Section 8.3 Trigonometric Equations

Σχετικά έγγραφα
Section 7.6 Double and Half Angle Formulas

PARTIAL NOTES for 6.1 Trigonometric Identities

Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1

Inverse trigonometric functions & General Solution of Trigonometric Equations

3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β

If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2

If we restrict the domain of y = sin x to [ π 2, π 2

CRASH COURSE IN PRECALCULUS

Section 9.2 Polar Equations and Graphs

CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS

Trigonometric Formula Sheet

Section 7.7 Product-to-Sum and Sum-to-Product Formulas

Areas and Lengths in Polar Coordinates

Matrices and Determinants

Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics

Review Test 3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Areas and Lengths in Polar Coordinates

2 Composition. Invertible Mappings

Example Sheet 3 Solutions

TRIGONOMETRIC FUNCTIONS

Trigonometry 1.TRIGONOMETRIC RATIOS

MathCity.org Merging man and maths

10/3/ revolution = 360 = 2 π radians = = x. 2π = x = 360 = : Measures of Angles and Rotations

Chapter 7 Analytic Trigonometry

ANSWERSHEET (TOPIC = DIFFERENTIAL CALCULUS) COLLECTION #2. h 0 h h 0 h h 0 ( ) g k = g 0 + g 1 + g g 2009 =?

Solutions to Exercise Sheet 5

Finite Field Problems: Solutions

Srednicki Chapter 55

Chapter 6 BLM Answers

Section 8.2 Graphs of Polar Equations

CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD

2 2 2 The correct formula for the cosine of the sum of two angles is given by the following theorem.

Homework 3 Solutions

HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:

is like multiplying by the conversion factor of. Dividing by 2π gives you the

Math221: HW# 1 solutions

Exercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.

Solution to Review Problems for Midterm III

Second Order RLC Filters

Pg The perimeter is P = 3x The area of a triangle is. where b is the base, h is the height. In our case b = x, then the area is

Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.

DESIGN OF MACHINERY SOLUTION MANUAL h in h 4 0.

Homework 8 Model Solution Section

EE512: Error Control Coding

9.09. # 1. Area inside the oval limaçon r = cos θ. To graph, start with θ = 0 so r = 6. Compute dr

2 2 2 The correct formula for the cosine of the sum of two angles is given by the following theorem.

(a,b) Let s review the general definitions of trig functions first. (See back cover of your book) sin θ = b/r cos θ = a/r tan θ = b/a, a 0

The Simply Typed Lambda Calculus

Second Order Partial Differential Equations

Principles of Mathematics 12 Answer Key, Contents 185

SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

1. If log x 2 y 2 = a, then dy / dx = x 2 + y 2 1] xy 2] y / x. 3] x / y 4] none of these

Concrete Mathematics Exercises from 30 September 2016

AREAS AND LENGTHS IN POLAR COORDINATES. 25. Find the area inside the larger loop and outside the smaller loop

derivation of the Laplacian from rectangular to spherical coordinates

4.6 Autoregressive Moving Average Model ARMA(1,1)

Approximation of distance between locations on earth given by latitude and longitude

Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)

Απόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.

2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.

6.3 Forecasting ARMA processes

Differentiation exercise show differential equation

( y) Partial Differential Equations

Differential equations

Derivations of Useful Trigonometric Identities

Numerical Analysis FMN011

University of Illinois at Urbana-Champaign ECE 310: Digital Signal Processing

D Alembert s Solution to the Wave Equation

Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =

CHAPTER 48 APPLICATIONS OF MATRICES AND DETERMINANTS

k A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +

MATH 150 Pre-Calculus

ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 19/5/2007

Reminders: linear functions

Quadratic Expressions

SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018

*H31123A0228* 1. (a) Find the value of at the point where x = 2 on the curve with equation. y = x 2 (5x 1). (6)

F-TF Sum and Difference angle

b. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!

3.4. Click here for solutions. Click here for answers. CURVE SKETCHING. y cos x sin x. x 1 x 2. x 2 x 3 4 y 1 x 2. x 5 2

Forced Pendulum Numerical approach

Problem 1.1 For y = a + bx, y = 4 when x = 0, hence a = 4. When x increases by 4, y increases by 4b, hence b = 5 and y = 4 + 5x.

C.S. 430 Assignment 6, Sample Solutions

Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit

An Inventory of Continuous Distributions

Answer sheet: Third Midterm for Math 2339

( ) 2 and compare to M.

Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1

Solution Series 9. i=1 x i and i=1 x i.

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

26 28 Find an equation of the tangent line to the curve at the given point Discuss the curve under the guidelines of Section

DiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation

Chapter 6: Systems of Linear Differential. be continuous functions on the interval

SOLUTIONS TO MATH38181 EXTREME VALUES AND FINANCIAL RISK EXAM

1 String with massive end-points

forms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with

ST5224: Advanced Statistical Theory II

Parametrized Surfaces

Jackson 2.25 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Transcript:

99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions. Many times, an equation with a trigonometric function will have an infinite number of solutions. Thus, we will need to write the general fm of the solution. Find the a) general solution as well as b) eight particular solutions: Ex. 1 cos(x) = If we examine the graph of y = cos(x) and y = are an infinite number of points the two curves intersect:, we see that there In the interval [0, π), the cosine function is positive in the first and fourth quadrants. In the first quadrant, x = cos 1 ( ) = π. Since π is also our reference angle, then π π = π is the angle in the fourth quadrant. The cosine function is periodic with period π, so these solutions will repeat every π. Thus, our general solution is a) {x x = π π + kπ x = + kπ, k is an integer} b) To find eight solutions, we can pick k = 1, 0, 1, k = 1 k = 0 π π π + ( 1)π = π 1.5 + ( 1)π = π 1 0.5 0 π π π -0.5 π π π -1-1.5 + (0)π = π π + (0)π = π y = y = cos(x)

100 k = 1 k = π 1π π + (1)π = + ()π = π Ex. sin(θ) = + (1)π = π So, { π, π, π, π solutions to the equation. π + ()π =, 1π, π,, } are eight In the interval [0, π), the sine function is negative in the third and fourth quadrants. In the first quadrant, θ = sin 1 ( ) = π. Thus, π is our reference angle. The angle we need in the third quadrant is π + π = and the angle we need in the fourth quadrant is π π =. The sine function is periodic with period π, so these solutions will repeat every π. Thus, our general solution is a) {x x = + kπ x = + kπ, k is an integer} b) To find eight solutions, we can pick k = 1, 0, 1, k = 1 k = 0 π + ( 1)π = + (0)π = + ( 1)π = π k = 1 k = 10π + (1)π = π + (1)π = So, { π, π, solutions to the equation. Ex. 5cot (x) = First, we need to solve f cot(x): 5cot (x) = 5cot (x) = 5 cot (x) = 1 cot(x) = ± 1 + (0)π = + ()π = 1π + ()π = 17π,, 10π, π, 1π, 17π } are eight

101 The cotangent function is positive in quadrant I and negative in quadrant II. Since cot(x) = 1 when tan(x) = 1, then x = π 4 is the reference angle. In quadrant II, the angle we need is π π 4 = π 4. Since the cotangent function is periodic with period of π, then the solutions will repeat every multiple of π. a) {x x = π π + nπ x = 4 4 + nπ, n is an integer}. Since the consecutive angles differ by π, we can write the general solution as: {x x = π 4 + kπ, k is an integer}. b) Eight solutions are { π 4, π 4, π 4, π 4, 4, 7π 4, 9π 4, π 4 }. When solving a trigonometric equation where the argument is a multiple of the variable, we will need to use the general solution f argument and then solve f variable. We will then need to run through values of k until we find all the angles within a specified interval. Solve the following f angles in [0, π). Ex. 4 cos(4θ) 1 = 0 First, solve f cos(4θ): cos(4θ) 1 = 0 cos(4θ) = 1 cos(4θ) = 1 (let x = 4θ) Thus, cos(x) = 1 when x = π x = π π =. Since the period of cosine is π, then the general solution will have the fm of: x = 4 + kπ + kπ Now, solve f θ by dividing by four: 1 + kπ 1 + kπ We need to find all the angles in [0, π). k = 1 1 + 1π = 1 1 + 1π = π No 1 k = 0 k = 1 1 + 0π = π 1 1 + 1π = 7π 1 1 + 0π = 1 1 + 1π = π 1

10 k = k = k = 4 1 + π = 1π 1 1 + π = 19π 1 1 + = 1 1 + π = 17π 1 1 + π = π 1 1 + = 9π 1 The solution is { π 1, 1, 7π 1, π 1, 1π 1, 17π 1, 19π 1, π 1 } No Ex. 5 4sin(θ) + = We first need to solve f sin(θ): 4sin(θ) + = 4sin(θ) = 0 sin(θ) = 0 (let x = θ) Thus, sin(x) = 0 when x = 0 π. Since the period of sine is π, then the general solution will have the fm of: x = θ = 0 + kπ π + kπ Since consecutive angles differ by π, then we can state the general solution as: x = kπ Now, solve f θ by dividing by : θ = kπ We need to find all the angles in [0, π). k = 1 θ = 1π = π 0π No k = 0 θ = = 0 k = 1 θ = 1π = π π k = θ = k = k = 5 θ = The solution is {0, π, π Ex. tan(θ + π ) = = π k = 4 θ = k =, π,, }. = π No Let x = θ + π. Since tan(x) = when x = π, then π is our reference angle. The tangent function is negative in quadrant II, so the angle is π π = π. Since the period of tangent is π, then the general solution will have the fm of:

x = θ + π = π + kπ Now, solve f θ: θ + π = π + kπ π + kπ + kπ 10 1 + kπ We need to find all the angles in [0, π). k = 1 1 + 1π = 1 No k = 0 1 + 0π = π 1 k = 1 1 + 1π = 7π 1 k = 1 + π = 1π 1 k = 1 + π = 19π 1 k = 4 1 + = 1 No The solution is { π 1, 7π 1, 1π 1, 19π 1 }. Objective : Solving a Trigonometric Equation with a Calculat. Solve the following f angles in [0, π). Ex. 7 cos(x) = 0. Here, we will need to use our calculat to find the value f x: cos(x) = 0. x = cos 1 (0.) = 0.979518 0.97 This angle is in the first quadrant. However, the cosine is also positive in the fourth quadrant. Since θ R 0.97, then the angle in the fourth quadrant is π 0.979518 5.559 Thus, the solution is { 0.97, 5.559} Ex. 8 tan(x) = Here, we will need to use our calculat to find the value f x: tan(x) = which means x = tan 1 ( ) = 1.1071487 This angle is not in [0, π). In that interval, the tangent function is negative in quadrant II, and IV. Since the inverse tangent function gave us the opposite of the reference angle, then θ R = 1.1071487 Thus, in the second quadrant, the angle is π 1.1071487

104 Ex. 9 =.0444.044. Similarly, in quadrant IV, the angle is π 1.1071487 = 5.1705 5.170 Hence, the solution is {.044, 5.170}. Due to bad weather, a plane in a holding pattern around the Dallas airpt. The distance d in miles the plane is from the airpt at time t minutes is given by d(t) = 80sin(0.55t) + 10. a) When the plane enters the holding pattern, t = 0, how far is it from the airpt? b) During the first 0 minutes after the plane enters the holding pattern, what time(s) t will the plane be exactly 80 miles from the airpt? a) d(0) = 80sin(0.55(0)) + 10 = 80sin(0) + 10 = 0 + 10 = 10 The plane was 10 miles from the airpt. b) Set d(t) = 80 and solve: 80sin(0.55t) + 10 = 80 80sin(0.55t) = 50 sin(0.55t) = 0.5 0.55t = sin 1 ( 0.5) = 0.755 Thus, the reference angle is 0.755 The sine is negative in quadrant III and IV, so the angles are π + 0.755 =.81741 and π 0.755 = 5.08057 Thus, 0.55t =.81741 + kπ 5.08057 + kπ, k is an integer. Solving f t yields: t =.994985 + 40kπ If k = 0, then t =.994985 + 40(0)π 10.1941 + 40kπ 10.1941 + 40(0)π t.995 minutes 10.195 minutes If k = 1, then t =.994985 + 40(1)π 10.1941 + 40(1)π t =.994985 +.497 10.1941 +.497 t = 18.471 1.044 t 18.5 minutes 1.04 minutes The three times that are within the first twenty minutes are {.995 minutes, 10.195 minutes, 18.5 minutes}

105 Objective : Solving a Trigonometric Equation in Quadratic Fm In solving trigonometric equation in quadratic fm, we will have to use an identity and/ fact befe we can get a series of linear equations involving one trigonometric function to solve. It will also be imptant to make a note of any values that make the iginal equation undefined. Solve f all values in [0, π): Ex. 10 cos (θ) + cos(θ) = 1 cos (θ) + cos(θ) = 1 (get zero on one side) cos (θ) + cos(θ) 1 = 0 Think of x + x 1 = (x 1)(x + 1), so cos (θ) + cos(θ) 1 = (cos(θ) 1)(cos(θ) + 1) Hence, (cos(θ) 1)(cos(θ) + 1) = 0 (solve) cos(θ) 1 = 0 cos(θ) + 1 = 0 cos(θ) = 1 cos(θ) = 1 π π = The solution is { π, π, }. Ex. sin (θ) 8sin(θ) = 0 sin (θ) 8sin(θ) = 0 Think of x 8x = (x )(x + 1), so sin (θ) 8sin(θ) = (sin(θ) )(sin(θ) + 1) Hence, (sin(θ) )(sin(θ) + 1) = 0 (solve) (sin(θ) ) = 0 (sin(θ) + 1) = 0 sin(θ) = No solution The solution is { π }. sin(θ) = 1 Objective 4: Solving Trigonometric Equations Using Identities. Ex. 1 csc (θ) = cot(θ) + 1

10 The cosecant and cotangent function is undefined when the sin(θ) = 0 θ = 0 π. Thus, our restrictions are θ 0 π. csc (θ) = cot(θ) + 1 (csc (θ) = cot (θ) + 1) cot (θ) + 1 = cot(θ) + 1 (subtract cot(θ) + 1 from both sides) cot (θ) cot(θ) = 0 (fact cot(θ)) cot(θ)[cot(θ) 1] = 0 (solve) cot(θ) = 0 cot(θ) 1 = 0 cot(θ) = 0 cot(θ) = 1 cot(θ) = 0 when cos(θ) = 0. cot(θ) = 1 when tan(θ) = 1 4 π + π 4 =. None of these values match our 4 π restrictions, so the solution is { π 4, π, 4, π }. Ex. 1 sec(θ) = tan(θ) + cot(θ) The secant and tangent function is undefined when the cos(θ) = 0. The cotangent function is undefined when the sin(θ) = 0 θ = 0 π. Thus, our restrictions are θ 0, π π, π,. sec(θ) = tan(θ) + cot(θ) (write in terms of sine and cosine) 1 cos(θ) = sin(θ) cos(θ) + cos(θ) (multiply by cos(θ)sin(θ)) sin(θ) π 1 sin(θ) cos(θ) cos(θ)sin(θ) = cos(θ)sin(θ) + cos(θ) cos(θ) sin(θ) cos(θ)sin(θ) sin(θ) = sin (θ) + cos (θ) (sin (θ) + cos (θ) = 1) sin(θ) = 1 But, our restrictions say that θ π, so we have to reject our answer. Thus, this equation has no solution.