sec(𝑑)

15. cot (πœ‹

2βˆ’ π‘₯) =

cos(πœ‹

2) cos(π‘₯)+sin(

πœ‹

2)sin (π‘₯)

sin(πœ‹

2) cos(𝑑)βˆ’cos(

πœ‹

2) sin(𝑑)

=sin(π‘₯)

cos(π‘₯)= tan(π‘₯)

17. 16 sin(16π‘₯) sin(11π‘₯) = 16 βˆ™1

2(cos(16π‘₯ βˆ’ 11π‘₯) βˆ’ cos(16π‘₯ + 11π‘₯)) = 8 cos(5π‘₯) βˆ’

8 cos(27π‘₯)

19. 2 sin(5π‘₯) cos(3π‘₯) = sin(5π‘₯ + 3π‘₯) + sin(5π‘₯ βˆ’ 3π‘₯) = sin(8π‘₯) + sin(2π‘₯)

21. cos(6𝑑) + cos(4𝑑) = 2 cos (6𝑑+4𝑑

2) cos (

6π‘‘βˆ’4𝑑

2) = 2 cos(5𝑑) cos(𝑑)

23. sin(3π‘₯) + sin(7π‘₯) = 2 sin (3π‘₯+7π‘₯

2) cos (

3π‘₯βˆ’7π‘₯

2) = 2 sin(5π‘₯) cos (βˆ’2π‘₯)

25. We know that sin(π‘Ž) =2

3 and cos(𝑏) = βˆ’

1

4 and that the angles are in quadrant II. We can

find cos (π‘Ž) and sin (𝑏) using the Pythagorean identity sin2(πœƒ) + cos2(πœƒ) = 1, or by using the

known values of sin(π‘Ž) and cos(𝑏) to draw right triangles. Using the latter method: we know

two sides of both a right triangle including angle a and a right triangle including angle b. The

triangle including angle a has a hypotenuse of 3 and an opposite side of 2. We may use the

pythagorean theorem to find the side adjacent to angle a. Using the same method we may find

the side opposite to b.

For the triangle containing angle a:

Adjacent = √32 βˆ’ 22 = √5

However, this side lies in quadrant II, so it will be βˆ’βˆš5.

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For the triangle containing angle b:

Opposite = √42 βˆ’ 12 = √15

In quadrant II, y is positive, so we do not need to change the sign.

From this, we know: sin(π‘Ž) =2

3, cos(π‘Ž) = βˆ’

√5

3, cos(𝑏) = βˆ’

1

4, sin(𝑏) =

√15

4.

a. sin(π‘Ž + 𝑏) = sin(π‘Ž) cos(𝑏) + cos(π‘Ž) sin(𝑏) =βˆ’2βˆ’5√3

12

b. cos(π‘Ž βˆ’ 𝑏) = cos(π‘Ž) cos(𝑏) + sin(π‘Ž) sin(𝑏) =√5+2√15

12

27. sin(3π‘₯) cos(6π‘₯) βˆ’ cos(3π‘₯) sin(6π‘₯) = βˆ’0.9

sin(3π‘₯ βˆ’ 6π‘₯) = βˆ’0.9

sin(βˆ’3π‘₯) = βˆ’0.9

βˆ’sin(3π‘₯) = βˆ’0.9

3π‘₯ = sinβˆ’1(0.9) + 2πœ‹π‘˜ or 3π‘₯ = πœ‹ βˆ’ sinβˆ’1(0.9) + 2πœ‹π‘˜, where k is an integer

π‘₯ =sinβˆ’1(0.9)+2πœ‹π‘˜

3 or π‘₯ =

πœ‹βˆ’sinβˆ’1(0.9)+2πœ‹π‘˜

3

π‘₯ β‰ˆ 0.373 +2πœ‹

3π‘˜ or π‘₯ β‰ˆ 0.674 +

2πœ‹

3π‘˜, where k is an integer

29. cos(2π‘₯) cos(π‘₯) + sin(2π‘₯) sin(π‘₯) = 1

cos(2π‘₯ βˆ’ π‘₯) = 1

π‘₯ = 0 + 2πœ‹π‘˜, where k is an integer

31. cos(5π‘₯) = βˆ’cos (2π‘₯)

cos(5π‘₯) + cos(2π‘₯) = 0

2 cos (5π‘₯+2π‘₯

2) cos (

5π‘₯βˆ’2π‘₯

2) = 0

cos (7π‘₯

2) = 0 or cos (

3π‘₯

2) = 0

7π‘₯

2=

πœ‹

2+ πœ‹π‘˜ or

3π‘₯

2=

πœ‹

2+ πœ‹π‘˜, where k is an integer

π‘₯ =πœ‹+2πœ‹π‘˜

7 or π‘₯ =

πœ‹+2πœ‹π‘˜

3

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33. cos(6πœƒ) βˆ’ cos(2πœƒ) = sin(4πœƒ)

βˆ’2 sin (6πœƒ+2πœƒ

2) sin (

6πœƒβˆ’2πœƒ

2) = sin(4πœƒ)

βˆ’2 sin(4πœƒ) sin(2πœƒ) βˆ’ sin(4πœƒ) = 0

sin(4πœƒ) (βˆ’2 sin(2πœƒ) βˆ’ 1) = 0

sin(4πœƒ) = 0 or βˆ’2 sin(2πœƒ) βˆ’ 1 = 0

sin(4πœƒ) = 0 or sin(2πœƒ) = βˆ’1

2

4πœƒ = πœ‹π‘˜ or 2πœƒ =7πœ‹

6+ 2πœ‹π‘˜ or

11πœ‹

6+ 2πœ‹π‘˜

πœƒ =πœ‹π‘˜

4 or

7πœ‹

12+ πœ‹π‘˜ or

11πœ‹

12+ πœ‹π‘˜

35. 𝐴 = √42 + 62 = 2√13

cos(𝑐) =2

√13, sin(𝑐) = βˆ’

3

√13

Since sin(C) is negative but cos(C) is positive, we know that C is in quadrant IV.

𝐢 = sinβˆ’1 (βˆ’3

√13)

Therefore the expression can be written as 2√13 sin (π‘₯ + sinβˆ’1 (βˆ’3

√13)) or approximately

2√13 sin(π‘₯ βˆ’ 0.9828).

37. 𝐴 = √52 + 22 = √29

cos(𝐢) =5

√29, sin(𝐢) =

2

√29

Since both sin(C) and cos(C) are positive, we know that C is in quadrant I.

𝐢 = sinβˆ’1 (2

√29)

Therefore the expression can be written as √29 sin (3π‘₯ + sinβˆ’1 (2

√29)) or approximately

√29 sin(3π‘₯ + 0.3805).

39. This will be easier to solve if we combine the 2 trig terms into one sinusoidal function of the

form 𝐴sin(𝐡π‘₯ + 𝐢).

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𝐴 = √52 + 32 = √34, cos(𝐢) = βˆ’5

√34, sin(𝐢) =

3

√34

C is in quadrant II, so 𝐢 = πœ‹ βˆ’ sinβˆ’1 (3

√34)

Then:

√34 sin (π‘₯ + πœ‹ βˆ’ sinβˆ’1 (3

√34)) = 1

βˆ’ sin (π‘₯ βˆ’ sinβˆ’1 (3

√34)) =

1

√34 (Since sin(π‘₯ + πœ‹) = βˆ’sin (π‘₯))

π‘₯ βˆ’ sinβˆ’1 (3

√34) = sinβˆ’1 (βˆ’

1

√34) or, to get the second solution π‘₯ βˆ’ sinβˆ’1 (

3

√34) = πœ‹ βˆ’

sinβˆ’1 (βˆ’1

√34)

π‘₯ β‰ˆ 0.3681 or π‘₯ β‰ˆ 3.8544 are the first two solutions.

41. This will be easier to solve if we combine the 2 trig terms into one sinusoidal function of the

form 𝐴sin(𝐡π‘₯ + 𝐢).

𝐴 = √52 + 32 = √34, cos(𝐢) =3

√34, sin(𝐢) = βˆ’

5

√34

C is in quadrant IV, so 𝐢 = sinβˆ’1 (βˆ’5

√34).

Then:

√34 sin (2π‘₯ + sinβˆ’1 (βˆ’5

√34)) = 3

sin (2π‘₯ + sinβˆ’1 (βˆ’5

√34)) =

3

√34

2π‘₯ + sinβˆ’1 (βˆ’5

√34) = sinβˆ’1 (

3

√34) and 2π‘₯ + sinβˆ’1 (βˆ’

5

√34) = πœ‹ βˆ’ sinβˆ’1 (

3

√34)

π‘₯ =

sinβˆ’1(3

√34)βˆ’sinβˆ’1(βˆ’

5

√34)

2 or

πœ‹βˆ’sinβˆ’1(3

√34)βˆ’sinβˆ’1(βˆ’

5

√34)

2.

43. sin(7𝑑)+sin (5𝑑)

cos(7𝑑)+cos(5𝑑)=

2 sin(7𝑑+5𝑑

2) cos(

7π‘‘βˆ’5𝑑

2)

2 cos(7𝑑+5𝑑

2) cos(

7π‘‘βˆ’5𝑑

2)

=2 sin(6𝑑)cos (𝑑)

2 cos(6𝑑)cos (𝑑) = tan(6𝑑)

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45. tan (πœ‹

4βˆ’ 𝑑) =

sin(πœ‹

4βˆ’π‘‘)

cos(πœ‹

4βˆ’π‘‘)

=sin(

πœ‹

4) cos(𝑑)βˆ’cos(

πœ‹

4) sin(𝑑)

cos(πœ‹

4) cos(𝑑)+sin(

πœ‹

4) sin(𝑑)

=√2

2(cos(𝑑)βˆ’sin(𝑑))

√2

2(cos(𝑑)+sin(𝑑))

=(cos(𝑑))(1βˆ’

sin(𝑑)

cos(𝑑))

(cos(𝑑))(1+sin(𝑑)

cos(𝑑))

=1βˆ’tan(𝑑)

1+tan(𝑑)

47. cos(π‘Ž+𝑏)

cos(π‘Žβˆ’π‘)=

cos(π‘Ž) cos(𝑏)βˆ’sin(π‘Ž) sin(𝑏)

cos(π‘Ž) cos(𝑏)+sin(π‘Ž) sin(𝑏)

=cos(π‘Ž) cos(𝑏)(1βˆ’

sin(π‘Ž) sin(𝑏)

cos(π‘Ž) cos(𝑏))

cos(π‘Ž) cos(𝑏)(1+sin(π‘Ž) sin(𝑏)

cos(π‘Ž) cos(𝑏))

=1βˆ’tan(π‘Ž) tan(𝑏)

1+tan(π‘Ž) tan(𝑏)

49. Using the Product-to-Sum identity:

2 sin(π‘Ž + 𝑏) sin(π‘Ž βˆ’ 𝑏) = 2 (1

2) cos((π‘Ž + 𝑏) βˆ’ (π‘Ž βˆ’ 𝑏)) βˆ’ cos((π‘Ž + 𝑏) + (π‘Ž βˆ’ 𝑏))

= cos(2𝑏) βˆ’ cos(2π‘Ž)

51. cos(π‘Ž+𝑏)

cos(π‘Ž)cos (𝑏)=

cos(π‘Ž) cos(𝑏)βˆ’sin(π‘Ž) sin(𝑏)

cos(π‘Ž) cos(𝑏)

=cos(π‘Ž) cos(𝑏)

cos(π‘Ž) cos(𝑏)βˆ’

sin(π‘Ž) sin(𝑏)

cos(π‘Ž) cos(𝑏)

= 1 βˆ’ tan(π‘Ž) tan(𝑏)

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7.3 Solutions to Exercises

1. a. sin(2π‘₯) = 2 sin π‘₯ cos π‘₯

To find cos π‘₯:

sin2 π‘₯ + cos2 π‘₯ = 1

cos2 π‘₯ = 1 βˆ’1

64=

63

64

cos π‘₯ = ±√63

64 Note that we need the positive root since we are told π‘₯ is in quadrant 1.

cos π‘₯ =3√7

8

So: sin(2π‘₯) = 2 (1

8) (

3√7

8) =

3√7

32

b. cos(2π‘₯) = 2 cos2 π‘₯ βˆ’ 1

= (2 (63

64)) βˆ’ 1 =

63βˆ’32

32=

31

32

c. tan(2π‘₯) =sin(2π‘₯)

cos(2π‘₯)=

3√7

32

31

32⁄ =

3√7

31

3. cos2 π‘₯ – sin2 π‘₯ = cos(2π‘₯), so cos2(28Β°) – sin2(28Β°) = cos(56Β°)

5. 1 βˆ’ 2 sin2(π‘₯) = cos(2π‘₯), so 1 – 2sin2(17Β°) = cos(2 (17Β°)) = cos(34Β°)

7. cos2(9π‘₯) – sin2(9π‘₯) = cos(2(9π‘₯)) = cos(18π‘₯)

9. 4 sin(8π‘₯) cos(8π‘₯) = 2 (2sin(8π‘₯) cos(8π‘₯)) = 2 sin(16π‘₯)

11. 6 sin(2𝑑) + 9 sin 𝑑 = 6 βˆ™ 2 sin 𝑑 cos 𝑑 + 9 sin 𝑑 = 3 sin 𝑑 (4 cos 𝑑 + 3), so we can solve

3 sin 𝑑 (4 cos 𝑑 + 3) = 0:

sin 𝑑 = 0 or cos 𝑑 = βˆ’3/4

𝑑 = 0, πœ‹ or 𝑑 β‰ˆ 2.4186, 3.8643.

13. 9cos (2πœƒ) = 9 cos2 πœƒ βˆ’ 4

9(cos2 πœƒ- sin2πœƒ)

= 9 cos2 πœƒ βˆ’ 4

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9 sin2 πœƒ βˆ’ 4 = 0

(3 sin πœƒ βˆ’ 2)(3 sin πœƒ + 2) = 0

sin πœƒ =2

3,-

2

3

πœƒ = sinβˆ’1 2

3, sinβˆ’1 βˆ’2

3

πœƒ β‰ˆ 0.7297, 2.4119, 3.8713, 5.5535

15. sin(2𝑑) = cos 𝑑

2 sin 𝑑 cos 𝑑 = cos 𝑑

2 sin 𝑑 cos 𝑑 βˆ’ cos 𝑑 = 0

cos 𝑑 (2 sin 𝑑 βˆ’ 1) = 0

cos 𝑑 = 0 or 2 sin 𝑑 βˆ’ 1 = 0

If cos 𝑑 = 0, then 𝑑 =πœ‹

2 or

3πœ‹

2. If 2 sin 𝑑 βˆ’ 1 = 0, then sin 𝑑 =

1

2, so 𝑑 =

πœ‹

6 or

5πœ‹

6. So 𝑑 =

πœ‹

2,

3πœ‹

2,

πœ‹

6

or 5πœ‹

6.

17. cos(6π‘₯) βˆ’ cos(3π‘₯) = 0

2 cos2(3π‘₯) βˆ’ 1 βˆ’ cos(3π‘₯) = 0

2 cos2(3π‘₯) βˆ’ cos(3π‘₯) βˆ’ 1 = 0

(2 cos(3π‘₯) + 1)(cos(3π‘₯) βˆ’ 1) = 0

cos(3π‘₯) = βˆ’1

2 or 1

Since we need solutions for π‘₯ in the interval [0, 2πœ‹), we will look for all solutions for 3π‘₯ in the

interval [0, 6πœ‹). If cos(3π‘₯) = βˆ’1

2, then there are two possible sets of solutions. First, 3π‘₯ =

2πœ‹

3+ 2πœ‹π‘˜ where π‘˜ = 0, 1, or 2, so π‘₯ =

2πœ‹

9+

2πœ‹π‘˜

3 where π‘˜ = 0, 1, or 2. Second, 3π‘₯ =

4πœ‹

3+

2πœ‹π‘˜ where π‘˜ = 0, 1, or 2, so π‘₯ =4πœ‹

9+

2πœ‹π‘˜

3 where π‘˜ = 0, 1, or 2 If cos(3π‘₯) = 1, then 3π‘₯ =

2πœ‹π‘˜ where π‘˜ = 0, 1, or 2, so π‘₯ =2πœ‹π‘˜

3 where π‘˜ = 0, 1, or 2.

19. cos2(5π‘₯) =cos(10π‘₯)+1

2 because cos2 π‘₯ =

cos(2π‘₯)+1

2 (power reduction identity)

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21. sin4(8π‘₯) = sin2(8π‘₯) βˆ™ sin2(8π‘₯)

= (1βˆ’cos(16π‘₯))

2 .

(1βˆ’cos(16π‘₯))

2 (because power reduction identity sin

2 x =

(1βˆ’cos(2π‘₯))

2

= 1βˆ’2 cos(16π‘₯)

4+

cos2(16π‘₯)

4

= 1βˆ’2 cos(16π‘₯)

4+

cos(32π‘₯)+1

8 because cos2 π‘₯ =

cos(2π‘₯)+1

2 (power reduction identity)

= 1

4 –

cos (16π‘₯)

2 +

cos (32π‘₯)

8 +

1

8

23. cos2 π‘₯ sin4 π‘₯

= cos2 π‘₯ βˆ™ sin2 π‘₯ βˆ™ sin2 π‘₯

= 1+cos(2π‘₯)

2βˆ™

1βˆ’cos (2π‘₯)

2βˆ™

1βˆ’cos(2π‘₯))

2

= 1βˆ’cos2(2π‘₯)

4βˆ™

1βˆ’cos(2π‘₯)

2

= 1βˆ’

cos(4π‘₯)+1

2

4βˆ™

1βˆ’cos (2π‘₯)

2

=1βˆ’cos(4π‘₯)

8βˆ™

1βˆ’cos (2π‘₯)

2

=1βˆ’cos(2π‘₯)βˆ’cos(4π‘₯)+cos(2π‘₯)cos (4π‘₯)

16

25. Since csc π‘₯ = 7 and π‘₯ is in quadrant 2, sin π‘₯ =1

7 (reciprocal of cosecant) and cos π‘₯ = βˆ’

4√3

7

(Pythagorean identity).

a. sinπ‘₯

2= √

(1βˆ’cos (π‘₯))

2 =√7+4√3

14 (Note that the answer is positive because π‘₯ is in quadrant 2, so

π‘₯

2

is in quadrant 1.)

b. cos(π‘₯

2) =√

(cos π‘₯+1)

2 =√7βˆ’4√3

14 (Note that the answer is positive because π‘₯ is in quadrant 2, so

π‘₯

2

is in quadrant 1.)

c. tan (π‘₯

2)=

sin(π‘₯

2)

cos(π‘₯

2)

= √7+4√3

7βˆ’4√3= √ (7+4√3)

2

(7βˆ’4√3)(7+4√3)= √(7+4√3)

2

1= 7 + 4√3

27. (sin 𝑑 βˆ’ cos 𝑑)2 = 1 βˆ’ sin(2𝑑)

Left side: (sin2 𝑑 βˆ’ 2 sin 𝑑 cos 𝑑 + cos2 𝑑)

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= 1 – 2 sin 𝑑 cos 𝑑 (because (sin2 𝑑 + cos2 𝑑 = 1)

= 1 βˆ’ sin(2𝑑), the right side (because sin(2𝑑) = 2 sin 𝑑 cos 𝑑)

29. sin(2π‘₯) =2tan (π‘₯)

1+tan2(π‘₯)

The right side:

2sin (π‘₯)

cos(π‘₯)

1+sin2 π‘₯

cos2 π‘₯

βˆ™cos2(π‘₯)

cos2(π‘₯)=

2 sin(π‘₯) cos(π‘₯)

cos2(π‘₯)+sin2(π‘₯) = 2 sin π‘₯ cos π‘₯ = sin(2π‘₯), the left side.

31. cot π‘₯ βˆ’ tan π‘₯ = 2 cot(2π‘₯)

The left side: cos (π‘₯)

sin (π‘₯) –

sin (π‘₯)

cos (π‘₯)

= cos2 π‘₯βˆ’sin2 π‘₯

sin(π‘₯) cos(π‘₯) =

cos(2π‘₯)sin(2π‘₯)

2

=2 cot(2π‘₯)

33. cos(2𝛼) =1βˆ’tan2(𝛼)

1+tan2(𝛼)

The left side: 1βˆ’tan2(𝛼)

1+tan2(𝛼) =

cos2 π›Όβˆ’sin2 𝛼

cos2 𝛼cos2 𝛼+sin2 𝛼

cos2 𝛼

=cos(2𝛼)

cos2 𝛼1

cos2 𝛼

= cos(2𝛼)

35. sin(3π‘₯) = 3sin(x) cos2 π‘₯ βˆ’ sin3 π‘₯

Left side: sin(π‘₯ + 2π‘₯) = sin(π‘₯) cos(2π‘₯) + cos(π‘₯) sin(2π‘₯) addition rule.

= sin(π‘₯) (cos2(π‘₯) – sin2(π‘₯)) + cos(π‘₯) (2 sin(π‘₯) cos(π‘₯))

= cos2(π‘₯) sin(x) – sin3(π‘₯) + 2 cos2(π‘₯) sin(π‘₯)

= 3 cos2(π‘₯) sin(x) βˆ’ sin3(π‘₯)

7.4 Solutions to Exercises

1. By analysis, the function has a period of 12 units. The frequency is 1/12 Hz. The average of

the y-values from 0 ≀ x < 12 is -1, and since the terms repeat identically there is no change in the

midline over time. Therefore the midline is y = f(x) = -1. The high point (y = 2) and low point (y

= -4) are both 3 units away from the midline. Therefore, amplitude = 3 units. The function also

starts at a minimum, which means that its phase must be shifted by one quarter of a cycle, or 3

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units, to the right. Therefore, phase shift = 3.

Now insert known values into the function:

𝑦 = 𝐴sin ((2πœ‹

period) (π‘₯ βˆ’ (phase shift))) + midline

𝑦 = 3sin (2πœ‹

12(π‘₯ βˆ’ 3)) βˆ’ 1

This can be reduced to 𝑦 = 3sin (πœ‹

6(π‘₯ βˆ’ 3)) βˆ’ 1

Alternatively, had we chosen to use the cosine function: 𝑦 = βˆ’3 cos (πœ‹

6π‘₯) βˆ’ 1.

3. By analysis of the function, we determine:

A = amplitude = 8 units

Solving 2πœ‹

period= 6πœ‹, we get: period = 1/3 seconds

Frequency = 3 Hz

5. In this problem, it is assumed that population increases linearly. Using the starting average as

well as the given rate, the average population is then y(x) = 650 + (160/12)x = 650 + (40/3)x ,

where x is measured as the number of months since January.

Based on the problem statement, we know that the period of the function must be twelve months

with an amplitude of 19. Since the function starts at a low-point, we can model it with a cosine

function since -[cos(0)] = -1

Since the period is twelve months, the factor inside the cosine operator is equal to 2πœ‹

12=

πœ‹

6. Thus,

the cosine function is βˆ’19 cos (πœ‹

6π‘₯).

Therefore, our equation is: 𝑦 = 𝑓(π‘₯) = 650 +40

3π‘₯ βˆ’ 19 cos (

πœ‹

6π‘₯)

7. By analysis of the problem statement, the amplitude of the sinusoidal component is 33 units

with a period of 12 months. Since the sinusoidal component starts at a minimum, its phase must

be shifted by one quarter of a cycle, or 3 months, to the right.

𝑦 = 𝑔(π‘₯) = 33 sin (πœ‹

6(π‘₯ βˆ’ 3))

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Using the starting average as well as the given rate, the average population is then:

𝑦 = 𝑓(π‘₯) = 900(1.07)π‘₯

𝑔(π‘₯) + 𝑓(π‘₯) = 33 sin (πœ‹

6(π‘₯ βˆ’ 3)) + 900(1.07)π‘₯

Alternatively, if we had used the cosine function, we’d get:

β„Ž(π‘₯) = βˆ’33 cos (πœ‹

6π‘₯) + 900(1.07)π‘₯

9. The frequency is 18Hz, therefore period is 1/18 seconds. Starting amplitude is 10 cm. Since

the amplitude decreases with time, the sinusoidal component must be multiplied by an

exponential function. In this case, the amplitude decreases by 15% every second, so each new

amplitude is 85% of the prior amplitude. Therefore, our equation is 𝑦 = 𝑓(π‘₯) = 10cos (36πœ‹π‘₯) βˆ™

(0.85)π‘₯.

11. The initial amplitude is 17 cm. Frequency is 14 Hz, therefore period is 1/14 seconds.

For this spring system, we will assume an exponential model with a sinusoidal factor.

The general equation looks something like this: 𝐷(𝑑) = 𝐴(𝑅)𝑑 βˆ™ cos (𝐡𝑑) where A is amplitude, R

determines how quickly the oscillation decays, and B determines how quickly the system

oscillates. Since 𝐷(0) = 17, we know 𝐴 = 17. Also, 𝐡 =2πœ‹

period= 28.

We know 𝐷(3) = 13, so, plugging in:

13 = 17(𝑅)3 cos(28πœ‹ βˆ™ 3)

13 = 17(𝑅)3 βˆ™ 1

𝑅3 =13

17

𝑅 = √13

17

3

β‰ˆ 0.9145

Thus, the solution is 𝐷(𝑑) = 17(0.9145)𝑑 cos(28πœ‹π‘‘).

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13. By analysis:

(a) must have constant amplitude with exponential growth, therefore the correct graph is IV.

(b) must have constant amplitude with linear growth, therefore the correct graph is III.

15. Since the period of this function is 4, and values of a sine function are on its midline at the

endpoints and center of the period, 𝑓(0) and 𝑓(2) are both points on the midline. We’ll start by

looking at our function at these points:

At 𝑓(0), plugging into the general form of the equation, 6 = π‘Žπ‘0 + 𝑐sin(0), so π‘Ž = 6.

At 𝑓(2): 96 = 6𝑏2 + 𝑐sin(πœ‹), so 𝑏 = 4.

At 𝑓(1): 29 = 6(4)1 + 𝑐sin (πœ‹

2). Solving gives 𝑐 = 5.

This gives a solution of 𝑦 = 6 βˆ™ 4π‘₯ + 5 sin (πœ‹

2π‘₯).

17. Since the period of this function is 4, and values of a sine function are on its midline at the

endpoints and center of the period, 𝑓(0) and 𝑓(2) are both points on the midline.

At 𝑓(0), plugging in gives 7 = π‘Žsin(0) + π‘š + 𝑏 βˆ™ 0, so π‘š = 7.

At 𝑓(2): 11 = π‘Žsin(πœ‹) + 7 + 2𝑏. Since sin(πœ‹) = 0, we get 𝑏 = 2.

At 𝑓(1): 6 = π‘Žsin (πœ‹

2) + 7 + 2 βˆ™ 1. Simplifying, π‘Ž = βˆ’3.

This gives an equation of 𝑦 = βˆ’3sin (πœ‹

2π‘₯) + 2π‘₯ + 7.

19. Since the first two places cos(πœƒ) = 0 are when πœƒ =πœ‹

2 or

3πœ‹

2, which for cos (

πœ‹

2π‘₯) occur when

π‘₯ = 1 or π‘₯ = 3, we’ll start by looking at the function at these points:

At 𝑓(1), plugging in gives 3 = π‘Žπ‘1 cos (πœ‹

2) + 𝑐. Since cos (

πœ‹

2) = 0, 𝑐 = 3. (Note that looking

at 𝑓(3) would give the same result.)

At 𝑓(0): 11 = π‘Žπ‘0 cos(0) + 3. Simplifying, we see π‘Ž = 8.

At 𝑓(2): 1 = 8𝑏2 cos(πœ‹) + 3. Since cos(πœ‹) = βˆ’1, it follows that 𝑏 =1

2:

1 = βˆ’8𝑏2 + 3

βˆ’8𝑏2 = βˆ’2

𝑏2 =1

4

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𝑏 = Β±1

2, but since we require exponential expressions to have a positive number as the base,

𝑏 =1

2. Therefore, the final equation is: 𝑦 = 8 (

1

2)

π‘₯

cos (πœ‹

2π‘₯) + 3.