BASIC ALGEBRA OF VECTORS
|
|
- Darrell Boone
- 5 years ago
- Views:
Transcription
1 Fomulae Fo u Vecto Algeba By Mi Mohammed Abbas II PCMB 'A' Impotant Tems, Definitions & Fomulae 01 Vecto - Basic Intoduction: A quantity having magnitude as well as the diection is called vecto It is denoted as AB o a Its magnitude (o modulus) is AB o a othewise, simply AB o a Vectos ae denoted by symbols such as a o a o a [Pictoial epesentation of vecto] 0 Initial and Teminal points: The initial and teminal points mean that point fom which the vecto oiginates and teminates espectively 03 Position Vecto: The position vecto of a point say P( x, y, z ) is OP x i ˆ y ˆ j z k ˆ and the magnitude is x y z The vecto OP x i ˆ y ˆ j z k ˆ is said to be in its component fom Hee x, y, z ae called the scala components o ectangula components of and xiˆ, yˆj, zk ˆ ae the vecto components of along x-, y-, z- axes espectively Also, AB Position Vecto of B Position Vecto of A Fo example, let A( x1, y 1,z 1) and B( x, y,z ) Then, AB ( x ˆ ˆ ˆ ˆ ˆ ˆ i y j zk) ( x1i y1 j z1k ) Hee iˆ, ˆj and ˆk ae the unit vectos along the axes OX, OY and OZ espectively (The discussion about unit vectos is given late in the point 05(e)) 04 Diection atios and diection cosines: If xiˆ yˆ j zkˆ, then coefficients of iˆ, ˆj, k ˆ in ie, x, y, z ae called the diection atios (abbeviated as d s) of vecto These ae denoted by a, b, c (ie a x, b y, c z ; in a manne we can say that scala components of vecto and its d s both ae the same) Also, the coefficients of iˆ, ˆj, k ˆ in ˆ (which is the unit vecto of x y ) ie,,, x y z x y z z ae called diection cosines (which is abbeviated as dc s) of vecto x y z These diection cosines ae denoted by l, m, n such that l cos, m cos, n cos and l m n 1 cos cos cos 1 x y z It can be easily concluded that l cos, m cos, n cos Theefoe, liˆ mˆj nkˆ (cos iˆ cos ˆj cos k ˆ) (Hee ) [See the OAP in Fig1] Angles,, ae made by the vecto with the positive diections of x, y, z-axes espectively and these angles ae known as the diection angles of vecto ) BASIC ALGEBRA OF VECTORS Fo a bette undestanding, you can visualize the Fig1 05 TYPES OF VECTORS a) Zeo o Null vecto: Its that vecto whose initial and teminal points ae coincident It is denoted by 0 Of couse its magnitude is 0 (zeo) Any non-zeo vecto is called a pope vecto b) Co-initial vectos: Those vectos (two o moe) having the same initial point ae called the coinitial vectos Page - [1] wwwmohammedabbas7wodpesscom
2 c) Co-teminous vectos: Those vectos (two o moe) having the same teminal point ae called the co-teminous vectos d) Negative of a vecto: The vecto which has the same magnitude as the but opposite diection It is denoted by Hence if, AB BA That is AB BA, PQ QP etc e) Unit vecto: It is a vecto with the unit magnitude The unit vecto in the diection of vecto is given by ˆ such that 1 So, if xiˆ yˆj zkˆ then its unit vecto is: x ˆ y ˆ z ˆ i j kˆ x y z x y z x y z Unit vecto pependicula to the plane of a a b and b is: a b f) Recipocal of a vecto: It is a vecto which has the same diection as the vecto but magnitude equal to the ecipocal of the magnitude of It is denoted as 1 Hence 1 1 g) Equal vectos: Two vectos ae said to be equal if they have the same magnitude as well as diection, egadless of the positions of thei initial points a b Thus a b a and b have same diection Also, if a b a1iˆ a ˆ ˆ ˆ ˆ ˆ j a3k b1i b j b3k a1 b1, a b, a3 b 3 h) Collinea o Paallel vecto: Two vectos a and b ae collinea o paallel if thee exists a nonzeo scala such that a b It is impotant to note that the espective coefficients of iˆ, ˆj, k ˆ in a and b ae popotional povide they ae paallel o collinea to each othe Conside ˆ ˆ ˆ ˆ ˆ ˆ a a1i a j a3k, b b1i b j b3k, then by using a b, we can conclude a1 a a3 that: b b b 1 3 The d s of paallel vectos ae same (o ae in popotion) The vectos a and b will have same o opposite diection as is positive o negative The vectos a and b ae collinea if a b 0 i) Fee vectos: The vectos which can undego paallel displacement without changing its magnitude and diection ae called fee vectos 06 ADDITION OF VECTORS a) Tiangula law: If two adjacent sides (say sides AB and BC) of a tiangle ABC ae epesented by a and b taken in same ode, then the thid side of the tiangle taken in the evese ode gives the sum of vectos a and b ie, AC AB BC AC a b See Fig Also since AC CA AB BC CA AA 0 And AB BC AC AB BC AC 0 AB BC CA 0 b) Paallelogam law: If two vectos a and b ae epesented in magnitude and the diection by the two adjacent sides (say AB and AD) of a paallelogam ABCD, then thei sum is given by that diagonal of paallelogam which is co-initial with a and b ie, OC OA OB Fo the illustation, see Fig3 Multiplication of a vecto by a scala Let a be any vecto and k be any scala Then the poduct ka is defined as a vecto whose magnitude is k times that of a and the diection is (i) same as that of a if k is positive, and (ii) opposite to that of a if k is negative Page - [] wwwmohammedabbas7wodpesscom
3 07 PROPERTIES OF VECTOR ADDITION Commutative popety: a b b a Conside ˆ ˆ ˆ a a1i a j a3k and b b ˆ ˆ ˆ 1i b j b3k be any two given vectos Then a b a1 b1 iˆ a b ˆj a3 b3 kˆ b a Associative popety: a b c a b c Additive identity popety: a 0 0 a a Additive invese popety: a ( a) 0 ( a) a 08 Section fomula: The position vecto of a point say P dividing a line segment joining the points A and B whose position vectos ae a and b espectively, in the atio m:n mb na (a) intenally, is OP m n mb na (b) extenally, is OP m n a b Also if point P is the mid-point of line segment AB then, OP Impotant Tems, Definitions & Fomulae 01 PRODUCT OF TWO VECTORS a) Scala poduct o Dot poduct: The dot poduct of two vectos a and b is defined by, a b a b cos whee θ is the angle between a and b, 0 See Fig4 Conside ˆ ˆ ˆ ˆ ˆ ˆ a a1i a j a3k, b b1i b j b3k Then a b a1b 1 ab a3b3 Popeties / Obsevations of Dot poduct iˆ iˆ iˆ iˆ cos0 1 iˆ iˆ 1 ˆj ˆj kˆ kˆ iˆ ˆj iˆ ˆj cos 0 iˆ ˆj 0 ˆj kˆ kˆ iˆ a b R, whee R is eal numbe ie, any scala a b b a (Commutative popety of dot poduct) a b 0 a b If θ = 0 then, a b a b Also a a a a ; as θ in this case is 0 Moeove if θ = then, a b a b a b c a b a c (Distibutive popety of dot poduct) PRODUCT OF VECTORS DOT PRODUCT & CROSS PRODUCT a b a b a b Angle between two vectos a and b can be found by the expession given below: cos a b a b Page - [3] wwwmohammedabbas7wodpesscom
4 1 o, cos a b a b Pojection of a vecto a on the othe vecto say b a b is given as ie, a bˆ b This is also known as Scala pojection o Component of a along b Pojection vecto of a on the othe vecto say b a b is given as b ˆ b This is also known as the Vecto pojection Wok done W in moving an object fom point A to the point B by applying a foce F is given as W F AB b) Vecto poduct o Coss poduct: The coss poduct of two vectos a and b is defined by, a b a b sin ˆ, whee is the angle between the vectos a and b, 0 and ˆ is a unit vecto pependicula to both a and b Fo bette illustation, see Fig5 Conside a a ˆ ˆ ˆ ˆ ˆ ˆ 1i a j a3k, b b1i b j b3k iˆ ˆj kˆ a b a a a a b a b iˆ a b a b ˆj a b a b kˆ Then, b b b 1 3 Popeties / Obsevations of Coss poduct iˆ iˆ iˆ iˆ sin 0 ˆj 0 iˆ iˆ 0 ˆj ˆj kˆ kˆ iˆ ˆj iˆ ˆj sin kˆ kˆ iˆ ˆj kˆ, ˆj kˆ iˆ, kˆ iˆ ˆj Fig6 at the end of chapte can be consideed fo memoizing the vecto poduct of iˆ, ˆj, k ˆ a b is a vecto c (say) and this vecto c is pependicula to both the vectos a and b a b a b sin ˆ a b sin ie, a b ab sin a b 0 a // b o, a 0, b 0 a a 0 a b b a (Commutative popety does not hold fo coss poduct) a b c a b a c; b c a b a c a (Distibutive popety of the vecto poduct o coss poduct) Angle between two vectos a and b in tems of Coss-poduct can be found by the ab expession given hee: sin a b a b 1 o, sin a b If a and b epesent the adjacent sides of a tiangle, then the aea of tiangle can be obtained by evaluating 1 a b Page - [4] wwwmohammedabbas7wodpesscom
5 If a and b epesent the adjacent sides of a paallelogam, then the aea of paallelogam can be obtained by evaluating a b If p and q epesent the two diagonals of a paallelogam, then the aea of paallelogam can be obtained by evaluating 1 p q If a and b epesent the adjacent sides of a paallelogam, then the diagonals d 1 and d of the paallelogam ae given as: d1 a b, d b a 0 Relationship between Vecto poduct and Scala poduct [Lagange s Identity] Conside two vectos a and b We also know that a b a b sin ˆ Now, a b a b sin ˆ a b a b sin a b a b sin a b a b 1 cos a b a b a b cos a b a b a b cos a b a b a b o, a b a b a b a a a b Note that a b Hee the RHS epesents a deteminant of ode a b b b 03 Cauchy- Schwatz inequality: Fo any two vectos a and b, we always have a b a b Poof: The given inequality holds tivially when eithe a 0 o b 0 ie, in such a case a b 0 a b So, let us check it fo a 0 b As we know, a b a b cos a b a b cos Also we know cos 1 fo all the values of a b cos a b a b a b a b a b [HP] 04 Tiangle inequality: Fo any two vectos a and b, we always have a b a b Poof: The given inequality holds tivially when eithe a 0 o b 0 ie, in such a case we have Page - [5] wwwmohammedabbas7wodpesscom
6 a b 0 a b So, let us check it fo a 0 b Then conside a b a b a b a b a b a b cos Fo cos 1, we have: a b cos a b a b a b cos a b a b a b a b a b a b [HP] SCALAR TRIPLE PRODUCT OF VECTORS Impotant Tems, Definitions & Fomulae 01 SCALAR TRIPLE PRODUCT: If a,b and c ae any thee vectos, then the scala poduct of poduct of a,b and c Thus, ( a b) c is called the scala tiple poduct of a,b and c a b with c is called scala tiple Notation fo scala tiple poduct: The scala tiple poduct of a,b and c is denoted by [ a b c ] That is, ( a b) c [ a b c ] Scala tiple poduct is also known as mixed poduct because in scala tiple poduct, both the signs of dot and coss ae used ˆ ˆ ˆ ˆ ˆ ˆ a a i a j a k, b b i b j b k, c c iˆ c ˆj c k ˆ Conside a a a Then, [ a b c] b b b c c c 1 3 Popeties / Obsevations of Scala Tiple Poduct ( a b) c a( b c ) That is, the position of dot and coss can be intechanged without change in the value of the scala tiple poduct (povided thei cyclic ode emains the same) [ a b c] [ b c a] [ c a b ] That is, the value of scala tiple poduct doesn t change when cyclic ode of the vectos is maintained Also [ a b c] [ b a c]; [ b c a] [ b a c ] That is, the value of scala tiple poduct emains the same in magnitude but changes the sign when cyclic ode of the vectos is alteed Fo any thee vectos a, b, c and scala, we have [ a b c] [ a b c ] The value of scala tiple poduct is zeo if any two of the thee vectos ae identical That is, [ a a c] 0 [ a b b] [ a b a ] etc Value of scala tiple poduct is zeo if any two of the thee vectos ae paallel o collinea Scala tiple poduct of iˆ, ˆj and ˆk is 1 (unity) ie, [ iˆ ˆj k ˆ] 1 Page - [6] wwwmohammedabbas7wodpesscom
7 If [ a b c ] 0 then, the non-paallel and non-zeo vectos a, b and c ae coplana Volume Of Paallelopiped If a, b and c epesent the thee co-teminus edges of a paallelopiped, then its volume can be obtained by: [ a b c] ( a b) c That is, ( a b) c Base aea of Paallelopiped Height of Paallelopiped on this base If fo any thee vectos a, b and c, we have [ a b c ] 0, then volume of paallelepiped with the co-teminus edges as a, b and c, is zeo This is possible only if the vectos a, b and c ae co-plana Page - [7] wwwmohammedabbas7wodpesscom
8 VARIOUS FIGURES RELATED TO THE VECTOR ALGEBRA
e.g: If A = i 2 j + k then find A. A = Ax 2 + Ay 2 + Az 2 = ( 2) = 6
MOTION IN A PLANE 1. Scala Quantities Physical quantities that have only magnitude and no diection ae called scala quantities o scalas. e.g. Mass, time, speed etc. 2. Vecto Quantities Physical quantities
More informationSUPPLEMENTARY MATERIAL CHAPTER 7 A (2 ) B. a x + bx + c dx
SUPPLEMENTARY MATERIAL 613 7.6.3 CHAPTER 7 ( px + q) a x + bx + c dx. We choose constants A and B such that d px + q A ( ax + bx + c) + B dx A(ax + b) + B Compaing the coefficients of x and the constant
More informationCartesian Coordinate System and Vectors
Catesian Coodinate System and Vectos Coodinate System Coodinate system: used to descibe the position of a point in space and consists of 1. An oigin as the efeence point 2. A set of coodinate axes with
More informationFREE Download Study Package from website: &
.. Linea Combinations: (a) (b) (c) (d) Given a finite set of vectos a b c,,,... then the vecto xa + yb + zc +... is called a linea combination of a, b, c,... fo any x, y, z... R. We have the following
More informationLESSON THREE DIMENSIONAL GEOMETRY
Intoduction LESSON THREE DIMENSIONAL GEOMETRY The coodinates of any point P in the 3 D Catesian system ae the pependicula distance fom P on the thee mutually ectangula coodinate planes XOZ, XOY and YOZ
More informationJ. N. R E DDY ENERGY PRINCIPLES AND VARIATIONAL METHODS APPLIED MECHANICS
J. N. E DDY ENEGY PINCIPLES AND VAIATIONAL METHODS IN APPLIED MECHANICS T H I D E DI T IO N JN eddy - 1 MEEN 618: ENEGY AND VAIATIONAL METHODS A EVIEW OF VECTOS AND TENSOS ead: Chapte 2 CONTENTS Physical
More informationPhysics Tutorial V1 2D Vectors
Physics Tutoial V1 2D Vectos 1 Resolving Vectos & Addition of Vectos A vecto quantity has both magnitude and diection. Thee ae two ways commonly used to mathematically descibe a vecto. y (a) The pola fom:,
More informationKEPLER S LAWS AND PLANETARY ORBITS
KEPE S AWS AND PANETAY OBITS 1. Selected popeties of pola coodinates and ellipses Pola coodinates: I take a some what extended view of pola coodinates in that I allow fo a z diection (cylindical coodinates
More information(A) 2log( tan cot ) [ ], 2 MATHEMATICS. 1. Which of the following is correct?
MATHEMATICS. Which of the following is coect? A L.P.P always has unique solution Evey L.P.P has an optimal solution A L.P.P admits two optimal solutions If a L.P.P admits two optimal solutions then it
More informationWhen two numbers are written as the product of their prime factors, they are in factored form.
10 1 Study Guide Pages 420 425 Factos Because 3 4 12, we say that 3 and 4 ae factos of 12. In othe wods, factos ae the numbes you multiply to get a poduct. Since 2 6 12, 2 and 6 ae also factos of 12. The
More informationMODULE 5a and 5b (Stewart, Sections 12.2, 12.3) INTRO: In MATH 1114 vectors were written either as rows (a1, a2,..., an) or as columns a 1 a. ...
MODULE 5a and 5b (Stewat, Sections 2.2, 2.3) INTRO: In MATH 4 vectos wee witten eithe as ows (a, a2,..., an) o as columns a a 2... a n and the set of all such vectos of fixed length n was called the vecto
More informationCALCULUS II Vectors. Paul Dawkins
CALCULUS II Vectos Paul Dawkins Table of Contents Peface... ii Vectos... 3 Intoduction... 3 Vectos The Basics... 4 Vecto Aithmetic... 8 Dot Poduct... 13 Coss Poduct... 21 2007 Paul Dawkins i http://tutoial.math.lama.edu/tems.aspx
More informationPrepared by: M. S. KumarSwamy, TGT(Maths) Page
Prepared by: M S KumarSwamy, TGT(Maths) Page - 119 - CHAPTER 10: VECTOR ALGEBRA QUICK REVISION (Important Concepts & Formulae) MARKS WEIGHTAGE 06 marks Vector The line l to the line segment AB, then a
More informationOLYMON. Produced by the Canadian Mathematical Society and the Department of Mathematics of the University of Toronto. Issue 9:2.
OLYMON Poduced by the Canadian Mathematical Society and the Depatment of Mathematics of the Univesity of Toonto Please send you solution to Pofesso EJ Babeau Depatment of Mathematics Univesity of Toonto
More information2. Electrostatics. Dr. Rakhesh Singh Kshetrimayum 8/11/ Electromagnetic Field Theory by R. S. Kshetrimayum
2. Electostatics D. Rakhesh Singh Kshetimayum 1 2.1 Intoduction In this chapte, we will study how to find the electostatic fields fo vaious cases? fo symmetic known chage distibution fo un-symmetic known
More informationVector d is a linear vector function of vector d when the following relationships hold:
Appendix 4 Dyadic Analysis DEFINITION ecto d is a linea vecto function of vecto d when the following elationships hold: d x = a xxd x + a xy d y + a xz d z d y = a yxd x + a yy d y + a yz d z d z = a zxd
More informationVectors. Teaching Learning Point. Ç, where OP. l m n
Vectors 9 Teaching Learning Point l A quantity that has magnitude as well as direction is called is called a vector. l A directed line segment represents a vector and is denoted y AB Å or a Æ. l Position
More informationCHAPTER 10 VECTORS POINTS TO REMEMBER
For more important questions visit : www4onocom CHAPTER 10 VECTORS POINTS TO REMEMBER A quantity that has magnitude as well as direction is called a vector It is denoted by a directed line segment Two
More informationVectors Serway and Jewett Chapter 3
Vectos Sewa and Jewett Chapte 3 Scalas and Vectos Vecto Components and Aithmetic Vectos in 3 Dimensions Unit vectos i, j, k Pactice Poblems: Chapte 3, poblems 9, 19, 31, 45, 55, 61 Phsical quantities ae
More informationPhysics 111 Lecture 5 (Walker: 3.3-6) Vectors & Vector Math Motion Vectors Sept. 11, 2009
Physics 111 Lectue 5 (Walke: 3.3-6) Vectos & Vecto Math Motion Vectos Sept. 11, 2009 Quiz Monday - Chap. 2 1 Resolving a vecto into x-component & y- component: Pola Coodinates Catesian Coodinates x y =
More informationanubhavclasses.wordpress.com CBSE Solved Test Papers PHYSICS Class XII Chapter : Electrostatics
CBS Solved Test Papes PHYSICS Class XII Chapte : lectostatics CBS TST PAPR-01 CLASS - XII PHYSICS (Unit lectostatics) 1. Show does the foce between two point chages change if the dielectic constant of
More informationUNIT 1 VECTORS INTRODUCTION 1.1 OBJECTIVES. Stucture
UNIT 1 VECTORS 1 Stucture 1.0 Introduction 1.1 Objectives 1.2 Vectors and Scalars 1.3 Components of a Vector 1.4 Section Formula 1.5 nswers to Check Your Progress 1.6 Summary 1.0 INTRODUCTION In this unit,
More informationINTRODUCTION. 2. Vectors in Physics 1
INTRODUCTION Vectos ae used in physics to extend the study of motion fom one dimension to two dimensions Vectos ae indispensable when a physical quantity has a diection associated with it As an example,
More informationKEPLER S LAWS OF PLANETARY MOTION
EPER S AWS OF PANETARY MOTION 1. Intoduction We ae now in a position to apply what we have leaned about the coss poduct and vecto valued functions to deive eple s aws of planetay motion. These laws wee
More informationVECTORS. Vectors OPTIONAL - I Vectors and three dimensional Geometry
Vectors OPTIONAL - I 32 VECTORS In day to day life situations, we deal with physical quantities such as distance, speed, temperature, volume etc. These quantities are sufficient to describe change of position,
More informationMoment. F r F r d. Magnitude of moment depends on magnitude of F and the length d
Moment Tanslation Tanslation + Rotation This otation tenency is known as moment M of foce (toque) xis of otation may be any line which neithe intesects no paallel to the line of action of foce Magnitue
More informationA Crash Course in (2 2) Matrices
A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula
More informationCHAPTER 25 ELECTRIC POTENTIAL
CHPTE 5 ELECTIC POTENTIL Potential Diffeence and Electic Potential Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic foce on the paticle given by F=E. When
More informationMath Notes on Kepler s first law 1. r(t) kp(t)
Math 7 - Notes on Keple s fist law Planetay motion and Keple s Laws We conside the motion of a single planet about the sun; fo simplicity, we assign coodinates in R 3 so that the position of the sun is
More informationChapter 1: Introduction to Polar Coordinates
Habeman MTH Section III: ola Coodinates and Comple Numbes Chapte : Intoduction to ola Coodinates We ae all comfotable using ectangula (i.e., Catesian coodinates to descibe points on the plane. Fo eample,
More informationAs is natural, our Aerospace Structures will be described in a Euclidean three-dimensional space R 3.
Appendix A Vecto Algeba As is natual, ou Aeospace Stuctues will be descibed in a Euclidean thee-dimensional space R 3. A.1 Vectos A vecto is used to epesent quantities that have both magnitude and diection.
More information7.2. Coulomb s Law. The Electric Force
Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat
More informationElectrostatics. 1. Show does the force between two point charges change if the dielectric constant of the medium in which they are kept increase?
Electostatics 1. Show does the foce between two point chages change if the dielectic constant of the medium in which they ae kept incease? 2. A chaged od P attacts od R whee as P epels anothe chaged od
More informationAppendix A. Appendices. A.1 ɛ ijk and cross products. Vector Operations: δ ij and ɛ ijk
Appendix A Appendices A1 ɛ and coss poducts A11 Vecto Opeations: δ ij and ɛ These ae some notes on the use of the antisymmetic symbol ɛ fo expessing coss poducts This is an extemely poweful tool fo manipulating
More informationMCV4U Final Exam Review. 1. Consider the function f (x) Find: f) lim. a) lim. c) lim. d) lim. 3. Consider the function: 4. Evaluate. lim. 5. Evaluate.
MCVU Final Eam Review Answe (o Solution) Pactice Questions Conside the function f () defined b the following gaph Find a) f ( ) c) f ( ) f ( ) d) f ( ) Evaluate the following its a) ( ) c) sin d) π / π
More informationMAGNETIC FIELD INTRODUCTION
MAGNETIC FIELD INTRODUCTION It was found when a magnet suspended fom its cente, it tends to line itself up in a noth-south diection (the compass needle). The noth end is called the Noth Pole (N-pole),
More informationPhysics 2B Chapter 22 Notes - Magnetic Field Spring 2018
Physics B Chapte Notes - Magnetic Field Sping 018 Magnetic Field fom a Long Staight Cuent-Caying Wie In Chapte 11 we looked at Isaac Newton s Law of Gavitation, which established that a gavitational field
More information6.4 Period and Frequency for Uniform Circular Motion
6.4 Peiod and Fequency fo Unifom Cicula Motion If the object is constained to move in a cicle and the total tangential foce acting on the total object is zeo, F θ = 0, then (Newton s Second Law), the tangential
More informationWelcome to Physics 272
Welcome to Physics 7 Bob Mose mose@phys.hawaii.edu http://www.phys.hawaii.edu/~mose/physics7.html To do: Sign into Masteing Physics phys-7 webpage Registe i-clickes (you i-clicke ID to you name on class-list)
More informationVIII - Geometric Vectors
MTHEMTIS 0-05-RE Linea lgeba Matin Huad Fall 05 VIII - Geometic Vectos. Find all ectos in the following paallelepiped that ae equialent to the gien ectos. E F H G a) b) HE c) H d) E e) f) F g) HE h) F
More information3.6 Applied Optimization
.6 Applied Optimization Section.6 Notes Page In this section we will be looking at wod poblems whee it asks us to maimize o minimize something. Fo all the poblems in this section you will be taking the
More informationSides and Angles of Right Triangles 6. Find the indicated side length in each triangle. Round your answers to one decimal place.
Chapte 7 Peequisite Skills BLM 7-1.. Convet a Beaing to an Angle in Standad Position 1. Convet each beaing to an angle in standad position on the Catesian gaph. a) 68 127 c) 215 d) 295 e) N40 W f) S65
More informationSHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.
Chapte 7-8 Review Math 1316 Name SHORT ANSWER. Wite the wod o phase that best completes each statement o answes the question. Solve the tiangle. 1) B = 34.4 C = 114.2 b = 29.0 1) Solve the poblem. 2) Two
More informationCOORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT
COORDINATE TRANSFORMATIONS - THE JACOBIAN DETERMINANT Link to: phsicspages home page. To leave a comment o epot an eo, please use the auilia blog. Refeence: d Inveno, Ra, Intoducing Einstein s Relativit
More information3.1 Random variables
3 Chapte III Random Vaiables 3 Random vaiables A sample space S may be difficult to descibe if the elements of S ae not numbes discuss how we can use a ule by which an element s of S may be associated
More informationSources of Magnetic Fields (chap 28)
Souces of Magnetic Fields (chap 8) In chapte 7, we consideed the magnetic field effects on a moving chage, a line cuent and a cuent loop. Now in Chap 8, we conside the magnetic fields that ae ceated by
More informationTo Feel a Force Chapter 7 Static equilibrium - torque and friction
To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on
More information(read nabla or del) is defined by, k. (9.7.1*)
9.7 Gadient of a scala field. Diectional deivative Some of the vecto fields in applications can be obtained fom scala fields. This is vey advantageous because scala fields can be handled moe easily. The
More informationq r 1 4πε Review: Two ways to find V at any point in space: Integrate E dl: Sum or Integrate over charges: q 1 r 1 q 2 r 2 r 3 q 3
Review: Lectue : Consevation of negy and Potential Gadient Two ways to find V at any point in space: Integate dl: Sum o Integate ove chages: q q 3 P V = i 4πε q i i dq q 3 P V = 4πε dq ample of integating
More informationESCI 342 Atmospheric Dynamics I Lesson 3 Fundamental Forces II
Reading: Matin, Section. ROTATING REFERENCE FRAMES ESCI 34 Atmospheic Dnamics I Lesson 3 Fundamental Foces II A efeence fame in which an object with zeo net foce on it does not acceleate is known as an
More informationworking pages for Paul Richards class notes; do not copy or circulate without permission from PGR 2004/11/3 10:50
woking pages fo Paul Richads class notes; do not copy o ciculate without pemission fom PGR 2004/11/3 10:50 CHAPTER7 Solid angle, 3D integals, Gauss s Theoem, and a Delta Function We define the solid angle,
More information. Using our polar coordinate conversions, we could write a
504 Chapte 8 Section 8.4.5 Dot Poduct Now that we can add, sutact, and scale vectos, you might e wondeing whethe we can multiply vectos. It tuns out thee ae two diffeent ways to multiply vectos, one which
More informationEELE 3331 Electromagnetic I Chapter 4. Electrostatic fields. Islamic University of Gaza Electrical Engineering Department Dr.
EELE 3331 Electomagnetic I Chapte 4 Electostatic fields Islamic Univesity of Gaza Electical Engineeing Depatment D. Talal Skaik 212 1 Electic Potential The Gavitational Analogy Moving an object upwad against
More informationVECTOR MECHANICS FOR ENGINEERS: STATICS
4 Equilibium CHAPTER VECTOR MECHANICS FOR ENGINEERS: STATICS Fedinand P. Bee E. Russell Johnston, J. of Rigid Bodies Lectue Notes: J. Walt Ole Texas Tech Univesity Contents Intoduction Fee-Body Diagam
More informationRigid Body Dynamics 2. CSE169: Computer Animation Instructor: Steve Rotenberg UCSD, Winter 2018
Rigid Body Dynamics 2 CSE169: Compute Animation nstucto: Steve Rotenbeg UCSD, Winte 2018 Coss Poduct & Hat Opeato Deivative of a Rotating Vecto Let s say that vecto is otating aound the oigin, maintaining
More informationΔt The textbook chooses to say that the average velocity is
1-D Motion Basic I Definitions: One dimensional motion (staight line) is a special case of motion whee all but one vecto component is zeo We will aange ou coodinate axis so that the x-axis lies along the
More informationThe Archimedean Circles of Schoch and Woo
Foum Geometicoum Volume 4 (2004) 27 34. FRUM GEM ISSN 1534-1178 The Achimedean Cicles of Schoch and Woo Hioshi kumua and Masayuki Watanabe Abstact. We genealize the Achimedean cicles in an abelos (shoemake
More informationCHAPTER 10 ELECTRIC POTENTIAL AND CAPACITANCE
CHAPTER 0 ELECTRIC POTENTIAL AND CAPACITANCE ELECTRIC POTENTIAL AND CAPACITANCE 7 0. ELECTRIC POTENTIAL ENERGY Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic
More information7.2.1 Basic relations for Torsion of Circular Members
Section 7. 7. osion In this section, the geomety to be consideed is that of a long slende cicula ba and the load is one which twists the ba. Such poblems ae impotant in the analysis of twisting components,
More informationElectrostatics (Electric Charges and Field) #2 2010
Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when
More informationarxiv: v1 [physics.pop-ph] 3 Jun 2013
A note on the electostatic enegy of two point chages axiv:1306.0401v1 [physics.pop-ph] 3 Jun 013 A C Tot Instituto de Física Univesidade Fedeal do io de Janeio Caixa Postal 68.58; CEP 1941-97 io de Janeio,
More informationPHYS 1444 Lecture #5
Shot eview Chapte 24 PHYS 1444 Lectue #5 Tuesday June 19, 212 D. Andew Bandt Capacitos and Capacitance 1 Coulom s Law The Fomula QQ Q Q F 1 2 1 2 Fomula 2 2 F k A vecto quantity. Newtons Diection of electic
More informationCh 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!
Ch 30 - Souces of Magnetic Field 1.) Example 1 Detemine the magnitude and diection of the magnetic field at the point O in the diagam. (Cuent flows fom top to bottom, adius of cuvatue.) Fo staight segments,
More informationPhysics 201 Lecture 18
Phsics 0 ectue 8 ectue 8 Goals: Define and anale toque ntoduce the coss poduct Relate otational dnamics to toque Discuss wok and wok eneg theoem with espect to otational motion Specif olling motion (cente
More informationAP-C WEP. h. Students should be able to recognize and solve problems that call for application both of conservation of energy and Newton s Laws.
AP-C WEP 1. Wok a. Calculate the wok done by a specified constant foce on an object that undegoes a specified displacement. b. Relate the wok done by a foce to the aea unde a gaph of foce as a function
More informationMark Scheme 4727 June 2006
Mak Scheme 77 June 006 77 Mak Scheme June 006 (a) Identity = + 0 i Invese = + i i = + i i 0 0 (b) Identity = 0 0 0 Invese = 0 0 i B Fo coect identity. Allow B Fo seen o implied + i = B Fo coect invese
More informationElectric field generated by an electric dipole
Electic field geneated by an electic dipole ( x) 2 (22-7) We will detemine the electic field E geneated by the electic dipole shown in the figue using the pinciple of supeposition. The positive chage geneates
More informationChapter 4. Newton s Laws of Motion
Chapte 4 Newton s Laws of Motion 4.1 Foces and Inteactions A foce is a push o a pull. It is that which causes an object to acceleate. The unit of foce in the metic system is the Newton. Foce is a vecto
More informationIntroduction to Arrays
Intoduction to Aays Page 1 Intoduction to Aays The antennas we have studied so fa have vey low diectivity / gain. While this is good fo boadcast applications (whee we want unifom coveage), thee ae cases
More informationSHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.
Math Pecalculus Ch. 6 Review Name SHORT ANSWER. Wite the wod o phase that best completes each statement o answes the question. Solve the tiangle. ) ) 6 7 0 Two sides and an angle (SSA) of a tiangle ae
More informationPhysics 2212 GH Quiz #2 Solutions Spring 2016
Physics 2212 GH Quiz #2 Solutions Sping 216 I. 17 points) Thee point chages, each caying a chage Q = +6. nc, ae placed on an equilateal tiangle of side length = 3. mm. An additional point chage, caying
More informationElectric Charge and Field
lectic Chage and ield Chapte 6 (Giancoli) All sections ecept 6.0 (Gauss s law) Compaison between the lectic and the Gavitational foces Both have long ange, The electic chage of an object plas the same
More information(n 1)n(n + 1)(n + 2) + 1 = (n 1)(n + 2)n(n + 1) + 1 = ( (n 2 + n 1) 1 )( (n 2 + n 1) + 1 ) + 1 = (n 2 + n 1) 2.
Paabola Volume 5, Issue (017) Solutions 151 1540 Q151 Take any fou consecutive whole numbes, multiply them togethe and add 1. Make a conjectue and pove it! The esulting numbe can, fo instance, be expessed
More informationB. Spherical Wave Propagation
11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We
More informationradians). Figure 2.1 Figure 2.2 (a) quadrant I angle (b) quadrant II angle is in standard position Terminal side Terminal side Terminal side
. TRIGONOMETRIC FUNCTIONS OF GENERAL ANGLES In ode to etend the definitions of the si tigonometic functions to geneal angles, we shall make use of the following ideas: In a Catesian coodinate sstem, an
More informationPhysics 11 Chapter 20: Electric Fields and Forces
Physics Chapte 0: Electic Fields and Foces Yesteday is not ous to ecove, but tomoow is ous to win o lose. Lyndon B. Johnson When I am anxious it is because I am living in the futue. When I am depessed
More information21 MAGNETIC FORCES AND MAGNETIC FIELDS
CHAPTER 1 MAGNETIC ORCES AND MAGNETIC IELDS ANSWERS TO OCUS ON CONCEPTS QUESTIONS 1. (d) Right-Hand Rule No. 1 gives the diection of the magnetic foce as x fo both dawings A and. In dawing C, the velocity
More informationENGI 1313 Mechanics I
ENGI 1313 Mechanics I Lectue 04: oce Vectos and System of Coplana oces Shawn Kenny, Ph.D., P.Eng. Assistant Pofesso aculty of Engineeing and Applied Science Memoial Univesity of Newfoundland spkenny@eng.mun.ca
More informationReview: Electrostatics and Magnetostatics
Review: Electostatics and Magnetostatics In the static egime, electomagnetic quantities do not vay as a function of time. We have two main cases: ELECTROSTATICS The electic chages do not change postion
More informationOnline Mathematics Competition Wednesday, November 30, 2016
Math@Mac Online Mathematics Competition Wednesday, Novembe 0, 206 SOLUTIONS. Suppose that a bag contains the nine lettes of the wod OXOMOXO. If you take one lette out of the bag at a time and line them
More informationChapter 8 Vectors and Scalars
Chapter 8 193 Vectors and Scalars Chapter 8 Vectors and Scalars 8.1 Introduction: In this chapter we shall use the ideas of the plane to develop a new mathematical concept, vector. If you have studied
More informationPhysics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism
Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up
More informationAST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1
Please ead this fist... AST S: The oigin and evolution of the Univese Intoduction to Mathematical Handout This is an unusually long hand-out and one which uses in places mathematics that you may not be
More informationTHE CONE THEOREM JOEL A. TROPP. Abstract. We prove a fixed point theorem for functions which are positive with respect to a cone in a Banach space.
THE ONE THEOEM JOEL A. TOPP Abstact. We pove a fixed point theoem fo functions which ae positive with espect to a cone in a Banach space. 1. Definitions Definition 1. Let X be a eal Banach space. A subset
More informationQuestion Bank. Section A. is skew-hermitian matrix. is diagonalizable. (, ) , Evaluate (, ) 12 about = 1 and = Find, if
Subject: Mathematics-I Question Bank Section A T T. Find the value of fo which the matix A = T T has ank one. T T i. Is the matix A = i is skew-hemitian matix. i. alculate the invese of the matix = 5 7
More informationDescribing Circular motion
Unifom Cicula Motion Descibing Cicula motion In ode to undestand cicula motion, we fist need to discuss how to subtact vectos. The easiest way to explain subtacting vectos is to descibe it as adding a
More informationChapter 1. Introduction
Chapte 1 Intoduction 1.1 The Natue of Phsics Phsics has developed out of the effots of men and women to eplain ou phsical envionment. Phsics encompasses a emakable vaiet of phenomena: planeta obits adio
More information15.081J/6.251J Introduction to Mathematical Programming. Lecture 6: The Simplex Method II
15081J/6251J Intoduction to Mathematical Pogamming ectue 6: The Simplex Method II 1 Outline Revised Simplex method Slide 1 The full tableau implementation Anticycling 2 Revised Simplex Initial data: A,
More informationIntroduction and Vectors
SOLUTIONS TO PROBLEMS Intoduction and Vectos Section 1.1 Standads of Length, Mass, and Time *P1.4 Fo eithe sphee the volume is V = 4! and the mass is m =!V =! 4. We divide this equation fo the lage sphee
More informationEuclidean Figures and Solids without Incircles or Inspheres
Foum Geometicoum Volume 16 (2016) 291 298. FOUM GEOM ISSN 1534-1178 Euclidean Figues and Solids without Incicles o Insphees Dimitis M. Chistodoulou bstact. ll classical convex plana Euclidean figues that
More informationOn the Quasi-inverse of a Non-square Matrix: An Infinite Solution
Applied Mathematical Sciences, Vol 11, 2017, no 27, 1337-1351 HIKARI Ltd, wwwm-hikaicom https://doiog/1012988/ams20177273 On the Quasi-invese of a Non-squae Matix: An Infinite Solution Ruben D Codeo J
More informationPDF Created with deskpdf PDF Writer - Trial ::
A APPENDIX D TRIGONOMETRY Licensed to: jsamuels@bmcc.cun.edu PDF Ceated with deskpdf PDF Wite - Tial :: http://www.docudesk.com D T i g o n o m e t FIGURE a A n g l e s Angles can be measued in degees
More informationHopefully Helpful Hints for Gauss s Law
Hopefully Helpful Hints fo Gauss s Law As befoe, thee ae things you need to know about Gauss s Law. In no paticula ode, they ae: a.) In the context of Gauss s Law, at a diffeential level, the electic flux
More informationAE301 Aerodynamics I UNIT B: Theory of Aerodynamics
AE301 Aeodynamics I UNIT B: Theoy of Aeodynamics ROAD MAP... B-1: Mathematics fo Aeodynamics B-2: Flow Field Repesentations B-3: Potential Flow Analysis B-4: Applications of Potential Flow Analysis AE301
More informationGauss Law. Physics 231 Lecture 2-1
Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing
More informationK.S.E.E.B., Malleshwaram, Bangalore SSLC Model Question Paper-1 (2015) Mathematics
K.S.E.E.B., Malleshwaam, Bangaloe SSLC Model Question Pape-1 (015) Mathematics Max Maks: 80 No. of Questions: 40 Time: Hous 45 minutes Code No. : 81E Fou altenatives ae given fo the each question. Choose
More information2 Governing Equations
2 Govening Equations This chapte develops the govening equations of motion fo a homogeneous isotopic elastic solid, using the linea thee-dimensional theoy of elasticity in cylindical coodinates. At fist,
More informationChapter 5 Linear Equations: Basic Theory and Practice
Chapte 5 inea Equations: Basic Theoy and actice In this chapte and the next, we ae inteested in the linea algebaic equation AX = b, (5-1) whee A is an m n matix, X is an n 1 vecto to be solved fo, and
More informationRight-handed screw dislocation in an isotropic solid
Dislocation Mechanics Elastic Popeties of Isolated Dislocations Ou study of dislocations to this point has focused on thei geomety and thei ole in accommodating plastic defomation though thei motion. We
More informationVectors, Vector Calculus, and Coordinate Systems
! Revised Apil 11, 2017 1:48 PM! 1 Vectos, Vecto Calculus, and Coodinate Systems David Randall Physical laws and coodinate systems Fo the pesent discussion, we define a coodinate system as a tool fo descibing
More information