SECTION 14.6 DIRECTIONAL DERIVATIVES AND THE GRADIENT VECTOR 0 215 17. h(r, s, t) = ln(37· + 6s + 9t) => 'ilh(r, s, t) = (3/(3r + 6s + 9t), 6/(3r + 6s + 9t), 9/(3r + 6s + 9t)), 'ilh(1, 1, 1) = (k, ft, ~ ), and a unit vector in the direction ofv = 4 i + 12j + 6 k is u = .; 16 +; 4 4+3& (4i + 12j + 6k) = ~ i .+ ~ j + ~ k, so ( ) ' 'il f(x, y) = (Hxy)- 1 1 2 (y), Hxy)- 112 (x)) = / yt=' ~) ·so 'il!(2, 8) = (1, ~ -- ). \2 yxy 2 yxy . . The unit vector in the direction of PQ = (5 - 2, 4 - 8) = (3, -4) is u = ( ~, - ~ ), so Duf(2,8)='il/(2,8)· . u= ( 1,4)· 1 (35•-6")- -5. 2 21. f(~,y) = 4yy'X => 'ilf(x,y) = ( 4y · ~x - 1 1 2 ,4v'x) = (2yjy'x,4.,fi).' · 'il f(4, 1) = {1, 8) is.the direction of maximum rat~ ofch~ge, and the maximum rate is·/'il /(4, 1)/ = v'1 + 64 = v'65. 23. J(x, y) = sin(xy) => 'il f(x, y) = (y cos(xy), x cos(xy)), 'il!(1, 0) = (0, 1). Thus the maximum rate of change is /'il f(1, 0)/ = 1 in the direction {0, 1). 25. f(x,y,z) = Jx2 + y2 + .z2 => 'il f(3, 6, -2) = ( -7,w. ~· ~) = ( ~. ¥, -¥ ). Th~ s the maximum rate ofchange is 27. (a) As in the proof of Theorem 15, Du f = /'il!I cos 0. Since the minimum value of cos(} is - 1 occurring when(} = 11', the minimum value of Du f is - /'il f/ occurring when(} = 11', that is when u is in the opposite direction of 'il f. (assuming \7 f "f 0). (b) f(x, y) = x 4 y - x 2 y 3 => 'il f(x, y) = ( 4x 3 y - 2xy 3 , x 4 - 3x 2 y 2 ), so f decreases fastest at the point (2, -3) in the direction-'il /(2, - 3) = - {12, -92) = (-12, 92). 29. The directionoffastestchange is 'ilf(x,y) = (2x- 2) i + (2y- 4)j , so we ne<strong>ed</strong> to find all points (x,y) where 'ilf(x,y) is parallel to i + j ¢'> (2x - 2) i + (2y - 4)j = k (i + j) ¢'> k = 2x- 2 and k = 2y - 4. Then 2x- 2 = 2y- 4 => y = x + 1, so the direction of fastest change is i + j at all points on the line y = x + 1. ® 2012 Ccngt~gc Lcnming. All Rights Rcscn·ccJ. M11y not be scann<strong>ed</strong>, copk-c.J, or duplico.tcd. or postl"li lou publicly occcssiblc wcbsilc, in whole or in pan.
216 0 CHAPTER 14 PARTIAL DERIVATIVES k Jx2 + y2 +z2 3 31. T = and 120 = T(1, 2, 2) = - so k = 360. k ( ) - (1, - 1, 1) au- v'3 , DuT(1, 2, 2) = 'VT(1, 2, 2) · u = [ .:._360( x 2 + y 2 + z 2 ) -S/ 2 (x, y, z)] . u = - .12 3 (1, 2, 2). -4.. (1, -1, 1) = -~ . . {1,2,2) v3 3v3 (b) From (a), 'VT = -360(x 2 + y 2 + z 2 ) - S/ 2 (x, y, z), and since (x, y, z) is the position vector of the point (x, y, z), the vector - (x, y, z), and thus 'VT, always points toward the origin. 33. 'VV(x, Y •. z) = (lOx- 3y + yz, xz - 3x, xy), 'VV(3, 4, 5) = (38, 6, 12) {a) Du V(3,4,5) = {38, 6, 12} · ~(1, 1, -1} = '7a (b) 'VV(3, 4, 5) = (38, 6, 12), or equivalently, (19, 3, 6). (c) IV'V(3, 4, 5)1 = v'382 + 6 2 + 12 2 = v'l624 = 2 v'406 -----t 35. A unit vector in the direction o(AB is i and a unit vector in the direction of AC isj. Thus D_..... f(1, 3) = f.,(1, 3) ~ 3 and AB D- f(l, 3) = / y(1, 3) = 26. Therefore \7 /(1, 3) = (!.,(1, 3), /y(l, 3)) = (3, 26}, and by definition, AC -----t DAD f (1 , 3) = V' f · u where u is a unit vector in the direction of AD, which is (fa, H). Therefore, 37 () DAD f (1, 3) = (3, 26) . . ( 153, H) = 3. fa + 26. H = 312;. . a v au + v ~ ' a a ~ + {) , a ~- + ~ a a , ~ + ~ ' a '["7( b)=(o(au+bv) 8(au+bv)) =\ au bav au bav)= (au au; b\av au; .= a 'Vu + b 'Vv uX y ux X uy uy X uy ux y -----t (d) '["7 n ( o(un) 8(u")) ( n - 1 au n - 1 au) n - 1 '["7 v u - , - nu , nu · - nu v u ax oy ox {)y 39. f(x, y) = x 3 + 5x 2 y + y 3 . "* Duf(x,y) = 'Vf(x, y) · u = (3x 2 + lOxy, 5x 2 + 3y 2 ) · (~, ~) = ~x 2 + 6xy+ 4x 2 + ¥v 2 = ~x 2 + 6xy + ¥y 2 . Then D~.J(x ,y) = Du (Duf(x,y)] = \7 [Duf(x,y)] · u = (¥x + 6y, 6x + -\1Y) · (~, ~) = l;s4x + Jfy + ¥x + ~y = 2is4x + ~ar,oY and D~f(2 , 1) = 2iu4 (2) + 12866 (1) = 72754 . @ 2012 Ccn&_:'lle Le:uning. All Rights Reserv<strong>ed</strong>. May not be scann<strong>ed</strong>, enpicd. ordupliealcd. or post<strong>ed</strong> 10 o publicly occessible " '"""ile, in whole or in p:ul.
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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 10.4 AREAS AND LENGTHS IN P
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SECTION 10.5 CONIC SECTIONS 0 27 5.
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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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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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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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Therefore E = { (x, y, z) I -2 ~ X~
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43. I,. = foL foL foL k(y2 + z2)dz.
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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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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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0 APPENDIX Appendix H Complex Numbe
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APPENDIX H COMPLEX NUMBERS 0 361 43