SECTION 14.8 LAGRANGE MULTIPLIERS 0 231 the possible points are ( ±-/2, ± 7:i, 72), ( ±V-2, ±~, - );) . Hence the maximum off subject to the constraints is f(±J2,±~,±jz ) = ~ andtheminimumisf(±J2,±~, 'f72) = ~· Note: Since xy = 1 is one of the constraints we could have solv<strong>ed</strong> the problem by solving f (y, z) = yz + 1 subject to y2 + z2 = 1. 19. f(x, y) = x 2 + y 2 + 4x - 4y. For the interior of the region, we find the critical points: fx = 2x + 4, f u = 2y - 4, so the only-critical point is ( - 2, 2) (which is inside the region) and f ( - 2, 2) = -8. For the boundary, we use Lagrange multipliers. g(x, y) = x 2 + y 2 = 9, so "iJ f = >. "ilg =;. (2x + 4, 2y - 4) = (2>.x, 2>.y). Thus 2x + 4 = 2>.x and 2y - 4 = 2>.y. Adding the two equations gives 2x + 2y = 2>.x + 2>.y =:. x + y = >.(x + y) =:. (x + y)(>.- 1) = 0, so x + y = 0 =;. y = -x or>. - 1 = 0 =;. >. = 1. But >. = 1 leads to a contradition in 2x + 4 = 2>.x, soy = - x and x 2 + y 2 = 9 implies 2y 2 = 9 => y = ±12. We have f ( ~· -72) = 9 + 12-/2 ~ 25.97 and r( - 12, ~ ) = 9- 12-/2 ~ - 7.97, so the maximum value off on the disk x 2 ~ y 2 :s: 9 is f ( 72· -12) = 9 + 12-/2 and the minimum is f( - 2, 2) = -8. 21. f(x, y) = e- xy. For the interior ofthe region, we find the critical points: f x = - ye-xu, / 11 = -xe-"'Y, so the only critical point is (0, 0), and f(O, 0) = 1. For the boundary, we use Lagrange multipliers. g(x, y) = x 2 + 4y 2 = 1 =;. >. "iJ g = (2>.x, 8>.y), so setting "iJ f = >. "iJ g we get -ye-"' 11 = 2>.x and -xe-"' 11 = 8>.y. The first of these gives e- "' 11 = -2>.xjy, and then .the second gives - x( - 2>.xjy) = 8>.y => x 2 = 4y 2 • Solving this last equation with.the constraint x 2 + 4y 2 = 1 gives X= ±72 and y=±~ . Now t( ±~, 'f 2~) = e 1 1 4 ~ 1.284 and f ( ±~ , ±;~ ) = e- 1 / 4 ~ 0.779. The former arc the maxima on the region and the latter are the min.ima. 23. (a) f(x, y) = x , g(x,y) = y 2 + x 4 - x 3 == 0 =;. "ilf = (1, 0) = >.Vg = >.(4x 3 - 3x 2 ,2y). Then 1 = >.( 4x 3 - 3x 2 ) (1) and 0 = 2>.y (2). We have >. i= 0 from (1), so (2) gives y = 0. Then, from the constraint equation, x 4 - x 3 =. 0 =;. x 3 (3; - 1) = 0 =;. x = 0 or x = 1. But x = 0 contradicts (1), so the only possible extreme value subject to the constraint is /(1, 0) = 1. (The question remains whether this is inde<strong>ed</strong> the minimum of f.) (b) The constraint is y 2 + x 4 - x 3 = 0 ¢} y 2 = x 3 - x 4 . The left side is non-negative, so we must have x 3 - x 4 :2: 0 which is true only for 0 :S: x :S: 1. Therefore the minimum possible value for f(x, y) =x is 0 which occurs for x = y = 0. However,>. "iJ g(O, 0) = >. (0- 0, 0) = (0, 0) and "iJ f(O, 0) = (1, 0), so "iJ f(O, 0) # >. "iJ g(O, 0) for all values of>.. (c) Here "iJ g(O, 0) = 0 but the method of Lagrange multipliers requires that "iJ g # 0 everywhere on the constraint curve. © 20 12 Ccngagc Lcruning. All Rights Reserv<strong>ed</strong>. May not be scann<strong>ed</strong>, copicc.l, or duplicat<strong>ed</strong>, or post<strong>ed</strong> to a publicly accessible website. in whole or in p:m.
232 D CHAPTER 14 PARTIAL DERIVATIVES 25. P(L,K)=bLo.Kl-o., g(L,K)=mL+nK=p '* 'VP=(abLo:- 1 K 1 - o.,(1-a)bL'""JC'""), >..'Vg=(>..m, >..n). Then ab(K/ L) 1 -o. = >..m and (1- a)b(L/ K)"' =>..nand mL + nK = p, so ab(K/ L?-"'/m = (1 - a)b(L/ K) 0 /n or naj[m(1-a)]= (L/ K)"'(L/ K) 1 -"'. or L = Kno/[m{1- a)]. Substituting into mL + nK = p gives K = (1- a)pjn and L = apjm for the maximum production. 27. Let the sides of the rectangle be x andy. Then f(x, y) = xy, g(x, y) = 2x + 2y = p '* 'V f(x, y) = (y, x)·, >.. 'Vg = (2>.., 2>..). Then A= ~y = ~x i~pli es x = y and the rectangle with maximum area is a square with side length iP· 29. The distance from {2,0, - 3) to a point (x,y,z) on the plane is d = .j(x- 2)2 + y 2 + (z + 3) 2 , so we seek to minimize d 2 = f(x, y, z) = (x- 2) 2 + y 2 + (z + 3) 2 subject to the constraint that (x, y, z) lies on the plane x + y + z = 1, that is, that g(x, y, z) = x + y + z = 1. Then 'V f =A 'Vg =* (2(x- 2), 2y, 2(z + 3)) = (A, .A, .A), sox= (A+ 4)/2, y = >./2, z = (>.. - 6)/2. Substituting into the constraint equation gives .A~ 4 + i + A; 6 = 1 >.. = ~ . sox = ~. y = ~.and z = -i· This must correspond to a minimum, so the shortest distance is d = J ( ~ - 2) ~ · + ( ~ )2 + (- i + 3) 2 = ..fi = ~ - '* 3A- 2 = 2 '* 31. Let f(x, y , z) = d 2 = (x- 4) 2 + (y- 2) 2 + z 2 • Then we want to minimize f subject to the constraint g (x,y,z) = x 2 +y 2 - z 2 = 0. 'Vf = )..'\Jg '* (2 (x --; 4) ,2(y- 2) ,2z) = (2>..x,2>..y, -2-Xz), sox- 4 = J..x, y - 2 = .Ay, and z = -J..z. From the last equation we have z + >..z = 0 '* z (1 +.A) = 0, so either z = 0 or>..= -1. But from the constraint equation we have z = 0 '* x 2 + y 2 = 0 '* x = y = 0 which is not possible from the first two equations. So ).. = - 1 and x - 4 = >..x '* x = 2, y - 2 = >..y '* y = 1, and x·2 + y 2 - z 2 = 0 '* 4 + 1 - z 2 = 0 '* z = ±v'S. This must correspond to a minimum, so the points on the cone closest to ( 4, 2, 0) are (2, 1, ±v'S).' 33. f(x,y,z) = xyz,g(x,y,z) = x +y + z = 100 =* 'Vf = (yz,xz, xy) = )..'\Jg =(>.., >..,>..). Then>.. = yz = xz = xy implies x = y = z = 1 ~ 0 . 35. If the dimensions are 2x, 2y, and 2z, then maximize f(x, y, z) = (2x)(2y)(2z) = 8xyz subject to g(x, y, z) := x 2 + y 2 + z 2 = r 2 (x > 0, y > 0, z > 0). Then 'V f = .A 'V g '* (8yz, Bxz, 8xy) = .A (2x, 2y, 2z) =* 41JZ 4xz 4xy . . 2 2 2 2 8yz = 2-Xx, Bxz = 2>.y, and 8xy = 2.Xz, so>.= - ·- = - = - .This gives x z = y z '* x = y (since z t= D) X Y Z ' and xy 2 = xz 2 '* z 2 = y 2 , so x 2 = y 2 = z 2 '* x = y = z, and substituting into the constraint equation gives 3x 2 = r 2 '* x = r/../3 = y = z. Thus the largest <strong>vol</strong>ume of such a box is . f ( ~, ~, ~ ) = 8 ( ~) ( 7J) ( ~) = 3 ~ r 3 . ' © 2012 Cengage Learning. All Rights Reserv<strong>ed</strong>. May nor be scnruu.xJ. copi<strong>ed</strong>, or duplicatC"d. or postctl to u publicly ucccssiblc website. in whole or in purt.
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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 10.4 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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0 PROBLEMS PLUS l lt sin u dx cost
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11 . D INFINITE SEQUENCES AND SERIE
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SECTION 11.3 THE INTEGRAL TEST AND
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17 lim I an+l I= SECTION 11.7 STRAT
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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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49./- 1 - dx = -ln{4- x) + C and 4-
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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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5. f~(t 2 i +tcos 1rtj +sin 1rt k )
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(b) The wedge in question is the sh
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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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SECTION 16.6 PARAMETRIC SURFACES AN
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that is, D = {( x, y) I x 2 + y 2 :
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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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350 0 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