CHAPTER 14 REVIEW D 241 45. j(x, y) = x 2 e- 11 => 'V f = (2xe- 11 , - x 2 e- 11 ), 'V f( -2, 0) = (-4, -4). The direction is given by (4, - 3), so u = 1 yf42+(-3)2 ... ... (4,-3} = { (4,-3) and Duf(-2,0} = 'Vf{-2,0} · u = (-4, -4) · t (4, -3) = t(-16 + 12} = -~. 47. 'V f = (2xy,x 2 + 1/(2JY)), I'Vf(2, 1)1 = 1(4, ~) I · Thus the maximum rate of change off at (2, 1} is o/ in the direction ( 4·, !). 49. First we draw a line passing through Homestea'd and the eye of the hurricane. We can approximate the directional derivative at Homestead in the direction of the eye of the hurricane by the average rate of change of wind spe<strong>ed</strong> between the points where this line intersects the contour lines closest to Homestead. In the direction of the eye of the hurricane, the wind spe<strong>ed</strong> changes from 45 to 50 knots. We estimate the distance between these two points to be approximately 8 miles, so the rate of change of wind spe<strong>ed</strong> in the direction given is approximately 50 8 45 = i = 0.625 knot/ mi. 51 . f(x,y)=x 2 - xy+y 2 + 9x -6y+10 => f, = ·2x-y+9, j 11 = - x + 2y- 6, f xx = 2 = / 1111 , f xv = - 1. Then f x = 0 and ! 11 = 0 imply y = 1, x = -4. Thus the only critical point is ( - 4, 1} and fx:r:( -4, 1) > 0, D(- 4, 1) = 3 > 0, so f( - 4, 1) = -11 is a local minimum. 53. f(x, y) = 3xy - x 2 y- xy 2 => fx = 3y - 2xy - y 2 , / 11 = 3x- x 2 - 2xy, f,, = - 2y, fv·u = - 2x, f xv = 3-2x- 2y. Then f, = 0 implies y(3- 2x- y) = 0 soy= 0 or y = 3 - 2x. Substituting into / 11 = 0 implies x(3 - x) = 0 or 3x( - 1 + x )' = 0. Hence the critical points are (0, 0), (3, 0}, (0, 3) and (1, 1). D(O, 0} = D(3, 0} = D(O, 3) = ·-9 < 0 so (0, 0), (3, 0), and (0, 3) are saddle points. D(1, 1) = 3 > 0 and f xx (1, 1} = - 2 < 0, so !(1, 1) = 1 is a local maximum. 55. First solve inside D. Here f ., = 4y 2 - 2xy 2 - y 3 , f 11 = 8xy - 2x 2 y - 3xy 2 • y Then f, =·o implies y = 0 or y = 4- 2x, but y = 0 isn't inside D. Substituting (O, 6 ) y = 4- 2x into / 11 = 0 implies x = 0, x = 2 or x = 1, but x = 0 isn't inside -D, and when x = 2, y = 0 but (2, 0} isn't inside D. Thus the only critical point inside D is (1, 2) and f (l , 2) = 4. Secondly we consider the boundary of D. On L1: f(x, 0) = 0 and so f = 0 on L 1. On L2: x = -y + 6 and (6,0) .t f( - y + 6, y) = y 2 (6 - y)( - 2) = -2{6y 2 - y 3 ) which has critical points at y = 0 and y = 4. Then !{6, 0) = 0 while !(2, 4) = -64. On La: f(O , y) = 0, so f = 0 on £ 3. Thus on D the absolute maximum off is !{1, 2} = 4 while the absolute minimum is /{2, 4) = - 64. ® 2012 Cengnge LC3rning. All Rights Rescf"\·<strong>ed</strong>. Mny not be scann<strong>ed</strong>, copi<strong>ed</strong>, or duplicat<strong>ed</strong>, or post<strong>ed</strong> to a publicly accessible website, in whole or in pan.
242 0 CHAPTER 14 PARTIAL DERIVATIVES 57. f(x, y) = x 3 - 3x + y 4 - 2y 2 2 z 0 l\ "'' 0 and f xx( -1, 0) = - 6 0 and / u(1, ±1} = 6 > 0 indicating local minima / (1, ± 1) = - 3; and D ( -1, ± 1) = - 48 and D(1, 0) = - 24, indicating saddle points. 59. f(x,y) = x 2 y, g(x,y) = x 2 +y 2 = 1 ~ 'ilf = (2xy,x 2 ) = )..'iJg = (2>.x,2>.y). Then 2xy = 2)..x impliesx = Oor y = >.. Ifx = 0 then x + 2 y 2 = 1 gives y = ±1 and we have possible points (0, ±1) where f (0, ± 1) = 0. lfy =).. then x 2 = 2)..y implies x 2 = 2y 2 and substitution into x 2 + y 2 = 1 gives 3y 2 = 1 ~ y = ± 7:J and x = ±jf. The corresponding possible points are ( ±jf, ±7:J). The absolute maximum is f ( ± jf, -Ja) = ~ while the absolute 61. f(x, y, z) = xyz, g(x,y,z) = ~ 2 + y 2 + z 2 = 3. 'ilf = )..'iJg ~ (yz,xz,xy) = >.(2x, 2y,2z). lfany ofx, y, or z is zero, then x = y = z = 0 which contradicts x 2 + y 2 + z 2 = 3. Then ).. = YZ ·=x 2 2 z = xy ~ 2y2 z = 2x 2 z ~ x y 2z . . y 2 = x 2 , and similarly 2yz 2 = 2x 2 y ~ z 2 = x 2 • Substituting into the constraint equation gives x 2 + x 2 + x 2 = 3 ~ I x 2 = 1 = y 2 = z 2 . Thus the possible points are (1, 1, ± 1), (1, -1, ± 1), ( - 1, 1, ±1), ( - 1, -1, ±1). The absolute maximum is / (1, 1, 1) = /(1, -1, - 1) = f( -1, 1, -1) = f( - 1, - 1, 1) = 1 and the absolute minimum is /(1, 1, -1) = /(1, ....:.1, 1) = f( -1,1, 1) = f( - 1, - 1, - 1) = - 1. 63. f(x,y,z) = x 2 +y 2 +z 2 , .g(x,y,z) = xy 2 z 3 = 2 ~ 'ilf = (2x, 2y,2z) = X'ilg = (>.y 2 z 3 , 2>.xyz 3 ,3)..xy 2 z 2 ). Since xy 2 z 3 = 2, x =I 0, y =I 0 and z =I 0, so 2x = )..y 2 z 3 (I), 1 = )..xz 3 (2), 2 = 3>.xy 2 z (3~ . Then (2) and (3) imply ~ = - 3 2 2 or y 2 = f z 2 soy = ±z q. Similarly (1) and (3) imply ~x 3 = - 3 2 ? or 3x 2 = z 2 sox = ± -jsz. But xz xy z V 3 y z xy-z ® 2012 Censa&e l.c4rning. All Rights Rescm:d. May not be scann<strong>ed</strong>, copi<strong>ed</strong>. or duplicat<strong>ed</strong>, or po.
- Page 1 and 2:
- STUDENT SOLUTIONS MANUAL for STEW
- Page 3 and 4:
.. BROOKS/COLE ~ I ~~r CENGAGE Lear
- Page 5 and 6:
D ABBREVIATIONS AND SYMBOLS CD cu D
- Page 7 and 8:
viii o CONTENTS 12.4 The Cross Prod
- Page 9 and 10:
10 D PARAMETRIC EQUATIONS AND POLAR
- Page 11 and 12:
SECTION 10.1 CURVES DEFINED BY PARA
- Page 13 and 14:
SECTION 10.1 CURVES DEFINED BY PARA
- Page 15 and 16:
SECTION 10.2 CALCULUS WITH PARAMETR
- Page 17 and 18:
SECTION 10.2 CALCULUS WITH PARAMETR
- Page 19 and 20:
SECTION 10.2 CALCULUS WITH PARAMETR
- Page 21 and 22:
SECTION 10.3 POLAR COORDINATES 0 13
- Page 23 and 24:
SECTION 10.3 POLAR COORDINATES 0 15
- Page 25 and 26:
SECTION 10.3 POLAR COORDINATES 0 17
- Page 27 and 28:
SECTION 10 .~ POLAR COORDINATES 0 1
- Page 29 and 30:
SECTION 10.4 A~~S AND LENGTHS IN PO
- Page 31 and 32:
SECTION 10.4 AREAS AND LENGTHS IN P
- Page 33 and 34:
SECTION 10.4 AREAS AND LENGTHS IN P
- Page 35 and 36:
SECTION 10.5 CONIC SECTIONS 0 27 5.
- Page 37 and 38:
SECTION 10.5 CONIC SECTIONS 0 29 35
- Page 39 and 40:
x2 y2 y2 a:2 _ a2 b 61. ;_2 - - = 1
- Page 41 and 42:
SECTION 10.6 CONIC SECTIONS IN POLA
- Page 43 and 44:
CHAPTER 10 REVIEW 0 35 the length o
- Page 45 and 46:
CHAPTER 10 REVIEW 0 37 EXERCISES 1.
- Page 47 and 48:
CHAPTER 10 REVIEW 0 39 25. x = t +
- Page 49 and 50:
CHAPTER 10 REVIEW 0 41 2 2 . 45. ~
- Page 51 and 52:
0 PROBLEMS PLUS l lt sin u dx cost
- Page 53 and 54:
11 . D INFINITE SEQUENCES AND SERIE
- Page 55 and 56:
SECTION 11.1 SEQUENCES 0 47 35. a,.
- Page 57 and 58:
SECTION 11.1 SEQUENCES D 49 71. Sin
- Page 59 and 60:
SECTION 11.2 SERIES 0 51 ak+l- a1.:
- Page 61 and 62:
SECTION 11.2 SERIES 0 53 13. n s.,
- Page 63 and 64:
SECTION 11.2 SERIES 0 55 47. F~r th
- Page 65 and 66:
. . (1+ c)- 2 scn es and set 1t equ
- Page 67 and 68:
SECTION 11.3 THE INTEGRAL TEST AND
- Page 69 and 70:
, SECTION 11.3 THE INTEGRAL TEST AN
- Page 71 and 72:
SECTION 11.4 THE COMPARISON TESTS D
- Page 73 and 74:
SECTION 11.5 ALTERNATING SERIES 0 6
- Page 75 and 76:
SECTION 11.5 ALTERNATING SERIES D 6
- Page 77 and 78:
SECTION 11.6 ABSOLUTE CONVERGENCE A
- Page 79 and 80:
SECTION 11.6 ABSOLUTE CONVERGENCE A
- Page 81 and 82:
17 lim I an+l I= SECTION 11.7 STRAT
- Page 83 and 84:
SECTION 11.8 POWER SERIES 0 75 l 00
- Page 85 and 86:
SECTION 11.8 POWER SERIES 0 n (b) I
- Page 87 and 88:
SECTION 11.9 REPRESENTATIONS OF FUN
- Page 89 and 90:
SECTION 11.9 REPRESENTATIONS OF FUN
- Page 91 and 92:
SECTION 11.10 TAYLOR AND MACLAURIN
- Page 93 and 94:
SECTION 11.10 TAYLOR AND MACLAURIN
- Page 95 and 96:
SECTION 11.10 TAYLOR AND MACLAURIN
- Page 97 and 98:
61 _ x_ x · sin x - x- tx 3 + 1~
- Page 99 and 100:
SECTION 11.11 APPLICATIONS OF TAYLO
- Page 101 and 102:
SECTION 11.11 APPLICATIONS OF TAYLO
- Page 103 and 104:
SECTION 11.11 APPLICATIONS OF TAYLO
- Page 105 and 106:
CHAPTER 11 REVIEW 0 97 J'(xn)(xn -
- Page 107 and 108:
CHAPTER 11 REVIEW 0 99 oo f (n) (O)
- Page 109 and 110:
CHAPTER 11 REVIEW 0 101 l 23. Consi
- Page 111 and 112:
49./- 1 - dx = -ln{4- x) + C and 4-
- Page 113 and 114:
D PROBLEMS PLUS 1. It would be far
- Page 115 and 116:
CHAPTER 11 PROBLEMS PLUS D 107 l 9.
- Page 117 and 118:
CHAPTER 11 PROBLEMS PLUS 0 109 x x
- Page 119 and 120:
112 0 CHAPTER 12 VECTORS AND THE GE
- Page 121 and 122:
114 0 CHAPTER 12 VECTORS AND THE GE
- Page 123 and 124:
116 0 CHAPTER 12 VECTORS AND THE GE
- Page 125 and 126:
118 0 CHAPTER 12 VECTORS AND THE GE
- Page 127 and 128:
120 D CHAPTER 12 VECTORS AND THE GE
- Page 129 and 130:
122 0 CHAPTER 12 VECTORS AND THE GE
- Page 131 and 132:
124 0 CHAPTER 12 VECTORS AND THE GE
- Page 133 and 134:
126 0 CHAPTER 12 VECTORS AND THE GE
- Page 135 and 136:
128 D CHAPTER 12 VECTORS AND THE GE
- Page 137 and 138:
130 D CHAPTER 12 VECTORS AND THE GE
- Page 139 and 140:
132 D CHAPTER 12 VECTORS AND THE GE
- Page 141 and 142:
134 D CHAPTER 12 VECTORS AND THE GE
- Page 143 and 144:
136 D CHA~TER 12 VECTORS AND THE GE
- Page 145 and 146:
138 D CHAPTER 12 VECTORS AND THE GE
- Page 147 and 148:
140 D CHAPTER 12 VECTORS AND THE GE
- Page 149 and 150:
142 D CHAPTER 12 VECTORS AND THE GE
- Page 151 and 152:
144 0 CHAPTER 12 VECTORS AND THE GE
- Page 153 and 154:
D PROBLEMS PLUS 1. Since three-dime
- Page 155 and 156:
l CHAPTER 12 PROBLEMS PLUS 0 149 Eq
- Page 157 and 158:
13 D VECTOR FUNCTIONS 13.1 Vector F
- Page 159 and 160:
SECTION 13.1 VECTOR FUNCTIONS AND S
- Page 161 and 162:
SECTION 13.1 VECTOR FUNCTIONS AND S
- Page 163 and 164:
SECTION 13.2 DERIVATIVES AND INTEGR
- Page 165 and 166:
SECTION 13.2 DERIVATIVES AND INTEGR
- Page 167 and 168:
SECTION 13.3 ARC LENGTH AND CURVATU
- Page 169 and 170:
SECTION 13.3 ARC LENGTH AND CURVATU
- Page 171 and 172:
SECTION 13.3 ARC LENGTH AND CURVATU
- Page 173 and 174:
SECTION 13.3 ARC LENGTH AND CURVATU
- Page 175 and 176:
SECTION 13.4 MOTION IN SPACE: VELOC
- Page 177 and 178:
2 SECTION 13.4 MOTION IN SPACE: VEL
- Page 179 and 180:
CHAPTER 13 REVIEW D 173 43. The tan
- Page 181 and 182:
5. f~(t 2 i +tcos 1rtj +sin 1rt k )
- Page 183 and 184:
CHAPTER 13 REVIEW 0 177 23. (a) r (
- Page 185 and 186:
180 0 CHAPTER 13 PROBLEMS PLUS (-2a
- Page 187 and 188:
182 0 CHAPTER 13 PROBLEMS PLUS vect
- Page 189 and 190:
184 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 191 and 192:
186 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 193 and 194:
188 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 195 and 196: 190 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 197 and 198: 192 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 199 and 200: 194 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 201 and 202: 196 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 203 and 204: 198 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 205 and 206: 200 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 207 and 208: 202 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 209 and 210: 204 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 211 and 212: 206 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 213 and 214: 208 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 215 and 216: 210 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 217 and 218: 212 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 219 and 220: 214 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 221 and 222: 216 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 223 and 224: 218 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 225 and 226: 220 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 227 and 228: 222 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 229 and 230: 224 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 231 and 232: 226 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 233 and 234: 228 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 235 and 236: 230 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 237 and 238: 232 D CHAPTER 14 PARTIAL DERIVATIVE
- Page 239 and 240: 234 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 241 and 242: 236 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 243 and 244: 238 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 245: 240 0 CHAPTER 14 PARTIAL DERIVATIVE
- Page 249 and 250: D PROBLEMS PLUS 1. The areas of the
- Page 251 and 252: 15 D MULTIPLE INTEGRALS 15.1 Double
- Page 253 and 254: SECTION 15.2 ITERATED INTEGRALS D 2
- Page 255 and 256: l SECTION 15.3 DOUBLE INTEGRALS OVE
- Page 257 and 258: SECTION 15.3 DOUBLE INTEGRALS OVER
- Page 259 and 260: SECTION 15.3 DOUBLE INTEGRALS OVER
- Page 261 and 262: 61 . Since m :S j(x, y) :S M, ffD m
- Page 263 and 264: SECTION 15.4 DOUBLE INTEGRALS IN PO
- Page 265 and 266: SECTION 15.5 APPLICATIONS OF DOUBLE
- Page 267 and 268: SECTION 15.5 APPLICATIONS OF DOUBLE
- Page 269 and 270: SECTION 1505 APPLICATIONS OF DOUBLE
- Page 271 and 272: -I SECTION 15.6 SURFACE AREA 0 267
- Page 273 and 274: SECTION 15.7 TRIPLE INTEGRALS 0 269
- Page 275 and 276: SECTION 15.7 TRIPLE INTEGRALS D 271
- Page 277 and 278: Therefore E = { (x, y, z) I -2 ~ X~
- Page 279 and 280: 43. I,. = foL foL foL k(y2 + z2)dz.
- Page 281 and 282: SECTION 15.8 TRIPLE INTEGRALS IN CY
- Page 283 and 284: M xv = I~1f I: I:2 6 - 3 r 2 (zK) r
- Page 285 and 286: SECTION 15.9 TRIPLE INTEGRALS IN SP
- Page 287 and 288: SECTION 15.9 TRIPLE INTEGRALS IN SP
- Page 289 and 290: (b) The wedge in question is the sh
- Page 291 and 292: SECTION 15.10 CHANGE OF VARIABLES I
- Page 293 and 294: CHAPTER 15 REVIEW 0 289 15 Review C
- Page 295 and 296: CHAPTER 15 REVIEW 0 291 l 9. The vo
- Page 297 and 298:
CHAPTER 15 REVIEW D 293 33. Using t
- Page 299 and 300:
49. Since u = x- y and v = x + y, x
- Page 301 and 302:
298 D CHAPTER 15 PROBLEMS PLUS To e
- Page 303 and 304:
300 0 CHAPTER 15 PROBLEMS PLUS 13.
- Page 305 and 306:
16 0 VECTOR CALCULUS 16.1 Vector Fi
- Page 307 and 308:
SECTION 16.2 LINE INTEGRALS 0 305 2
- Page 309 and 310:
SECTION 16.2 LINE INTEGRALS 0 307 (
- Page 311 and 312:
SECTION 16.2 LINE INTEGRALS D 309 3
- Page 313 and 314:
SECTION 16.3 THE FUNDAMENTAL THEORE
- Page 315 and 316:
SECTION 16.4 GREEN'S THEOREM D 313
- Page 317 and 318:
SECTION 16.4 GREEN'S THEOREM 0 315
- Page 319 and 320:
8 8 8 (b)clivF = 'V ·iF=- (x+yz) +
- Page 321 and 322:
SECTION 16.5 CURL AND DIVERGENCE 0
- Page 323 and 324:
SECTION 16.6 PARAMETRIC SURFACES AN
- Page 325 and 326:
SECTION 16.6 PARAMETRIC SURFACES AN
- Page 327 and 328:
SECTION 16.6 PARAMETRIC SURFACES AN
- Page 329 and 330:
that is, D = {( x, y) I x 2 + y 2 :
- Page 331 and 332:
SECTION 16.7 SURFACE INTEGRALS 0 32
- Page 333 and 334:
SECTION 16.7 SURFACE INTEGRALS 0 33
- Page 335 and 336:
SECTION 16.8 STOKES' THEOREM 0 333
- Page 337 and 338:
dS SECTION 16.9 THE DIVERGENCE THEO
- Page 339 and 340:
CHAPTER 16 REVIEW 0 337 27. JI 5 cu
- Page 341 and 342:
CHAPTER 16 REVIEW 0 339 TRUE-FALSE
- Page 343 and 344:
CHAPTER 16 REVIEW D 341 Alternate s
- Page 345 and 346:
344 0 CHAPTER 16 PROBLEMS PLUS Simi
- Page 347 and 348:
3.c6 0 CHAPTER 17 SECOND-ORDER DIFF
- Page 349 and 350:
348 0 CHAPTER 17 SECOND-ORDER DIFFE
- Page 351 and 352:
350 0 CHAPTER 17 SECOND-ORDER DIFFE
- Page 353 and 354:
352 D CHAPTER 17 SECOND-ORDER DIFFE
- Page 355 and 356:
354 0 CHAPTER 17 SECOND-ORDER DIFFE
- Page 357 and 358:
356 D CHAPTER 17 SECOND-ORDER DIFFE
- Page 359 and 360:
0 APPENDIX Appendix H Complex Numbe
- Page 361:
APPENDIX H COMPLEX NUMBERS 0 361 43