SECTION 14.7 MAXIMUM AND MINIMUM VALUES 0 225 local minima, !(0.170, - 1.215) ::::: 3.197 is a local maximum, and ( -1.301, -1.215), (0.170, 0.549), and (1.131, -1.215) are saddle points. There is no highest or lowest point on the graph. 3 z 29. Since f is a polynomial it is contint,Jous on D, so an absolute maximum and minimum exist. Here f x = 2x- 2, jy = 2y, and setting fx = jy = 0 gives (1, 0) as the only critical point (which is inside D), where f (1, 0) = - 1. Along £ 1 : x = 0 and f(O, y) = y 2 for -2 ~ y ::=:; 2, a quadratic function which attains its minimum at y = b, where f(O, 0) = 0, and its maximum ·aty = ±2, wheref(0,±2) = 4. Along £2: y = x- 2 forO ::=:; x ~ 2, and f(x,x- 2) = 2x 2 - 6x + 4 = 2 (x _ ~) 2 _ ~ . a quadratic which attains its minimum at x = £, where f ( ~, - ~) = - ~, and its maximum at x = 0, where f ( 0, - 2) = 4. Along £3: y = 2 - x for 0 ~ x ::::; 2, and f(x, 2- x) = 2x 2 - 6x + 4 = 2(x- ~) 2 - ~.a quadratic which attains its minimum at x =~~where f(~, ~) =-~,and its maximum at x = 0, where f (O, 2) = 4. Thus the absolute maximum off on D is f(O, ±2) = 4 and the absolute minimum is !(1, 0) = -1. y (0,2) L, (0, - 2) (2,0) X 31. f x(x,y) = 2x +2xy, jy(x,y) = 2y +x 2 , and setting f.,= f" = 0 gives (0, 0) as the only critical point in D , with .f(O, 0) = 4. On £ 1: y = -1, j(x, - 1) = 5, a constant. On £2: x = 1, /(1, y) = y 2 + 11 + 5, a quadratic in y which attains its maximum at (1, 1), /(1, 1) = 7 and its minimum at (1, - ~) , f(1, - t) =.!f. On £ 3: f(x, 1) = 2x 2 + 5 which attains its maximum at (-1, 1) and (1, 1) with f(±l , 1) = 7 and its minimum at (0, 1), f(O, 1) = 5. (-1, 1) L• (-1,-1) y L, (I, I) L2 0 L, (1,-1) X © 2012 Ccngagc Learning. AU Rights Reserv<strong>ed</strong>. Mny not be scann<strong>ed</strong>, copi<strong>ed</strong>, or duplicat<strong>ed</strong>. or JlOsh.:t.l to n publicly ncccssiblc website, in whole or in part.
226 D CHAPTER 14 PARTIAL DERIVATIVES On .i4 : f( -1, y) = y 2 + y + 5 with maximum at ( -1, 1 ), f( - 1, 1) = 7 and minimum at ( -1, -D. f( - 1, -~) = Jf. Thus the absolute maximum is attain<strong>ed</strong> at both (±1, 1) with /(±1, 1) = 7 and the absolute minimum on Dis attain<strong>ed</strong> at (0, 0) with f(O, 0) = 4. 33. f(x, y) = x 4 +y 4 - 4xy + 2 is a polynomial and hence continuous on D, so Y it has an absolute maximum and minimum on D. fx(x, y) = 4x 3 - 4y and (0, 2)+---L--'3'-------1(3, 2) . fv(x, y) = ·4y 3 - 4x; then f x = 0 implies y = x 3 , and substitution into fv = 0 => x = y 3 gives x 9 - x = 0 => x(x 8 - 1) = 0 => x = 0 or x = ±1. Thus the critical points are -(0, 0), (1, 1), and ( - 1, - 1), but only (0,0) (3,0) X (1, 1) with f(1, 1) = 0 is inside D . On £1: y = 0, f(x, 0) = x 4 + 2, 0 ~ x ~ 3, a polynomial in x which attains its maximum at x = 3, !(3, 0) = 83, and its minimum at x = 0, f (O, 0) = 2. On £ 2 : x = 3, /(3, y) = y 4 - 12y + 83, 0 ~ y ~ 2, a polynomial in y which attains its minimum at y = {/3, /(3, {13) = 83- 9 .{/3 ~ 70.0, and its maximum at y = 0, ! (3, 0) = 83. On L 3 : y = 2, f(x, 2) = x 4 - Bx + 18, 0 ~ x ~ 3, a polynomial in x which attains its minimum at x = q'2, f( q'2, 2) = is- 6 ij2 ~ 10.4, and its maximum at x = 3, /(3, 2) = 75. On £ 4: x = 0, f(O, y) = y 4 + 2, 0 ~ y ~ 2, a polynomial in y which attains its maximum at y = 2, f(O , 2) = 18, and its minimum at y = 0, f(O, 0) = 2. Thus the absolute maximum off on Dis /(3, 0) = 83 and the absolute minimum is /(1, 1) = 0. 35. f,(x, y) = 6x 2 and fv(x, y) = 4y 3 • And so f x = 0 and fv = 0 only occur when x = y = 0. Hence, the only critical point .inside the disk is at x = y :::o 0 where /(0, 0) = 0. Now on the circle x 2 + y 2 = 1, y 2 = 1 - x 2 so let g(x) = f(x, y) =·2x 3 + (1- x 2 ) 2 = .x 4 + 2x 3 - 2x 2 + 1,-1 ~ x ~ 1. Then g'(x) = 4x 3 + 6x 2 - 4~ = 0 => x = 0, -2, or ~ - /(0,±1) = g(~) = 1, !(~, ±1 ) = g(~) = ~· and ,(-2,-3) is not in D. Checking the endpoints, we get .f( -1, 0) = g( -1) = -2 and f(1 , 0) = g(1) = 2. Thus the absolute maximum and minimum off on Dare /(1, 0) = 2 and f(- 1,0) = - 2. Another method: On the boundary x 2 + y 2 = 1 we can write x = cos (;I, y = sin 8, so f (cos 8, sin 8) = 2 cos 3 8 + sin 4 (;I, 0 ~ () ~ 27T. 37. f(x, y) = - (x 2 - 1) 2 - (x 2 y- x - 1) 2 => f,(x, y) = - 2(x 2 - 1)(2x) - 2(x 2 y- x - 1)(2xy- 1) and jy(X, y) = -2(x 2 y- x - 1)x 2 . Setting j y(x, y) = 0 gives either x = 0 or x 2 y - x- 1 = 0. There are no critical points for x = O,.since f:.,(O, y) = .:_2, so we set x 2 y - x- 1 = 0 {:} y = x ~ 1 [x =/= 0], X so f, ( x, x~ 1 ) = ·-2(x 2 - 1){2x)- 2(x 2 x ~ 1 - x - 1) (2x x ~ 1 - 1) = -4x(x 2 - 1). Therefore f,(x, y) = fv(x, y)- = 0 at the points (1, 2) and ( -1, 0). To classifY these critical points, we calculate ® 2012 Cc.ngage Learning. All Rights Rescrvcc.l. MilY not be scann<strong>ed</strong>, copi<strong>ed</strong>, or duplicat<strong>ed</strong>, or postcd'1o n publicly occcssiblo \\'Cb~ite, in \\'hole or in part.
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- STUDENT SOLUTIONS MANUAL for STEW
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.. BROOKS/COLE ~ I ~~r CENGAGE Lear
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D ABBREVIATIONS AND SYMBOLS CD cu D
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viii o CONTENTS 12.4 The Cross Prod
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10 D PARAMETRIC EQUATIONS AND POLAR
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SECTION 10.1 CURVES DEFINED BY PARA
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SECTION 10.1 CURVES DEFINED BY PARA
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SECTION 10.2 CALCULUS WITH PARAMETR
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SECTION 10.2 CALCULUS WITH PARAMETR
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SECTION 10.2 CALCULUS WITH PARAMETR
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SECTION 10.3 POLAR COORDINATES 0 13
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SECTION 10.3 POLAR COORDINATES 0 17
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SECTION 10 .~ POLAR COORDINATES 0 1
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SECTION 10.4 A~~S AND LENGTHS IN PO
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SECTION 10.4 AREAS AND LENGTHS IN P
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SECTION 10.4 AREAS AND LENGTHS IN P
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SECTION 10.5 CONIC SECTIONS 0 27 5.
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SECTION 10.5 CONIC SECTIONS 0 29 35
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x2 y2 y2 a:2 _ a2 b 61. ;_2 - - = 1
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SECTION 10.6 CONIC SECTIONS IN POLA
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CHAPTER 10 REVIEW 0 35 the length o
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CHAPTER 10 REVIEW 0 37 EXERCISES 1.
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CHAPTER 10 REVIEW 0 39 25. x = t +
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CHAPTER 10 REVIEW 0 41 2 2 . 45. ~
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0 PROBLEMS PLUS l lt sin u dx cost
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11 . D INFINITE SEQUENCES AND SERIE
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SECTION 11.1 SEQUENCES 0 47 35. a,.
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SECTION 11.1 SEQUENCES D 49 71. Sin
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SECTION 11.2 SERIES 0 51 ak+l- a1.:
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SECTION 11.3 THE INTEGRAL TEST AND
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SECTION 11.4 THE COMPARISON TESTS D
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SECTION 11.6 ABSOLUTE CONVERGENCE A
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17 lim I an+l I= SECTION 11.7 STRAT
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SECTION 11.8 POWER SERIES 0 n (b) I
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SECTION 11.9 REPRESENTATIONS OF FUN
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SECTION 11.9 REPRESENTATIONS OF FUN
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SECTION 11.10 TAYLOR AND MACLAURIN
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SECTION 11.10 TAYLOR AND MACLAURIN
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SECTION 11.10 TAYLOR AND MACLAURIN
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61 _ x_ x · sin x - x- tx 3 + 1~
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SECTION 11.11 APPLICATIONS OF TAYLO
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CHAPTER 11 REVIEW 0 97 J'(xn)(xn -
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49./- 1 - dx = -ln{4- x) + C and 4-
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D PROBLEMS PLUS 1. It would be far
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112 0 CHAPTER 12 VECTORS AND THE GE
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D PROBLEMS PLUS 1. Since three-dime
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13 D VECTOR FUNCTIONS 13.1 Vector F
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SECTION 13.1 VECTOR FUNCTIONS AND S
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SECTION 15.8 TRIPLE INTEGRALS IN CY
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M xv = I~1f I: I:2 6 - 3 r 2 (zK) r
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(b) The wedge in question is the sh
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CHAPTER 15 REVIEW 0 289 15 Review C
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300 0 CHAPTER 15 PROBLEMS PLUS 13.
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16 0 VECTOR CALCULUS 16.1 Vector Fi
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SECTION 16.6 PARAMETRIC SURFACES AN
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SECTION 16.6 PARAMETRIC SURFACES AN
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that is, D = {( x, y) I x 2 + y 2 :
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SECTION 16.7 SURFACE INTEGRALS 0 32
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SECTION 16.8 STOKES' THEOREM 0 333
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dS SECTION 16.9 THE DIVERGENCE THEO
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CHAPTER 16 REVIEW 0 337 27. JI 5 cu
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CHAPTER 16 REVIEW 0 339 TRUE-FALSE
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CHAPTER 16 REVIEW D 341 Alternate s
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344 0 CHAPTER 16 PROBLEMS PLUS Simi
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3.c6 0 CHAPTER 17 SECOND-ORDER DIFF
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348 0 CHAPTER 17 SECOND-ORDER DIFFE
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352 D CHAPTER 17 SECOND-ORDER DIFFE
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0 APPENDIX Appendix H Complex Numbe
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APPENDIX H COMPLEX NUMBERS 0 361 43