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Thomas Calculus 15Th Hass Solutions Manual

Page 1


Solutions

Manual for Thomas' Calculus

15th Edition by Hass, Heil, Weir

ISBN: 9780137615582

INSTRUCTOR’S SOLUTIONS MANUAL

JENNIFER A. BLUE

SUNY Empire State College

T HOMAS ’ C ALCULUS

L ATE T RANSCEN DENTALS

FIFTEENTH EDITION

Based on the original work by George B. Thomas, Jr

Massachusetts Institute of Technology

as revised by

Joel Hass

University of California, Davis

Christopher Heil

Georgia Institute of Technology

Maurice D. Weir

Naval Postgraduate School

The author and publisher of this book have used their best efforts in preparing this book. These efforts include the development, research, and testing of the theories and programs to determine their effectiveness. The author and publisher make no warranty of any kind, expressed or implied, with regard to these programs or the documentation contained in this book. The author and publisher shall not be liable in any event for incidental or consequential damages in connection with, or arising out of, the furnishing, performance, or use of these programs.

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ISBN-13: 978-0-13-761600-8

ISBN-10: 0-13-761600-7

TABLE OF CONTENTS

1 Functions 1

1.1 Functions and Their Graphs 1

1.2 Combining Functions; Shifting and Scaling Graphs 9

1.3 Trigonometric Functions 19

1.4 Graphing with Software 27

Practice Exercises 32

Additional and Advanced Exercises 40

2 Limits and Continuity 43

2.1 Rates of Change and Tangents to Curves 43

2.2 Limit of a Function and Limit Laws 47

2.3 The Precise Definition of a Limit 57

2.4 One-Sided Limits 65

2.5 Continuity 70

2.6 Limits Involving Infinity; Asymptotes of Graphs 75

Practice Exercises 86

Additional and Advanced Exercises 92

3 Derivatives 99

3.1 Tangents and the Derivative at a Point 99

3.2 The Derivative as a Function 105

3.3 Differentiation Rules 116

3.4 The Derivative as a Rate of Change 121

3.5 Derivatives of Trigonometric Functions 127

3.6 The Chain Rule 134

3.7 Implicit Differentiation 146

3.8 Related Rates 155

3.9 Linearization and Differentials 160

Practice Exercises 167

Additional and Advanced Exercises 180

4 Applications of Derivatives 187

4.1 Extreme Values of Functions on Closed Intervals 187

4.2 The Mean Value Theorem 195

4.3 Monotonic Functions and the First Derivative Test 201

4.4 Concavity and Curve Sketching 213

4.5 Applied Optimization 236

4.6 Newton's Method 251

4.7 Antiderivatives 255

Practice Exercises 263

Additional and Advanced Exercises 277

5 Integrals 285

5.1 Area and Estimating with Finite Sums 285

5.2 Sigma Notation and Limits of Finite Sums 290

5.3 The Definite Integral 296

5.4 The Fundamental Theorem of Calculus 312

5.5 Indefinite Integrals and the Substitution Method 322

5.6 Definite Integral Substitutions and the Area Between Curves 328 Practice Exercises 345

Additional and Advanced Exercises 355

6 Applications of Definite Integrals 361

6.1 Volumes Using Cross-Sections 361

6.2 Volumes Using Cylindrical Shells 373

6.3 Arc Length 384

6.4 Areas of Surfaces of Revolution 391

6.5 Work and Fluid Forces 397

6.6 Moments and Centers of Mass 408

Practice Exercises 422

Additional and Advanced Exercises 432

7 Transcendental Functions 439

7.1 Inverse Functions and Their Derivatives 439

7.2 Natural Logarithms 449

7.3 Exponential Functions 457

7.4 Exponential Change and Separable Differential Equations 472

7.5 Indeterminate Forms and L’Hôpital’s Rule 478

7.6 Inverse Trigonometric Functions 487

7.7 Hyperbolic Functions 501

7.8 Relative Rates of Growth 510

Practice Exercises 515

Additional and Advanced Exercises 529

8 Techniques of Integration 533

8.1 Using Basic Integration Formulas 533

8.2 Integration by Parts 544

8.3 Trigonometric Integrals 558

8.4 Trigonometric Substitutions 567

8.5 Integration of Rational Functions by Partial Fractions 577

8.6 Integral Tables and Computer Algebra Systems 588

8.7 Numerical Integration 599

8.8 Improper Integrals 612

8.9 Probability 626

Practice Exercises 634

Additional and Advanced Exercises 648

9 First-Order Differential Equations 657

9.1 Solutions, Slope Fields, and Euler's Method 657

9.2 First-Order Linear Equations 667

9.3 Applications 671

9.4 Graphical Solutions of Autonomous Equations 675

9.5 Systems of Equations and Phase Planes 683

Practice Exercises 688

Additional and Advanced Exercises 696

10 Infinite Sequences and Series 699

10.1 Sequences 699

10.2 Infinite Series 711

10.3 The Integral Test 720

10.4 Comparison Tests 728

10.5 Absolute Convergence; The Ratio and Root Tests 738

10.6 Alternating Series and Conditional Convergence 745

10.7 Power Series 755

10.8 Taylor and Maclaurin Series 767

10.9 Convergence of Taylor Series 773

10.10 The Binomial Series and Applications of Taylor Series 781

Practice Exercises 791

Additional and Advanced Exercises 801

11 Parametric Equations and Polar Coordinates 807

11.1 Parametrizations of Plane Curves 807

11.2 Calculus with Parametric Curves 816

11.3 Polar Coordinates 825

11.4 Graphing Polar Coordinate Equations 831

11.5 Areas and Lengths in Polar Coordinates 839

11.6 Conic Sections 845

11.7 Conics in Polar Coordinates 856

Practice Exercises 866

Additional and Advanced Exercises 877

12 Vectors and the Geometry of Space 883

12.1 Three-Dimensional Coordinate Systems 883

12.2 Vectors 888

12.3 The Dot Product 894

12.4 The Cross Product 900

12.5 Lines and Planes in Space 908

12.6 Cylinders and Quadric Surfaces 916

Practice Exercises 922

Additional and Advanced Exercises 930

13 Vector-Valued Functions and Motion in Space 937

13.1 Curves in Space and Their Tangents 937

13.2 Integrals of Vector Functions; Projectile Motion 944

13.3 Arc Length in Space 953

13.4 Curvature and Normal Vectors of a Curve 957

13.5 Tangential and Normal Components of Acceleration 965

13.6 Velocity and Acceleration in Polar Coordinates 972

Practice Exercises 974

Additional and Advanced Exercises 981

14 Partial Derivatives 985

14.1 Functions of Several Variables 985

14.2 Limits and Continuity in Higher Dimensions 995

14.3 Partial Derivatives 1003

14.4 The Chain Rule 1012

14.5 Directional Derivatives and Gradient Vectors 1025

14.6 Tangent Planes and Differentials 1030

14.7 Extreme Values and Saddle Points 1038

14.8 Lagrange Multipliers 1055

14.9 Taylor's Formula for Two Variables 1066

14.10 Partial Derivatives with Constrained Variables 1070

Practice Exercises 1073

Additional and Advanced Exercises 1090

15 Multiple Integrals 1097

15.1 Double and Iterated Integrals over Rectangles 1097

15.2 Double Integrals over General Regions 1100

15.3 Area by Double Integration 1115

15.4 Double Integrals in Polar Form 1120

15.5 Triple Integrals in Rectangular Coordinates 1126

15.6 Moments and Centers of Mass 1132

15.7 Triple Integrals in Cylindrical and Spherical Coordinates 1139

15.8 Substitutions in Multiple Integrals 1152

Practice Exercises 1160

Additional and Advanced Exercises 1168

16 Integrals and Vector Fields 1175

16.1 Line Integrals 1175

16.2 Vector Fields and Line Integrals: Work, Circulation, and Flux 1181

16.3 Path Independence, Conservative Fields, and Potential Functions 1193

16.4 Green's Theorem in the Plane 1199

16.5 Surfaces and Area 1207

16.6 Surface Integrals 1217

16.7 Stokes' Theorem 1228

16.8 The Divergence Theorem and a Unified Theory 1235 Practice Exercises 1242

Additional and Advanced Exercises 1252

17 Second-Order Differential Equations 1257

17.1 Second-Order Linear Equations 1257

17.2 Nonhomogeneous Linear Equations 1263

17.3 Applications 1275

17.4 Euler Equations 1281

17.5 Power-Series Solutions 1284

18 Complex Functions 1295

18.1 Complex Numbers 1295

18.2 Functions of a Complex Variable 1297

18.3 Derivatives 1298

18.4 The Cauchy-Riemann Equations 1299

18.5 Complex Power Series 1299

18.6 Some Complex Functions 1300

18.7 Conformal Maps 1302

Additional and Advanced Exercises 1303

19 Fourier Series and Wavelets 1305

19.1 Periodic Functions 1305

19.2 Summing Sines and Cosines 1305

19.3 Vectors and Approximation in Three and More Dimensions 1307

19.4 Approximation of Functions 1310

19.5 Advanced Topic: The Haar System and Wavelets 1317

Additional and Advanced Exercises 1321

CHAPTER 1 FUNCTIONS

1.1 FUNCTIONS AND THEIR GRAPHS

1. domain (,);range[1,) 

2. domain [0,);range(,1] 

3. domain [2,); y  in range and y  510 x  0 y   can be any positive real number range   [0,). 

4. domain (,0][3,); y  in range and 2 30 y xx y   can be any positive real number  range[0,) 

5. domain (,3)(3,); y  in range and

4 3 3 00 t ty    can be any nonzero real number range(,0)(0,). 

6. domain (,4)(4,4)(4,); y 

  or if 2 2 22 16 16 4416160 t tt     , or if 2 2 2 16 41600 t t ty       can be any nonzero real number 1 8 range(,](0,).  

7. (a) Not the graph of a function of x since it fails the vertical line test. (b) Is the graph of a function of x since any vertical line intersects the graph at most once.

8. (a) Not the graph of a function of x since it fails the vertical line test. (b) Not the graph of a function of x since it fails the vertical line test.

9. base

2 22 3 22 ;(height) height; x x xx    area is 1 2 ()ax  (base)(height)  2 33 1 224 () ; x xx perimeter is ()3. p xxxxx  10. 222 2 sidelength ; d ss s ds

11. Let D  diagonal length of a face of the cube and   the length of an edge. Then 222 Dd  and 2222 3 23. d D d       The surface area is 2 22 6 3 62 d d   and the volume is   23 3/2 3 3 33 . dd 

12. The coordinates of P are  ,x x so the slope of the line joining P to the origin is 1 (0). x x x m x  Thus, 

 2 11 ,,. m m xx 

13. 222222 55525 111 24244416 245 ;(0)(0)() xyyxLxyxxxxx    2 2 202025 202025 2 5525 4416164 xx xx xx 

14. 22 2 2 2 2 2 2 2 33;(4)(0)(34)(1) y xyxLxyyyyy   42242 21 1 yyyyy 

15. The domain is (,). 

17. The domain is (,). 

19. The domain is (,0)(0,). 

21. The domain is (,5)(5,3][3,5)(5,). 

23. Neither graph passes the vertical line test.

16. The domain is (,). 

18. The domain is (,0]. 

20. The domain is (,0)(0,). 

22. The range is [5,)  .

(a) (b)

24. Neither graph passes the vertical line test. (a) (b)

012 010 x y

012 100 x y 27. 2 2 4,1 () 2,1 x x F x x xx

29. (a) Line through (0, 0) and (1, 1): ; y x  Line through (1, 1) and (2, 0): 2 y x  ,01 () 2,12 x x fx x x

(b) 2,01 0,12 () 2,23 0,34 x x fx x x

30. (a) Line through (0, 2) and (2, 0): 2 y x  Line through (2, 1) and (5, 0): 01 11 5233 , m  so 5 11 333 (2)1 y xx

5 1 33 2,02 () ,25 xx fx xx

1 Functions

(b) Line through (1,0) and (0,3): 30 0(1) 3, m  so 33 y x 

Line through (0, 3) and 13 4 202 (2,1): 2, m  so 23 y x  33,10 () 23,02 x x fx x x

31. (a) Line through (1,1) and (0, 0): y x 

Line through (0, 1) and (1, 1): 1 y 

Line through (1, 1) and (3, 0): 01 11 3122 , m  so 3 11 222 (1)1 y xx

3 1 22 10 ()101 13 x x fxx x x

(b) Line through (2,1) and (0, 0): 1 2 y

Line through (0, 2) and (1, 0): 22 y x

Line through (1,1) and (3,1): 1 y

32. (a) Line through  2 ,0 T and (T, 1): 10 2 (/2) , TTT m

33. (a) 0for[0,1)xx

only when x is an integer.

35. For any real number ,1,x nxn where n is an integer. Now: 1(1). nxnnxn

By definition: and

36. To find f (x) you delete the decimal or fractional portion of x, leaving only the integer part.

for all

Copyright  2023 Pearson Education, Inc.

37. Symmetric about the origin

Dec: x   

Inc: nowhere

39. Symmetric about the origin

Dec: nowhere

Inc: 0 0 x x 

41. Symmetric about the y-axis

Dec: 0 x 

Inc: 0 x 

38. Symmetric about the y-axis

Dec: 0 x 

Inc: 0 x  

40. Symmetric about the y-axis

Dec: 0 x  

Inc: 0 x 

42. No symmetry

Dec: 0 x 

Inc: nowhere

43. Symmetric about the origin

Dec: nowhere

Inc: x   

45. No symmetry

Dec: 0 x  

Inc: nowhere

44. No symmetry

Dec: 0 x  

Inc: nowhere

46. Symmetric about the y-axis

Dec: 0 x 

Inc: 0 x 

47. Since a horizontal line not through the origin is symmetric with respect to the y-axis, but not with respect to the origin, the function is even.

48.   55 5 55111 () ()and()() (). xx x f xxfxx fx  Thus the function is odd.

49. Since 22 ()1()1(). f xxxfx  The function is even.

50. Since 22 [ ()][()()] f xxxfxxx   and 22 [ ()][()()] f xxxfxxx   the function is neither even nor odd.

51. Since (),()333()() g xxxgxxxxxgx  So the function is odd.

52. 4242 ()31()3()1(), g xxxxxgx  thus the function is even.

53. 22 11 1()1 () (). xx g xg x  Thus the function is even.

54. ();()2211 (). x x xx g xgxgx  So the function is odd.

55. 111 ();();()111 ttt hththt Since ()()and()(), hthththt   the function is neither even nor odd.

56. Since 33 |||()|,()() tththt  and the function is even.

57. ()21,()21. htthtt  So ()().()21, hththtt   so ()().htht   The function is neither even nor odd.

58. ()2||1and()2||12||1. htthttt  So ()() htht  and the function is even.

59. ()sin2;()sin2(). g xxgxxgx  So the function is odd.

60. 22 ()sin;()sin(). g xxgxxgx  So the function is even.

61. ()cos3;()cos3(). g xxgxxgx  So the function is even.

62. ()1cos;()1cos(). g xxgxxgx  So the function is even.

63. 111 333 25(75) ;60180sktkksttt

64. 2222 12960(18)4040;40(10)4000joulesKcvccKvK

65. 242412 624;1045kk sss rkrs  

66. 3 147001470024500 100039 14.7 14700 ;23.4 628.2in. kk VVV PkPV

67. 32 ()(142)(222)472308;07 Vfxxxxxxxx 

68. (a) Let h  height of the triangle. Since the triangle is isosceles,   22 2 22.ABABAB    So,

2 22121 hhB     is at (0,1)  slope of 1 AB   The equation of AB is ()1;[0,1].yfxxx  (b) 2 ()22(1) [0, 2] ;1 2 Axxyxxxx x 

69. (a) Graph h because it is an even function and rises less rapidly than does Graph g.

(b) Graph f because it is an odd function.

(c) Graph g because it is an even function and rises more rapidly than does Graph h.

70. (a) Graph f because it is linear.

(b) Graph g because it contains (0, 1).

(c) Graph h because it is a nonlinear odd function.

71. (a) From the graph, 4 2 1(2,0)(4,) x x x   

(b) 44 22110 x x x x    2 28(4)(2) 4 0:10222 0 0 xxxx x x xx x 

4 x   since x is positive; 2 28(4)(2) 4 0:10222 0 0 xxxx x x xx x 

    2 x   since x is negative; sign of (4)(2) x x 

Solution interval: (2,0)(4,) 

72. (a) From the graph, 3 2 11 (,5)(1,1) xx x    

(b) Case 1: x  3(1) 3 2 111 2 x xxx      33225. x xx     Thus, (,5) x  solves the inequality.

Case 11: x  3 2 11xx   3(1) 1 2 x x   33225 x xx     which is true if 1. x  Thus, (1,1) x  solves the inequality.

Case 1 : x  3 2 11 3 xx x     3 22 x   5 x  which is never true if 1 ,x  so no solution here.

In conclusion, (,5)(1,1). x 

73. A curve symmetric about the x-axis will not pass the vertical line test because the points (x, y) and (,) x y lie on the same vertical line. The graph of the function () 0 y fx  is the x-axis, a horizontal line for which there is a single y-value, 0, for any x.

74. price405, x  quantity  30025 x  () R x  (405)(30025) x x 

76. (a) Note that 2mi10,560ft,  so there are 80022 x  feet of river cable at $180 per foot and (10,560) x feet of land cable at $100 per foot. The cost is ()18080022 Cxx

100(10,560 - x). (b) (0)$1,200,000 (500)$1,175,812 (1000)$1,186,512 (1500)$1,212,000 (2000)$1,243,732 (2500)$1,278,479 (3000)$1,314,870

Values beyond this are all larger. It would appear that the least expensive location is less than 2000 feet from the point P

1.2 COMBINING FUNCTIONS; SHIFTING AND SCALING GRAPHS

1.

2.

3.

5. (a) 2 (b)

(d) 22 (5)31022 xxx

(g) 10 x  (h) (3)362242 6 xxx

6. (a) 1 3 (b) 2 (c) 1 11 1 x xx  (d)

7. ()()((())) f ghxfghx

((4)) f gx

8. 2 ()()((()))(()) fghxfghxfgx

9.

1 ()()((())) x fghxfghxfg

10.

()()((()))2 fghxfghxfgx

(3(4)) f x (123)(123) f xx

11. (a) ()() f gx  (b) ()() j gx  (c) ()() g gx  (d) ()() j jx  (e) ()() g hfx

12. (a) ()() f jx

(d) ()() f fx

(b) ()() g hx

(e) ()() j gfx

13. g(x) f (x) ()() f gx  (a) 7 x x 7 x (b) 2 x  3x 3(2)36 x x  (c) 2 x 5 x 2 5 x (d) 1 x x 1 x x 1 1 (1) 1 x x x x x xx x  (e) 1 1 x 1 1 x

(f ) ()() hjfx

(c) ()() hhx

(f ) ()() g fhx

14. (a) 1 1 ()()|()| x fgxgx 

(b) ()1 ()1 ()() g x x gxx fgx  

(c) Since ()()()||, f gxgxx   2 (). g xx 

(d) Since  ()()||, f gxfxx   2 (). f xx  (Note that the domain of the composition is [0,).  )

The completed table is shown. Note that the absolute value sign in part (d) is optional.

x

15. (a) ((1))(1)1 f gf (b) ((0))(2)2 g fg

(c) ((1))(0)2 f ff (d) ((2))(0)0 g gg (e) ((2))(1)1 g fg

(f) ((1))(1)0 f gf

16. (a) ((0))(1)2(1)3, f gf where (0)011 g 

(b) ((3))(1)(1)1, g fg

where (3)231 f 

(c) ((1))(1)110, g gg where (1)(1)1 g 

(d) ((2))(0)202, f ff where (2)22 0 f 

(e) ((0))(2)211, g fg where (0)202 f 

(f )

5 111 2222 2, fgf

17. (a) 1 1 ()()(())1 x x x fgxfgx

 1 1 ()()(()) x gfxgfx    (b) Domain ():(,1](0,), f g 

18. (a) ()()(())12 f gxfgxxx

()()(())1|| g fxgfxx

Domain

()()(()) f gxxfgxx

22. (a)
23. (a)

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Thomas' Calculus 15e Hass Solutions Manual

Copyright  2023 Pearson Education, Inc.

Thomas' Calculus

57. (a) domain: [0, 2]; range: [2, 3]

(c) domain: [0, 2]; range: [0, 2]

(b) domain: [0, 2]; range: [–1, 0]

(d) domain: [0, 2]; range: [–1, 0]

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(e) domain: [–2, 0]; range: [0, 1]

(g) domain: [–2, 0]; range: [0, 1]

58. (a) domain: [0, 4]; range: [–3, 0]

(c) domain: [–4, 0]; range: [0, 3]

(e) domain: [2, 4]; range: [–3, 0]

(f ) domain: [1, 3]; range: [0,1]

(h) domain: [–1, 1]; range: [0, 1]

(b) domain: [–4, 0]; range: [0, 3]

(d) domain: [–4, 0]; range: [1, 4]

(f ) domain: [–2, 2]; range: [–3, 0]

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(g) domain: [1, 5]; range: [–3, 0] (h) domain: [0, 4]; range: [0, 3] 59. 2 33yx

22 (2)141yxx

63. 41 y x 

2 2 1 22 416 x y x 

67. 1(3)12733 y xx

69. Let 21() y xfx and let 1/2 (), g xx 

1/2 1 2 (),hxx

1/2 1 2 ()2, ixx and 1/2 1 2 ()2 ().jxxfx     The graph of ()hx is the graph of () g x shifted left 1 2 unit; the graph of () i x is the graph of ()hx stretched vertically by a factor of 2; and the graph of ()() jxfx  is the graph of () i x reflected across the x-axis.

70. Let 2 1(). x y fx  Let () g x  1/2 (), x ()hx  1/2 (2), x  and 1/2 1 2 ()(2) ixx

2 1(). x f x  The graph of () g x is the graph of y x  reflected across the x-axis. The graph of ()hx is the graph of () g x shifted right two units. And the graph of () i x is the graph of ()hx compressed vertically by a factor of 2 .

31 y x 

2 1 3 4 y x

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71. 3 (). y fxx Shift () f x one unit right followed by a shift two units up to get 3 ()(1)2gxx .

72. 33 (1)2[(1)(2)](). yxxfx 

Let 33 (),()(1), gxxhxx 3 ()(1)(2), ixx and ()[(1)3 jxx (2)]. The graph of ()hx is the graph of () g x shifted right one unit; the graph of () i x is the graph of ()hx shifted down two units; and the graph of () f x is the graph of () i x reflected across the x-axis.

73. Compress the graph of 1 () x fx  horizontally by a factor of 2 to get 1 2 () x gx  Then shift () g x vertically down 1 unit to get 1 2 ()1. x hx 

74. Let 2 1 () x fx  and 2 2 2 21 ()11 x x gx

 Since 21.4,  we see that the graph of () f x stretched horizontally by a factor of 1.4 and shifted up 1 unit is the graph of () g x .

75. Reflect the graph of 3 () y fxx across the x-axis to get 3 (). g xx 

76. 2/3 ()(2)[(1)(2)](1)(2)2/32/32/3 yfxxxx  2/3 (2). x  So the graph of () f x is the graph of 2/3 () g xx  compressed horizontally by a factor of 2.

79. (a) ()()()()()(()) fgxfxgxfxgx ()(), fgx odd

(b)

(c)

()() ()() () (), ffxfxf ggxgxg x x  odd

()() ()() () (), ggxgxg ffxfxf x x  odd

(d) 22 ()()()()()(), f xfxfxfxfxfx  even

(e) 222 2 ()(())(())(), g xgxgxgx  even

(f ) ()()(())(()) f gxfgxfgx 

(g) ()()(())(()) g fxgfxgfx

(h) ()()(())(()) f fxffxffx

(i) ()()(())(()) g gxggxggx

(())()(), f gxfgx

even

()(), g fx   even

f fx 

even

(()) g gx ()(), g gx

 odd

80. Yes, ()0 f x  is both even and odd since ()0() f xfx and ()0() f xfx .

81. (a) (b)

1.3 TRIGONOMETRIC FUNCTIONS

1.

2.

period2  22. period2 

23. 2 period,   symmetric about the origin

25. period4,  symmetric about the s-axis

27. (a) cos x and sec x are positive for x in the interval 22,;  and cos x and sec x are negative for x in the intervals  3 22 ,  and  3 22 ,  sec x is undefined when cos x is 0. The range of sec x is (,1][1,);  the range of cos x is [ 1,1].

24. period1,  symmetric about the origin

26. period4,   symmetric about the origin

(b) sin x and csc x are positive for x in the intervals  3 2 ,   and (0,);  and sin x and csc x are negative for x in the intervals (,0)  and  3 2 , .   csc x is undefined when sin x is 0. The range of csc x is (,1][1,);  the range of sin x is [ 1,1].

28. Since 1 tan cot, x x  cot x is undefined when tan 0 x  and is zero when tan x is undefined. As tan x approaches zero through positive values, cot x approaches infinity. Also, cot x approaches negative infinity as tan x approaches zero through negative values. 29.

33.   222 sinsincoscossin(sin)(0)(cos)(1)cos x xxxxx 

34.   222 sinsincoscossin(sin)(0)(cos)(1)cos x xxxxx 

35. cos()cos(())coscos()sinsin()coscossin(sin) coscossinsin A BABABABABAB A BAB  

36. sin()sin(())sincos()cossin()sincoscos(sin) sincoscossin A BABABABABAB A BAB  

37. If , 0cos()cos01. B AABAB   Also cos()cos()cos A BAA  cos A A  sin A sin A 22 cossin. A A  Therefore, 2 cos A  2 sin1. A 

38. If 2, B   then cos(2) A   coscos2 A  sinsin2(cos)(1) A A   (sin)(0)cos A A  and sin(2)sincos2cossin2(sin)(1)(cos)(0)sin A AAAAA  . The result agrees with the fact that the cosine and sine functions have period 2. 

39. cos()coscossinsin(1)(cos)(0)(sin)cos x xxxxx 

40. sin(2)sin2cos()cos(2)sin()(0)(cos())(1)(sin())sin x xxxxx

41.

333 222 sinsincos()cossin()(1)(cos)(0)(sin())cos x

42.

43.

333 222 coscoscossinsin(0)(cos)(1)(sin)sin x

62 3 22 7 1 1243434322224 sinsinsincoscossin

26 3 22 11222 1 1243434322224 coscoscoscossinsin

52.

53. sin2cos02sincoscos0     cos(2sin1)0cos0 or 2sin10     3 1 222 cos0 or sin ,,or 

 55 3 666262 ,,,,     

54. 2 cos2cos02cos1cos0     2 2coscos10(cos1)(2cos1)0  

  cos10or2cos1    1 2 0cos1orcos or        55 3333 ,,,     

55. sincoscossin coscoscoscos coscossinsin coscoscoscos sin()sincoscoscos tantan cos()coscossinsin 1tantan tan() ABAB ABAB ABAB ABAB A BABAB AB A BABAB AB AB      

56. sincoscossin coscoscoscos coscossinsin coscoscoscos sin()sincoscoscos tantan cos()coscossinsin 1tantan tan()

ABAB ABAB ABAB ABAB A BABAB AB A BABAB AB AB 

57. According to the figure in the text, we have the following: By the law of cosines, 222 2coscabab   22 112cos()22cos() A BAB . By distance formula, 222 (coscos)(sinsin) cABAB  22 22 cos2coscoscossin2sinsinsin22(coscossinsin) A ABBAABBABAB . Thus 2 22cos()22(coscossinsin)cos()coscossinsin cABABABABABAB    .

58. (a) cos()coscossinsin A BABAB 

sincosandcossin22    Let A B  

sin()cos()cos2222coscossinsin sincoscossin A BABABABAB A BAB 



    Because the cosine function is even and the sine function is odd.

(b) cos()coscossinsin cos(())coscos()sinsin() cos()coscos()sinsin()coscossin(sin)coscossinsin

ABABAB ABABAB A BABABABABABAB

59. 222 22 2cos232(2)(3) c ababC 

1 2 cos(60)4912cos(60)13127  Thus, 72.65. c 

60. 222 22 2cos232(2)(3) c ababC  cos(40)1312cos(40).  Thus, 1312cos40°1.951. c 

61. From the figures in the text, we see that sin . h c B  If C is an acute angle, then sin. h b C  On the other hand, if C is obtuse (as in the figure on the right in the text), then sin C  sin() . h b C   Thus, in either case, sinsin sinsin. hbCcBahabCacB   

By the law of cosines, 222 2 cos abc ab C   and 222 2 cos . acb ac B   Moreover, since the sum of the interior angles of triangle is , we have sin A  sin(()) BC   sin() BC sincosBC  cossinBC

222 2 abc h cab  

222 2 acb h acb 

22222 2 (2 ) h abc abccb  ah bc ah  sin. bcA 

Combining our results we have ahab  sin C, ahac  sin B, and ahbc  sin A. Dividing by abc gives sinsinsin law of sines A CB h bcacb 

62. By the law of sines, 3/2 sinsin 23 AB c  By Exercise 59 we know that 7. c  Thus 33 27 sin0.982. B 

63. From the figure at the right and the law of cosines,  222 22 1 2 22(2)cos 4424. b aaB aaaa  

Applying the law of sines to the figure, sinsin A B ab   2/23/2 3 2 ab ba    Thus, combining results, 22 24 aab 22 3 1 22 0 aa   2 24048 aaa   . From the quadratic formula and the fact that 0, a  we have 2 444(1)(8) 434 22 1.464. a  

64.

tan hh

tantantantan

tantantantan

tantan(tantan)

65. sin

66. (a) The graphs of sin y x  and y x  nearly coincide when x is near the origin (when the calculator is in radians mode).

(b) In degree mode, when x is near zero degrees the sine of x is much closer to zero than x itself. The curves look like intersecting straight lines near the origin when the calculator is in degree mode. 67. 2,2,,1 A

68. 11 22 ,2,1, ABCD 

69. 21 ,4,0, ABCD

71–74. Example CAS commands: Maple:

f :x-A*sin((2*Pi/B)*(x-C))D1; A:3; C:0; D1:0; f_list :[seq(f(x), B[1,3,2*Pi,5*Pi])]; plot(f_list, x-4*Pi..4*Pi, scalingconstrained, color[red,blue,green,cyan], linestyle[1,3,4,7],

legend["B1", "B3","B2*Pi","B3*Pi"], title"#71 (Section 1.3)");

Mathematica: Clear[a, b, c, d, f, x] f[x_]:a Sin[2/b(xc)]d Plot[f[x]/.{a3, b1, c0, d0},{x,4, 4}]

71. (a) The graph stretches horizontally.

(b) The period remains the same: period || B  . The graph has a horizontal shift of 1 2 period.

72. (a) The graph is shifted right C units.

(b) The graph is shifted left C units.

(c) A shift of  one period will produce no apparent shift. ||6 C 

73. (a) The graph shifts upwards || D units for 0. D  (b) The graph shifts down || D units for 0. D 

74. (a) The graph stretches || A units. (b) For 0, A  the graph is inverted.

1.4 GRAPHING WITH SOFTWARE

1–4. The most appropriate viewing window displays the maxima, minima, intercepts, and end behavior of the graphs and has little unused space.

1. d.
c. 3. d.
b.

5–30. For any display there are many appropriate display widows. The graphs given as answers in Exercises 5–30 are not unique in appearance.

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5. [2, 5] by [15, 40]
6. [4, 4] by [4, 4]
7. [2, 6] by [250, 50]
8. [1, 5] by [5, 30]
9. [4, 4] by [5, 5]
10. [2, 2] by [2, 8]
11. [2, 6] by [5, 4]
12. [4, 4] by [8, 8]
13. [1, 6] by [1, 4]
14. [1, 6] by [1, 5]
15. [3, 3] by [0, 10]
16. [1, 2] by [0, 1]
17. [10, 10] by [10, 10]
18. [5, 1] by [2, 4]
19. [4, 4] by [0, 3]
20. [5, 5] by [2, 2]

21. [10, 10] by [6, 6]

23. [6, 10] by [6, 6]

25. [0.03,0.03] by [1.25,1.25]

27. [300,300]by[1.25,1.25]

22. [5, 5] by [2, 2]

24. [3, 5] by [2, 10]

26. [0.1,0.1]by[3,3]

28. [50,50]by[0.1,0.1]

29. [0.25,0.25]by[0.3,0.3]

31. 22 244 x xyyy   2 228. xx  The lower half is produced by graphing 2 228.yxx 

30. [0.15,0.15]by[0.02,0.05]

32. 22 2 161116. yxyx    The upper branch is produced by graphing 2 116. y x 

33. 34.
35. 36.

CHAPTER 1 PRACTICE EXERCISES

1. The area is 2 A r  and the circumference is 2.Cr   Thus,  2 2 224 rACCC 

2. The surface area is 1/2 2 4 4. S Srr      The volume is 3 3 4 3 34 . V Vrr      Substitution into the formula for surface area gives  2/3 2 3 4 44. V Sr  

3. The coordinates of a point on the parabola are (x, x2). The angle of inclination  joining this point to the origin satisfies the equation 2 tan. x x x   Thus the point has coordinates 2 (,) xx  2 (tan,tan) 

4. rise run500 tan 500tanft h h 

Symmetric about the origin

Symmetric about the y-axis

Symmetric about the y-axis

16. ()()cos()cos(); yxxxxxyx  odd

17. Since f and g are odd ()() f xfx   and ()(). g xgx

(a) ()()()() f gxfxgx  [()] f x [()] gx  ()()()() f xgxfgxfg    is even.

(b) 3 ()()()() f xfxfxfx  [()] f x  [] f x [()] fx

(c) (sin())(sin()) fxfx (sin())fx  (sin()) f x is odd.

(d) (sec())(sec())(sec()) g xgxgx  is even.

(e) |()||()||()||| g xgxgxg   is even.

()()() f xfxfx  33 () f xf  is odd.

18. Let ()() f axfax  and define () g x  (). f xa  Then ()(()) g xfxa  ()() f axfax ()()()() f xagxgxfxa    is even.

19. (a) The function is defined for all values of x, so the domain is (,) 

(b) Since || x attains all nonnegative values, the range is [2,) 

20. (a) Since the square root requires 10 x  , the domain is (,1] 

(b) Since 1 x attains all nonnegative values, the range is [2,) 

21. (a) Since the square root requires 2 160, x  the domain is [4,4] .

(b) For values of x in the domain, 2 01616, x  so 2 0164. x  The range is [0,4]

22. (a) The function is defined for all values of x, so the domain is (,) 

(b) Since 32 x attains all positive values, the range is (1,) 

23. (a) The function is defined for all values of x, so the domain is (,)  .

(b) Since 2 x e attains all positive values, the range is (3,) 

24. (a) The function is equivalent to tan2, y x  so we require 2 2 k x   for odd integers k. The domain is given by 4 k x   for odd integers k

(b) Since the tangent function attains all values, the range is (,) 

25. (a) The function is defined for all values of x, so the domain is (,). 

(b) The sine function attains values from –1 to 1, so 22sin(3)2 x   and hence 32sin(3)11. x   The range is [3,1].

26. (a) The function is defined for all values of x, so the domain is (,). 

(b) The function is equivalent to 5 2 , yx  which attains all nonnegative values. The range is [0,) 

27. (a) The function is defined for all values of x, so the domain is (,). 

(b) The cosine function attains values from –1 to 1, so  1cos31 x  and hence  0cos312. x  The range is   0,2.

28. (a) The function is defined for all values of x, so the domain is (,).  (b) The cube root attains all real values, so the range is (,). 

29. 5(3)(1)yxx so the domain(,1][3,);  (3)(1)0 xx and can be any positive number, so the range(,5]. 

30. 2 2 3 4 2 x x y   so the domain(,);  2 2 3 4 03 x x   so the range[2,5). 

31.  1 4sin x y  so the domain(,0)(0,);  if 22 3 , x   then  1 1sin1, x  so the range[4,4]. 

32. 3cos4sin yxx  so the domain(,);  and 22 345  so  3 4 55 3cos4sin5cossin x xxx 5(coscossinsin )5cos(), x xx  where and 1cos()1 x   so the range[5,5]. 

33. (a) Increasing because volume increases as radius increases (b) Neither, since the greatest integer function is composed of horizontal (constant) line segments. (c) Decreasing because as the height increases, the atmospheric pressure decreases. (d) Increasing because the kinetic (motion) energy increases as the particles velocity increases.

34. (a) Increasing on [2,)  (b) Increasing on [ 1,) (c) Increasing on (,)  (d) Increasing on  1 2 ,   

35. (a) The function is defined for 44, x  so the domain is [ 4,4].

(b) The function is equivalent to ||,4yx 4, x  which attains values from 0 to 2 for x in the domain. The range is [0,2]

36. (a) The function is defined for 22, x  so the domain is [ 2,2].

(b) The range is [ 1,1]

37. First piece: Line through (0, 1) and (1, 0); 01 10 m  1 1 1

Second piece: Line through (1, 1) and (2, 0); m  01 21 1 1 1(1) yx

1,01 () 2,12 xx fx xx

38. First piece: Line through (0, 0) and (2, 5);

Second piece: Line through (2,

40. (a)

3 ()(1)((1))11 fgfgf  (0)202 f

(b) ()(2)((2))(22)(0) g ffggg

(c) ()()(())(2)2(2) ffxffxfxxx  

(d)

3 33 ()()(())111 ggxggxgxx

41. (a)

()()(())2 fgxfgxfx  

2 ()()(())(2) g fxgfxgx

(b) Domain of :[2,). fg  

(c) Range of :(,2]. fg   Domain of :[2,2]. gf  Range of :[0,2]. gf 

42. (a)

fgxfgxfx

()()(())1 g fxgfxgxx  

(b) Domain of :(,1] fg  

(c) Range of :[0,) fg   Domain of :[0,1] gf  Range of :[0,1] gf 

47.

The graph of 21()(||) fxfx  is the same as the graph of 1 ()fx to the right of the y-axis. The graph of 2 ()fx to the left of the y-axis is the reflection of 1 (),yfx  0 x  across the y-axis.

48.

Whenever 1 () g x is positive, the graph of y 

2 () g x 1 () g x  is the same as the graph of y 

1 (). g x When 1 () g x is negative, the graph of y 

2 () g x is the reflection of the graph of 1 ()ygx  across the x-axis.

It does not change the graph.

Whenever 1 () g x is positive, the graph of y 

2 () g x  1 |()| g x is the same as the graph of y 

1 (). g x When 1 () g x is negative, the graph of y 

2 () g x is the reflection of the graph of 1 ()ygx  across the x-axis.

49.

Whenever 1 () g x is positive, the graph of 21()|()|ygxgx  is the same as graph of 1 ().ygx  When 1 () g x is negative, the graph of 2 ()ygx  is the reflection of the graph of 1 ()ygx  across the x-axis.

50.

The graph of 21()(||) fxfx  is the same as the graph of 1 ()fx to the right of the y-axis. The graph of 2 ()fx to the left of the y-axis is the reflection of 1 (),0yfxx across the y-axis.

Copyright  2023 Pearson Education, Inc.

52.

The graph of 21()(||) fxfx  is the same as the graph of 1 ()fx to the right of the y-axis. The graph of 2 ()fx to the left of the y-axis is the reflection of 1 (),0yfxx across the y-axis.

53. (a) 1 2 (3)ygx (c) ()ygx  (e) 5()ygx

54. (a) Shift the graph of f right 5 units.

The graph of 21()(||) fxfx  is the same as the graph of 1 ()fx to the right of the y-axis. The graph of 2 ()fx to the left of the y-axis is the reflection of 1 (),0yfxx across the y-axis.

(b)  2 3 2 ygx

(d) ()ygx  (f ) (5)ygx 

(b) Horizontally compress the graph of f by a factor of 4.

(c) Horizontally compress the graph of f by a factor of 3 and then reflect the graph about the y-axis.

(d) Horizontally compress the graph of f by a factor of 2 and then shift the graph left 1 2 unit.

(e) Horizontally stretch the graph of f by a factor of 3 and then shift the graph down 4 units.

(f ) Vertically stretch the graph of f by a factor of 3, then reflect the graph about the x-axis, and finally shift the graph up 1 4 unit.

55. Reflect the graph of y x  about the x-axis followed by a horizontal compression by a factor of 1 2 , then shift left 2 units.

56. Reflect the graph of yx  about the x-axis, followed by a vertical compression of the graph by a factor of 3, then shift the graph up 1 unit.

57. Vertical compression of the graph of 2 1 x y  by a factor of 2, then shift the graph up 1 unit.

58. Reflect the graph of 1/3 yx  about the y-axis, then compress the graph horizontally by a factor of 5.

67. (a) tan tan bb BaaB    (b) sin sin aa AccA   

68. (a) sin a c A  (b) 22 sin cb a cc A 

69. Let h  height of vertical pole, and let b and c denote the distances of points B and C from the base of the pole, measured along the flat ground, respectively.

Then, tan50 h c  , tan35 h b  , and 10. bc

Thus, tan50 hc and tan35(10)hbc

tan35 tan50(10)tan35cc   (tan50tan35)10tan35 c   10tan35 tan50tan35 tan50 ch c        10tan35tan50 tan50tan35 16.98 m. 

70. Let h  height of balloon above ground. From the figure at the right, tan40 h a  , tan70 h b  , and 2 ab . Thus, tan70(2) hbha    tan70 and tan40 ha (2)tan70 a   tan40 a  (tan40tan70) a   2tan70   a  2tan70 tan40tan70   tan40 ha    2tan70tan40 tan40tan70   1.3 km. 

71. (a)

(b) The period appears to be 4.  (c) (4)sin(4) fxx   4 2 cos x    sin(2) x   22 cos2sincos x x x   since the period of sine and cosine is 2.  Thus, f (x) has period 4.  72. (a)

(b) Domain: (,0)(0,);  Range: [1,1]

(c) f is not periodic. For suppose f has period p. Then 

Choose k so large that 1 2 kp  

11 22 sin20 fkpf   for all integers k

11 1/(2) 0. kp

But then  1 2 fkp      1 (1/(2)) sin 0 kp    which is a contradiction. Thus f has no period, as claimed.

CHAPTER 1 ADDITIONAL AND ADVANCED EXERCISES

1. There are (infinitely) many such function pairs. For example, ()3 fxx  and ()4 g xx  satisfy (())(4)3(4)12 fgxfxxx  4(3) x  (3)(()). g xgfx 

2. Yes, there are many such function pairs. For example, if ()(23)3gxx and 1/3 () fxx  , then 3 ()()(())((23)) fgxfgxfx  31/3 ((23))23. xx

3. If f is odd and defined at x, then ()fx ().fx Thus ()()2 gxfx ()2fx whereas ()(()2)gxfx  ()2.fx  Then g cannot be odd because ()() gxgx   ()fx 2  ()fx  2 40,   which is a contradiction. Also, () g x is not even unless ()0fx  for all x. On the other hand, if f is even, then () g x  ()2fx is also even: ()()2 gxfx ()2(). fxgx 

4. If g is odd and g(0) is defined, then (0)(0)gg (0). g Therefore, 2(0)0(0)0 gg   

5. For (x, y) in the 1st quadrant, |||| x y  1 x  11 x yxy  . For (x, y) in the 2nd quadrant, |||| x y  x  1 x y  1 x  21.yx  In the 3rd quadrant, ||||1 x yx  1 xyx  21.yx In the 4th quadrant, |||| x y  1()1 x xyx  1. y  The graph is given at the right.

6. We use reasoning similar to Exercise 5.

(1) 1st quadrant: |||| yyxx  22. y xyx

(2) 2nd quadrant: |||| yyxx  2()00. yxxy 

(3) 3rd quadrant: |||| yyxx  ()yy 

()00xx  all points in the 3rd quadrant satisfy the equation.

(4) 4th quadrant: |||| yyxx  ()2 yyx  0. x 

Combining these results we have the graph given at the right.

7. (a) 222 sincos1sin x xx   2 1cos x  (1cos)(1cos) xx

sin 1cos x x 

(b) Using the definition of the tangent function and the double angle formulas, we have

8. The angles labeled  in the accompanying figure are equal since both angles subtend arc CD. Similarly, the two angles labeled α are equal since they both subtend arc AB. Thus, triangles AED and BEC are similar which implies 2cos acab bac

Copyright  2023 Pearson Education,

9. As in the proof of the law of sines of Section 1.3, Exercise 61, sinsin ahbcAabC  ac sin B the area of ABC   11 22 (base)(height) ah  111 222sinsinsin bcAabCacB  .

10. As in Section 1.3, Exercise 61, 2 (Area of ) ABC  22 1 4 (base)(height)  1122222 44 sin ahabC  222 1 4 (1cos) abC . By the law of cosines, 222 cab 2coscos abCC   222 2 . abc ab  Thus, 2222 1 4 (areaof)(1cos)

Therefore, the area of ABC equals ()()() s sasbsc

11. If f is even and odd, then ()() f xfx and ()()()() f xfxfxfx

for all x in the domain of f Thus 2()0()0. fxfx

12. (a) As suggested, let ()() ()(())()() 222 () () () fxfx fxfxfxfx Ex Ex ExE

 is an even function. Define ()() 2 ()()()() fxfx OxfxExfx   ()() 2 . f xfx Then ()() 2 () f xfx Ox

()()()() 22 () fxfxfxfx OxO    is an odd function ()()() f xExOx   is the sum of an even and an odd function. (b) Part (a) shows that ()()() f xExOx  is the sum of an even and an odd function. If also 11 ()()(), f xExOx  where E1 is even and O1 is odd, then ()()0fxfx 11 (()())(()()) ExOxExOx . Thus, ()Ex 11()()() ExOxOx  for all x in the domain of f (which is the same as the domain of 1EE and 1OO ). Now 1 ()() EEx ()Ex 1 ()Ex 1 ()() ExEx (since E and E1 are even) ()()11 EExEE  is even. Likewise, 11 ()()()() OOxOxOx  1 ()(())OxOx (since O and O1 are odd) 1 (()()) OxOx  1 () OO 1 () x OO  is odd. Therefore, 1EE and 1 OO are both even and odd so they must be zero at each x in the domain of f by Exercise 11. That is, 1 EE  and 1 ,OO  so the decomposition of f found in part (a) is unique.

(a) If 0 a  the graph is a parabola that opens upward. Increasing a causes a vertical stretching and a shift of the vertex toward the y-axis and upward. If 0 a  the graph is a parabola that opens downward. Decreasing a causes a vertical stretching and a shift of the vertex toward the y-axis and downward.

(b) If 0 a  the graph is a parabola that opens upward. If also 0, b  then increasing b causes a shift of the graph downward to the left; if 0, b  then decreasing b causes a shift of the graph downward and to the right.

If 0 a  the graph is a parabola that opens downward. If 0, b  increasing b shifts the graph upward to the right. If 0, b  decreasing b shifts the graph upward to the left.

(c) Changing c (for fixed a and b) by c shifts the graph upward c units if 0, c  and downward c units if 0. c 

14. (a) If 0, a  the graph rises to the right of the vertical line x b and falls to the left. If <0, a the graph falls to the right of the line x b and rises to the left. If 0 a  , the graph reduces to the horizontal line yc  As || a increases, the slope at any given point 0 x x  increases in magnitude and the graph becomes steeper. As || a decreases, the slope at 0x decreases in magnitude and the graph rises or falls more gradually.

(b) Increasing b shifts the graph to the left; decreasing b shifts it to the right.

(c) Increasing c shifts the graph upward; decreasing c shifts it downward.

15. Each of the triangles pictured has the same base (1sec) bvtv  . Moreover, the height of each triangle is the same value h. Thus 1 2 (base)(height) 1 2 bh  123A AA  … . In conclusion, the object sweeps out equal areas in each one second interval.

16. (a) Using the midpoint formula, the coordinates of P are 

00 2222,,. ab ab   Thus the slope of /2 /2 y bb x aa OP    (b) The slope of 0 0 b b aa AB  The line segments AB and OP are perpendicular when the product of their slopes is

1 bb aa 

a Thus, 22 baab    (since both are positive). Therefore, AB is perpendicular to OP when .ab 

.

17. From the figure we see that 2 0    and 1. ABAD From trigonometry we have the following: sin , EB AB EB   cos , AE AB AE   tan , CD AD CD   and sin cos tan . EB AE     We can see that: area AEB  area sector  DB  area 2 11 22 ()()() ADCAEEBAD     1 2 () AD () CD 2 111 222 sincos(1)(1)(tan)     sin 111 222cos sincos   

18. ()()(())() f gxfgxacxdb   and()()(()) acxadbgfxgfx  () caxbdacxcbd  Thus ()()()() f gxgfxacxadb     acxbcdadbbcd    Note that () f dadb  and (), g bcbd  thus ()()()() if ()(). f gxgfxfdgb 

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