SECTION 14.7 MAXIMUM AND MINIMUM VAL4ES 0 227 f :u:(x, y) = - 12x 2 - 12x 2 y 2 + 12xy + 4y + 2, fvv(x, y) = - 2x", and f zv(x, y) = -8x 3 y + 6x 2 + 4x. In order to use the Second Derivatives Test we calculate - I Of-----1~ D(-1,0) = fxx(-1, 0) / 7171 (-1,0) - [f:c 71 (- 1 , 0)] ~ = 16 > 0, -2 / :r:c ( - 1, 0) = -10 < 0, D (1, 2) = 16 > 0, and f:r:c{1, 2) = -26 < 0, so both ( -1, 0) and (1, 2) give local maxima. X 39. Let d be the distance fr~m {2, 0, -3) to any point (x, y, z ) on the plane x + y + z = 1, sod= J(x - 2) 2 + y 2 + (z + 3)2 where z = 1-x- y, and we minimize d 2 ~ f(x, y) = (x - 2) 2 + y 2 + {4 - x- y) 2 • Then j;,(x,y) = 2(x- 2) + 2{4- x - y)( -1) = 4x + 2y -12, f 71 (x,y) = 2y + 2(4 - x- y){-1) = 2x + 4y - 8. Solving 4x + 2y- 12 = 0 and 2x + 4y- 8 = 0 simultaneously gives x = ~. y = ~.so the only critical point is(~,~). An absolute minimum exists (since there is a minimum di.stance from the point to the plane) and it must occur at a critical point, so the shortest distance occurs for x = ~. y = ~ for which d = J (~ - 2) 2 + (j) 2 + (4 - ~ - ~) 2 = ji = ~- 41. Let d be the distance from the point {4, 2, 0) to any point {x, y, z) on the cone, sod = ,j(x - 4)2 + (y- 2)2 + z2 where z 2 = x 2 + y 2 , and we minimize d 2 = (x - 4) 2 + (y - 2) 2 + x 2 + y 2 = f(x, y). Then fz(x, y) = 2 (x - 4) + 2x = 4x - 8, f 71 (x, y) = 2 (y - 2) + 2y = 4y- 4, and the critical points occur when f., = 0 => x = 2, fu = 0 => y = 1. Thus the only critical point is (2, 1). An absolute minimum exists (since there is a minimum distance from the cone to the point) which must occur at a critical point, so the points on the cone closest to ( 4, 2, 0) are (2, 1, ±v'5). 43. x + y + z = 100, so maximize f(x, y) = xy(l OO - x- y). f x = 100y- 2xy- y 2 , f 71 = 100x - x 2 - 2xy, f,:r. = - 2y, f vu = -2x, fxv = 100-2x- 2y. Then J,r; = 0 implies y = 0 or y = 100- 2x. Substituting y = 0 into fv = 0 gives x = 0 or x = 100 and substi~ting y = 100 - 2x into fv = 0 gives 3x 2 - 100x = 0 sox = 0 or 1 ~ . Thus the critical points are (0, 0), (100, 0), (0, 100) and ( 1 ~ 0 , D(O, 0) = D{100, 0) = D {O, 100) = -10,000 while D(1~ 0 , 1 ~ 0 ) = 10·~ 00 and f xx (1~ 0 , 1 ~ 0 ) = - 2 ~ < 0. Thus (0, 0), (100, 0) and {0, 100) are saddle points whereas f( 1 ~ 0 , 1 ~ 0 ) is a local maximum. Thus the numbers are x = y = z = 1 ~ 0 . 45. Center the sphere at the origin so that its equation is x 2 + y 2 + z 2 = 1·2 , and orient the inscrib<strong>ed</strong> rectangular box so that its <strong>ed</strong>ges are parallel to the coordinate axes. Any vertex of the box satisfies x 2 + y 2 + z 2 = r 2 , so take (x, y, z) to be the vertex 1 ~ 0 ) . in the fi rst octant. Then the box has length 2x, width 2y, and height 2z = 2 ,jr 2 - x 2 - y 2 with <strong>vol</strong>ume given by V(x, y) = (2x)(2y)(2 Jr 2 - x 2 - y 2 ) = 8xy Jr 2 - x 2 - y 2 forO < x < r, 0 < y < r. Then 8y(r 2 - 2x 2 - y 2 ) 8x(r 2 - x 2 - 2y 2 ) ,j r2 _ x2 _ y2 . J r2 _ x2 _ y2 V., = (Bxy) . ~(r2- x2- y2)-1f2( -2x) + ,jr2 - x2 - y2. By= . ·and Vv = . Setting Vx = 0 gives y = 0 or 2x 2 + y 2 = r 2 , but y > 0 so only the latter solution applies. Similarly, V 71 = 0 with x > 0 © 201 2 Ccngoge lcruniny. All Rights Rcscn"Cd. May nol be scwliiCd. copi<strong>ed</strong>. or duplical<strong>ed</strong>. or post<strong>ed</strong> loa publicly accessible website, in \\bole or in pn.
228 0 CHAPTER 14 PARTIAL DERIVATIVES implies x 2 + 2y 2 = r 2 . Substituting, we have 2x 2 + y 2 = x 2 + 2y 2 ::::> x 2 = y 2 ::::> y = x. Then x 2 + 2y 2 = r 2 '* 3x 2 = r 2 ::::> x = .jr"i]3 = r I vf3 = y. Thus the oni,Y critical point is (r I vf3, r I ,/3). There must be a maximum <strong>vol</strong>ume and here it must occur at a critical point, so the maximum <strong>vol</strong>ume occurs when x = y = r 1 V3 and the maximum .47. Maximize f(x, y) = x; (6-x- 2y), then the maximum <strong>vol</strong>ume is V = xyz. f., = i(6y ~ 2xy- y 2 ) = h(6- 2x- 2y) and fv = ~x (6 - x - 4y). Setting fx =:= 0 and j 11 = 0 gives the critical point (2, 1} which geometrically must give a maximum. Thus the <strong>vol</strong>ume of the largest such box is V = (2)(1) ( ~) = t· 49. Let the dimensions be x, y, and z; then 4x + 4y + 4z = c and the <strong>vol</strong>ume is V = xyz = xv(ic- x - y) = ic:cy- x 2 y - xy 2 , x > 0, y > 0. Then V, = ~cy- 2xy- y 2 and Vy = ~ex- x 2 - 2xy, so Vx = 0 = Vy when 2x + y = ic and x + 2y =~c. Solving, we get x =f-ie, y = 1 12 c and z = ic- x- y = f-ie. From the geometrical nature of the ·problem, this critical point must give an absolute maximum. Thus the box is a cube with <strong>ed</strong>ge length -f2c. 51. Let the dimensions be x, y and z, then minimize xy + 2(xz + yz) if xyz = 32,000 cm 3 • Then f(x,y) = xy + [64,000(x + y)fxy] = xy + 64,000(x- 1 + y- 1 ), fx = y- 64,000x- 2 , fv = x- 64,000y- 2 . And fx = 0 implies y = 64,000/x 2 ; substituting into /y = 0 implies x 3 = 64,000 or x = 40 and then y = 40. Now D(x, y) = [(2)(64,000Wx - 3 y- 3 - dimensions of the box are x = y = 40 em, z = 20 em. 1 > 0 for ( 40, 40) and 'f.,, ( 40, 40) > 0 so this is inde<strong>ed</strong> a minimum. Thus the 53. Let x, y, z be the dimensions of the rectangular box. Then the <strong>vol</strong>ume of the box is xyz and' L = J xz + y2 + z2 ::::> L 2 = x 2 + y 2 + z 2 ::::> z = J L 2 - x 2 - y 2 . Substituting, we have <strong>vol</strong>ume V(x,y) = xy JL2- x 2 - y 2 (x,y > 0). 2 Vy = xJL2 -x 2 -y 2 - xy . V., =Oimpliesy(L 2 - x 2 -y 2 )=x 2 y JP - x2 - y2 ::::> y(L 2 -2x 2 -y 2 ) =0 ::::> 2x 2 + y 2 = L 2 (since y > 0), and v; 1 = o ·implies x(L 2 - x 2 - y 2 ) = xy 2 ::::> x(L 2 - x 2 - 2y 2 ) = 0 ::::> x 2 + 2y 2 = L 2 (since x > 0). Substituting y 2 = L 2 - 2x 2 into x 2 + 2y 2 = L 2 gives x 2 + 2L 2 - 4x 2 = L 2 ::::> 3x 2 = L 2 ::::> x = L/vf3 (since x > 0) f!nd then y = J L2- 2(L/vf3) 2 = L/vf3. So the only critical point is (Lf,/3, Llvf3 ) which, from th~ geometrical nature of the problem, must give an absolute maximum. Thus th~ maximum <strong>vol</strong>ume is V(LI,/3, Ll,/3) = (LI,/3) 2 j L2- (Livf3) 2 - (LI ,/3) 2 = L 3 I (3 ,/3) cubic units. © 2012 Cen,SD.Gc Learning. All Rir)lts Rcsco·cd. May not be scann<strong>ed</strong>. copi<strong>ed</strong>. or duplicaLCd, or poster.! to a publicly accessible website, in whole or in pnrt.
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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 10.2 CALCULUS WITH PARAMETR
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x2 y2 y2 a:2 _ a2 b 61. ;_2 - - = 1
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11 . D INFINITE SEQUENCES AND SERIE
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61 _ x_ x · sin x - x- tx 3 + 1~
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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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0 APPENDIX Appendix H Complex Numbe
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APPENDIX H COMPLEX NUMBERS 0 361 43