082-Engineering-Mathematics-Anthony-Croft-Robert-Davison-Martin-Hargreaves-James-Flint-Edisi-5-2017

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7 VectorsContents 7.1 Introduction 2247.2 Vectorsandscalars:basicconcepts 2247.3 Cartesiancomponents 2327.4 Scalarfieldsandvectorfields 2407.5 Thescalarproduct 2417.6 Thevectorproduct 2467.7 Vectorsofndimensions 253Reviewexercises7 2557.1 INTRODUCTIONCertainphysicalquantitiesarefullydescribedbyasinglenumber:forexample,themassof a stone, the speed of a car. Such quantities are called scalars. On the other hand,some quantities are not fully described until a direction is specified in addition to thenumber. For example, a velocity of 30 metres per second due east is different from avelocityof30metrespersecondduenorth.Thesequantitiesarecalledvectorsanditisimportanttodistinguishthemfromscalars.There aremany engineering applications inwhich vector and scalar quantities play important roles. For example, speed, potential,work and energy are scalar quantities, while velocity, electric and magnetic forces, theposition of a robot and the state-space representation of a system can all be describedby vectors. A variety of mathematical techniques have been developed to enable usefulcalculations tobe carriedout usingvectors and inthischapter these will be discussed.7.2 VECTORSANDSCALARS:BASICCONCEPTSScalarsarethesimplestquantitieswithwhichtodeal;thespecificationofasinglenumberisallthatisrequired.Vectorsalsohaveadirectionanditisusefultoconsideragraphicalrepresentation. Thus the line segment AB of length 4 in Figure 7.1 can represent
7.2 Vectors and scalars: basic concepts 225AaBACABBCDDFigure7.1Avector, AB,oflength → 4.Figure7.2Two equal vectors.a vector in the direction shown by the arrow on AB. This vector is denoted by AB.→→Note that AB ≠ BA. → The vector AB → →is directed from A to B, but BA is directed fromBtoA.An alternative notation is frequently used: we denote AB → by a. This bold notationis commonly used in textbooks but the notation a is preferable for handwritten work.Wenowneedtorefertothediagramtoappreciate theintended direction.Thelengthofthe line segment represents the magnitude, or modulus, of the vector and we use thenotation | → AB|, |a| or simply a to denote this. Note that whereas a is a vector, |a| is ascalar.7.2.1 NegativevectorsThe vector −a is a vector in the opposite direction to, but with the same magnitude as,a. Geometrically itwill be → BA. Thus −aisthe same as → BA.7.2.2 EqualvectorsTwovectorsareequaliftheyhavethesamemagnitudeanddirection.InFigure7.2vectors→ CDand → ABareequaleventhoughtheirlocationsdiffer.Thisisausefulpropertyofvectors:avectorcanbetranslated,maintainingitslengthanddirectionwithoutchangingthevectoritself.Thereareexceptionstothisproperty.Forexample,weshallsoonmeetposition vectors which are used to locate specific fixed points in space. They clearlycannot be moved around freely. Nevertheless most of the vectors we shall meet can betranslated freely, and assuch are often calledfree vectors.7.2.3 VectoradditionItisfrequentlyusefultoaddtwoormorevectorstogetherandtheadditionofvectorsisdefinedbythetrianglelaw.ReferringtoFigure7.3,ifwewishtoaddABto → CD,→ CDistranslateduntilCandBcoincide.Asmentionedearlier,thistranslationdoesnotchange→thevectorCD.Thenthesum,→ AB+ CD,isdefinedbythevectorrepresentedbythethird→sideof the completed triangle, thatis → AD(Figure 7.4).Thus,→AB + → CD = → AD→Similarly,ifABisdenotedbya,→ CDisdenotedbyb, ADisdenotedbyc,thenwehavec=a+bWenotethattoaddaandbatriangleisformedusingaandbastwoofthesidesinsucha way that the head of one vector touches the tail of the other as shown in Figure 7.4.The suma +bisthen represented by the third side.→→
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ENGINEERINGMATHEMATICSA Foundation
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At Pearson, we have a simple missio
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PEARSONEDUCATIONLIMITEDEdinburghGat
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ContentsPrefaceAcknowledgementsxvii
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Contents ix8.3 Addition,subtraction
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Contents xiChapter17 Numericalinteg
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Contents xiiiChapter24 TheFouriertr
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Contents xvAppendixI Representing a
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PrefaceAudienceThis book has been w
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AcknowledgementsWearegratefultothef
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1 ReviewofalgebraictechniquesConten
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1.2 Laws of indices 3So6 2 6 3 =6 5
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1.2 Laws of indices 5(c)(d)x 9x 5 =
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1.2 Laws of indices 71.2.4 Multiple
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1.2 Laws of indices 9Similarly(2 1/
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1.3 Number bases 11Solutions1 (a) 8
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1.3 Number bases 13giving83=64+16+3
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1.3 Number bases 15Example1.16 Conv
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1.3 Number bases 17Table1.4isusedto
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1.3 Number bases 19The display show
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1.4 Polynomial equations 21Example1
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1.4 Polynomial equations 23We now i
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so thatβ=−13Bycomparing coeffici
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1.5.1 Properandimproperfractions1.5
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1.5 Algebraic fractions 29(b) Facto
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1.5 Algebraic fractions 31and4x +2
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1.6 Solution of inequalities 33(g)(
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1.6 Solution of inequalities 35Exam
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1.6 Solution of inequalities 37Case
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1.7 Partial fractions 391.7 PARTIAL
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1.7 Partial fractions 41Thus we hav
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1.7 Partial fractions 43Solution Th
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1.7 Partial fractions 45EXERCISES1.
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1.8 Summation notation 47Engineerin
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1.8 Summation notation 49thecircuit
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Review exercises 1 513 Removethe br
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Review exercises 1 53[ ((d) 3 z −
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2.2 Numbers and intervals 55in orde
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2.3 Basic concepts of functions 57f
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2.3 Basic concepts of functions 59s
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2.3 Basic concepts of functions 61b
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2.3 Basic concepts of functions 63E
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2.3 Basic concepts of functions 65f
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2.3 Basic concepts of functions 67T
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2.3 Basic concepts of functions 691
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2.4 Review of some common engineeri
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2.4.2 Rationalfunctions2.4 Review o
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Table2.2Values ofa x fora = 0.5, 2
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2.4.4 Logarithmfunctions2.4 Review
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Review exercises 2 113REVIEWEXERCIS
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3 ThetrigonometricfunctionsContents
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Note thattanθ = BCAB = BCAC × ACA
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3.3 The trigonometric ratios 119yyB
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3.4 The sine, cosine and tangent fu
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3.5 The sincxfunction 123EXERCISES3
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3.6 Trigonometric identities 125ors
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3.6 Trigonometric identities 127Exa
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3.6 Trigonometric identities 129Exa
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3.7 Modelling waves using sint and
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3.8 Trigonometric equations 145sin
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3.8 Trigonometric equations 147tan
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Usingascientific calculator wehavez
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Review exercises 3 1516 Simplify th
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Review exercises 3 153(d) 1.581sin(
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4.2 Cartesian coordinate system --
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4.3 Cartesian coordinate system --
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4.4 Polar coordinates 1594.4 POLARC
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4.4 Polar coordinates 161yOurxFigur
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4.5 Some simple polar curves 163EXE
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4.5 Some simple polar curves 165uAn
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4.6 Cylindrical polar coordinates 1
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4.6 Cylindrical polar coordinates 1
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4.7 Spherical polar coordinates 171
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Page 197 and 198: 5.2 Set theory 177Example5.1 Useset
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Page 201 and 202: 5.2 Set theory 181someelementsinA.W
Page 203 and 204: 5.3 Logic 183CDCD(a)(b)CDCD(c)(d)(e
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Page 217 and 218: Review exercises 5 19712 (a) A·B+A
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Page 221 and 222: 6.2 Sequences 2016.2 SEQUENCESAsequ
Page 223 and 224: 6.2 Sequences 203sin t1x[k]1- 3p-2p
Page 225 and 226: 6.2 Sequences 205Ageneralgeometricp
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Page 229 and 230: 6.3 Series 20913 ±12814 315 016 (a
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Page 237 and 238: 6.4 The binomial theorem 217EXERCIS
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Page 243: Review exercises 6 22315 (a) Write
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Page 253 and 254: yjOirFigure7.19Thex--y plane withpo
Page 255 and 256: 7.3 Cartesian components 235Solutio
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Page 261 and 262: 7.5 The scalar product 241OEFigure7
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Page 277 and 278: 8 MatrixalgebraContents 8.1 Introdu
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8.6.1 FindingtheinverseofamatrixFor
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8.6 The inverse of a 2 × 2 matrix
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8.7 Determinants 279In addition to
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8.8 The inverse of a 3 × 3 matrix
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8.9 Application to the solution of
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8.9 Application to the solution of
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Solution Firstconsider the equation
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8.10 Gaussian elimination 289anythi
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Eliminating the unwanted values int
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⎛R 1R 2→R 2−6R 1⎝R 3→R 3
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8.11 Eigenvalues and eigenvectors 2
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Itfollows thatso that(2−λ)(4−
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8.12 Analysis of electrical network
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8.13 Iterative techniques for the s
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8.14 Computer solutions of matrix p
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Review exercises 8 321V = [3;−6;4
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Review exercises 8 3234 (a) −8⎛
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9.2 Complex numbers 3259.2 COMPLEXN
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9.2 Complex numbers 3279.2.1 Thecom
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Similarly, wefind, by equating imag
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9.3 Operations with complex numbers
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9.5 Polar form of a complex number
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9.5.1 Multiplicationanddivisioninpo
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9.7 The exponential form of a compl
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9.7 The exponential form of a compl
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9.8 Phasors 341example, in the case
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9.8 Phasors 343Therefore,Ṽ S=ṼR
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which isclearly true,and the theore
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9.9 De Moivre’s theorem 347y25p
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9.9 De Moivre’s theorem 349Now, w
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9.10 Loci and regions of the comple
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9.10 Loci and regions of the comple
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Review exercises 9 3559 Sketch the
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10.2 Graphical approach to differen
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10.3 Limits and continuity 359f (t)
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10.3 Limits and continuity 361Theli
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10.4 Rate of change at a specific p
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10.5 Rate of change at a general po
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10.6 Existence of derivatives 371x
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10.7 Common derivatives 373Table10.
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10.8 Differentiation as a linear op
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Review exercises 10 385REVIEWEXERCI
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11.2 Rules of differentiation 387Th
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11.2 Rules of differentiation 389Th
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(b) Ify = ln(1 −t),theny ′ =
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11.3 Parametric, implicit and logar
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11.4 Higher derivatives 401Example1
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11.4 Higher derivatives 403yCByCAyB
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Review exercises 11 405Solutions1 (
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12.2 Maximum points and minimum poi
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12.3 Points of inflexion 415Solutio
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12.3 Points of inflexion 417y ′ =
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12.4 The Newton--Raphson method for
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12.4 The Newton--Raphson method for
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12.5 Differentiation of vectors 423
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Solution (a) Ifa = 3t 2 i +cos2tj,
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13.2 Elementary integration 42913.2
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13.2 Elementary integration 431Tabl
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Solution (a)sinx+cosx(j)2(k) 2t −
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13.2 Elementary integration 435Engi
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13.2 Elementary integration 4374.00
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Therefore,∫∫ 1sinmtsinnt dt = {
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13.2 Elementary integration 4412 (a
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13.3 Definite and indefinite integr
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Review exercises 13 4536716438 (a)
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Review exercises 13 45522 Calculate
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14 TechniquesofintegrationContents
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14.2 Integration by parts 459Usingt
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Usingintegration by parts we have
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14.3 Integration by substitution 46
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14.3 Integration by substitution 46
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14.4 Integration using partial frac
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Review exercises 14 469∫ π/3(b)
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15 ApplicationsofintegrationContent
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15.2 Average value of a function 47
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15.3 Root mean square value of a fu
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15.3 Root mean square value of a fu
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Review exercises 15 479(d) 0.7071(e
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[Example16.1 Show that f (x) =xandg
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Solution (a) We use the trigonometr
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16.3 Improper integrals 485iC 1 C 2
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∫ 2either of the integrals failst
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16.4 Integral properties of the del
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16.5 Integration of piecewise conti
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16.6 Integration of vectors 49316.6
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Review exercises 16 49512 Given14 G
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17.2 Trapezium rule 497y{ {y 0 y ny
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17.2 Trapezium rule 499The differen
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yABCDE17.3 Simpson’s rule 501quad
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17.3 Simpson’s rule 503Table17.6T
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Review Exercises 17 505EXERCISES17.
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18 Taylorpolynomials,Taylorseriesan
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18.2 Linearization using first-orde
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18.2 Linearization using first-orde
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18.3 Second-order Taylor polynomial
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18.3 Second-order Taylor polynomial
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18.4 Taylor polynomials of the nth
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18.4. Taylor polynomials of the nth
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18.5 Taylor’s formula and the rem
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We know |x| < 1, and so 4x51518.5 T
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18.6 Taylor and Maclaurin series 52
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Review exercises 18 5337 (a) 0, 2,
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19.2 Basic definitions 535In engine
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19.2 Basic definitions 537Note also
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19.2 Basic definitions 539fromwhich
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19.3 First-order equations: simple
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19.4 First-order linear equations:
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and so, upon integrating,so that(co
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19.5 Second-order linear equations
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19.6 Constant coefficient equations
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thatis,β = 332The required particu
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19.7 Series solution of differentia
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19.8 Bessel’s equation and Bessel
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fromwhicha 5=− 124 a 3 = 1192 a 1
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n 5 2n 5 3n5 419.8 Bessel’s equat
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Review exercises 19 601quencies, kn
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20 OrdinarydifferentialequationsIIC
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20.2 Analogue simulation 605y iy i
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20.3 Higher order equations 607High
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20.4 State-space models 609Solution
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20.4 State-space models 611statevar
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20.4 State-space models 613R a L aT
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20.5 Numerical methods 615Combining
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20.6 Euler’s method 617and we can
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20.6 Euler’s method 619Whenx = 1,
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20.7 Improved Euler method 621Table
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20.8 Runge--Kutta method of order 4
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20.8.1 Higherorderequations20.8 Run
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21 TheLaplacetransformContents 21.1
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21.3 Laplace transforms of some com
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21.4 Properties of the Laplace tran
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(b) Usethe first shift theorem with
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21.5 Laplace transform of derivativ
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21.5 Laplace transform of derivativ
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21.6 Inverse Laplace transforms 639
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21.7 Using partial fractions to fin
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21.8 Finding the inverse Laplace tr
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21.8 Finding the inverse Laplace tr
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21.9 The convolution theorem 64721.
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21.9 Solving linear constant coeffi
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21.10 Solving linear constant coeff
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X(s)= s3 −3s 2 −4s+6s 2 (s 2
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21.11 Transfer functions 659(c) x
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21.11 Transfer functions 661R(s)G(s
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21.11 Transfer functions 663R(s) +-
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21.11 Transfer functions 665Fuel va
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21.11 Transfer functions 667u a (t)
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21.12 Poles, zeros and thesplane 66
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21.13 Laplace transforms of some sp
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21.13.2 Periodicfunctions21.13 Lapl
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Review exercises 21 6792 Find the L
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22 Differenceequationsandtheztransf
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22.2 Basic definitions 68322.2.2 Th
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22.2 Basic definitions 685an inhomo
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22.3 Rewriting difference equations
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22.4 Block diagram representation o
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22.4 Block diagram representation o
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22.5 Design of a discrete-time cont
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22.6 Numerical solution of differen
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22.6 Numerical solution of differen
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22.7 Definition of the z transform
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22.7 Definition of the z transform
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22.8 Sampling a continuous signal 7
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22.9 The relationship between the z
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22.9 The relationship between the z
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22.10 Properties of the z transform
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22.11 Inversion of z transforms 715
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22.11 Inversion of z transforms 717
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22.12 The z transform and differenc
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Review exercises 22 721(e) q[k +3]
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23.2 Periodic waveforms 72323.2 PER
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23.2 Periodic waveforms 725f(t)1f(t
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23.3 Odd and even functions 727f(t)
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23.3 Odd and even functions 729f(t)
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23.3 Odd and even functions 731the
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23.5 Fourier series 733Table23.1Som
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23.5 Fourier series 735point out th
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23.5 Fourier series 737but cos(−n
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23.5 Fourier series 739Example23.16
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23.5 Fourier series 741y4- 3π -- -
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23.5 Fourier series 743We conclude
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23.6 Half-range series 745EXERCISES
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23.6 Half-range series 747Half-rang
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23.8 Complex notation 749Engineerin
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23.9 Frequency response of a linear
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23.9 Frequency response of a linear
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̸̸̸Review exercises 23 755The va
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24 TheFouriertransformContents 24.1
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24.2 The Fourier transform -- defin
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24.3 Some properties of the Fourier
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∫ 2[ ] eSolution (a) F(ω)=3 e
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24.3 Some properties of the Fourier
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24.4 Spectra 767uF(v)u2-4p -3p -2p
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The t−ω duality principle 769f(t
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24.6 Fourier transforms of some spe
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24.7 The relationship between the F
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24.8 Convolution and correlation 77
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and theirproduct isF(ω)G(ω) =1(1+
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24.9 The discrete Fourier transform
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24.9 The discrete Fourier transform
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24.10 Derivation of the d.f.t. 787T
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(Solution ConsiderF˜ ω + 2π )for
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24.11 Using the d.f.t.to estimate a
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24.13 Some properties of the d.f.t.
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24.14 The discrete cosine transform
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24.15 Discrete convolution and corr
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25 FunctionsofseveralvariablesConte
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25.3 Partial derivatives 825DCAz =
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25.3 Partial derivatives 827Enginee
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25.4 Higher order derivatives 829
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25.4 Higher order derivatives 831Ex
Page 853 and 854:
25.5 Partial differential equations
Page 855 and 856:
25.6 Taylor polynomials and Taylor
Page 857 and 858:
Page 859 and 860:
Page 861 and 862:
25.7 Maximum and minimum points of
Page 863 and 864:
Page 865 and 866:
Page 867 and 868:
Review exercises 25 8474 Find allfi
Page 869 and 870:
26 VectorcalculusContents 26.1 Intr
Page 871 and 872:
26.3 The gradient of a scalar field
Page 873 and 874:
(b) At (0,0,0), ∇φ =0i+3j+0k =3j
Page 875 and 876:
26.3 The gradient of a scalar field
Page 877 and 878:
26.4.1 Physicalinterpretationof ∇
Page 879 and 880:
26.5 The curl of a vector field 859
Page 881 and 882:
26.6 Combining the operators grad,
Page 883 and 884:
26.6 Combining the operators grad,
Page 885 and 886:
Equation3Review exercises 26 865cur
Page 887 and 888:
27 Lineintegralsandmultipleintegral
Page 889 and 890:
27.2 Line integrals 869SolutionThe
Page 891 and 892:
27.3 Evaluation of line integrals i
Page 893 and 894:
27.4 Evaluation of line integrals i
Page 895 and 896:
27.5 Conservative fields and potent
Page 897 and 898:
27.5 Conservative fields and potent
Page 899 and 900:
Substitutingy =x 2 and dy = 2xdx we
Page 901 and 902:
27.6 Double and triple integrals 88
Page 903 and 904:
Page 905 and 906:
Page 907 and 908:
y10GDR27.6 Double and triple integr
Page 909 and 910:
27.7 Some simple volume and surface
Page 911 and 912:
Page 913 and 914:
Page 915 and 916:
27.8 The divergence theorem and Sto
Page 917 and 918:
27.8 The divergence theorem and Sto
Page 919 and 920:
27.9 Maxwell’s equations in integ
Page 921 and 922:
Page 923 and 924:
28 ProbabilityContents 28.1 Introdu
Page 925 and 926:
28.2 Introducing probability 905Ifm
Page 927 and 928:
28.2 Introducing probability 907Eng
Page 929 and 930:
28.3 Mutually exclusive events: the
Page 931 and 932:
28.3 Mutually exclusive events: the
Page 933 and 934:
28.4 Complementary events 913EXERCI
Page 935 and 936:
28.5 Concepts from communication th
Page 937 and 938:
28.5 Concepts from communication th
Page 939 and 940:
28.6 Conditional probability: the m
Page 941 and 942:
28.6 Conditional probability: the m
Page 943 and 944:
P(A ∩C) =P(C ∩A) =P(C)P(A|C)P(A
Page 945 and 946:
28.7 Independent events 9255 Compon
Page 947 and 948:
28.7 Independent events 927Solution
Page 949 and 950:
28.7 Independent events 929E 1,E 2a
Page 951 and 952:
Review exercises 28 931(d) A compon
Page 953 and 954:
29 Statisticsandprobabilitydistribu
Page 955 and 956:
29.3 Probability distributions -- d
Page 957 and 958:
29.4 Probability density functions
Page 959 and 960:
29.5 Mean value 939Example29.3 Find
Page 961 and 962:
29.6 Standard deviation 94129.6 STA
Page 963 and 964:
29.7 Expected value of a random var
Page 965 and 966:
29.7 Expected value of a random var
Page 967 and 968:
29.8 Standard deviation of a random
Page 969 and 970:
29.9 Permutations and combinations
Page 971 and 972:
29.9 Permutations and combinations
Page 973 and 974:
29.10 The binomial distribution 953
Page 975 and 976:
29.10 The binomial distribution 955
Page 977 and 978:
29.11 The Poisson distribution 957I
Page 979 and 980:
Table29.6Theprobabilitiesforbinomia
Page 981 and 982:
29.12 The uniform distribution 9615
Page 983 and 984:
29.14 The normal distribution 963So
Page 985 and 986:
29.14 The normal distribution 965N(
Page 987 and 988:
29.14 The normal distribution 967Ta
Page 989 and 990:
29.14 The normal distribution 969EX
Page 991 and 992:
29.15 Reliability engineering 971in
Page 993 and 994:
29.15 Reliability engineering 973En
Page 995 and 996:
29.15 Reliability engineering 975k
Page 997 and 998:
Review exercises 29 977Solutions1 0
Page 999 and 1000:
AppendicesContents I Representingac
Page 1001 and 1002:
II The Greek alphabet 981f(t)T0 t 0
Page 1003 and 1004:
Indexabsolute quantity88absorption
Page 1005 and 1006:
Index 985chord 357--8circuital law
Page 1007 and 1008:
Index 987cycle ofsint 131cycles ofl
Page 1009 and 1010:
Index 989eigenvalues andeigenvector
Page 1011 and 1012:
Index 991spectra 766--8t-w duality
Page 1013 and 1014:
Index 993characteristic impedance o
Page 1015 and 1016:
Index 995exclusive OR gate 189NAND
Page 1017 and 1018:
Index 997second-order 829--30, 833,
Page 1019 and 1020:
Index 999remainder term,Taylor’s
Page 1021 and 1022:
Index 1001solenoidal vectorfield 85
Page 1023 and 1024:
Index 1003calculus 849--66curl859--
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082-Engineering-Mathematics-Anthony-Croft-Robert-Davison-Martin-Hargreaves-James-Flint-Edisi-5-2017

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