( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ( )) ( )

Similar documents
Created by T. Madas VECTOR MOMENTS. Created by T. Madas

TABLE OF CONTENTS 2 CHAPTER 1

We could express the left side as a sum of vectors and obtain the Vector Form of a Linear System: a 12 a x n. a m2

Vectors in Physics. Topics to review:

Dot Product August 2013

Find the component form of with initial point A(1, 3) and terminal point B(1, 3). Component form = 1 1, 3 ( 3) (x 1., y 1. ) = (1, 3) = 0, 6 Subtract.

EXAM 1. OPEN BOOK AND CLOSED NOTES Thursday, February 18th, 2010

When two letters name a vector, the first indicates the and the second indicates the of the vector.

Vectors. J.R. Wilson. September 27, 2018

Vectors. J.R. Wilson. September 28, 2017

Chapter 2 One-Dimensional Kinematics

Section 8.2 Vector Angles

7.1 Projections and Components

Math 234. What you should know on day one. August 28, You should be able to use general principles like. x = cos t, y = sin t, 0 t π.

VECTORS IN A STRAIGHT LINE

9.5. Lines and Planes. Introduction. Prerequisites. Learning Outcomes

Vectors. AP/Honors Physics Mr. Velazquez

Equivalent Force Systems

Chapter 6 Additional Topics in Trigonometry, Part II

Topic Learning Outcomes Suggested Teaching Activities Resources On-Line Resources

CALCULUS AB/BC SUMMER REVIEW PACKET (Answers)

( ) 2. = kq 1 q 2 r 2. Analysis: F E. k q 1. Solution: F E % 8.99!10 9 ( (1.00!10 )4 C )(1.00!10 )5 C ) $ (2.00 m) 2 F E

UNIT 1 VECTORS INTRODUCTION 1.1 OBJECTIVES. Stucture

F A C U L T Y O F E D U C A T I O N. Physics Electromagnetism: Induced Currents Science and Mathematics Education Research Group

Chapter 4. Motion in Two Dimensions. Professor Wa el Salah

6.1.1 Angle between Two Lines Intersection of Two lines Shortest Distance from a Point to a Line

Mathematics 2203, Test 1 - Solutions

Module 10 Polar Form of Complex Numbers

VECTORS. Vectors OPTIONAL - I Vectors and three dimensional Geometry

CHAPTER 10 VECTORS POINTS TO REMEMBER

9.1 VECTORS. A Geometric View of Vectors LEARNING OBJECTIVES. = a, b

MR. YATES. Vocabulary. Quadratic Cubic Monomial Binomial Trinomial Term Leading Term Leading Coefficient

BSc (Hons) in Computer Games Development. vi Calculate the components a, b and c of a non-zero vector that is orthogonal to

Vectors and Matrices Lecture 2

Solutions for Chapter 3

Vectors for Physics. AP Physics C

CSC 470 Introduction to Computer Graphics. Mathematical Foundations Part 2

Math 215 HW #9 Solutions

Vectors Summary. can slide along the line of action. not restricted, defined by magnitude & direction but can be anywhere.

MT225 Homework 6 - Solution. Problem 1: [34] 5 ft 5 ft 5 ft A B C D. 12 kips. 10ft E F G

12.3 Dot Products, 12.4 Cross Products

RELATIVE MOTION ANALYSIS (Section 12.10)

VECTORS. Section 6.3 Precalculus PreAP/Dual, Revised /11/ :41 PM 6.3: Vectors in the Plane 1

ES 111 Mathematical Methods in the Earth Sciences Lecture Outline 3 - Thurs 5th Oct 2017 Vectors and 3D geometry

Written as per the revised G Scheme syllabus prescribed by the Maharashtra State Board of Technical Education (MSBTE) w.e.f. academic year

Calculus II - Basic Matrix Operations

APPLIED MECHANICS I Resultant of Concurrent Forces Consider a body acted upon by co-planar forces as shown in Fig 1.1(a).

9.1 VECTORS. A Geometric View of Vectors LEARNING OBJECTIVES. = a, b

The Cross Product of Two Vectors

Vectors. However, cartesian coordinates are really nothing more than a way to pinpoint an object s position in space

The Cross Product. Philippe B. Laval. Spring 2012 KSU. Philippe B. Laval (KSU) The Cross Product Spring /


MathCity.org Merging man and maths

2.1 Scalars and Vectors

Chapter 4. Motion in Two Dimensions

SUPPLEMENT I. Example. Graph the vector 4, 3. Definition. Given two points A(x 1, y 1 ) and B(x 2, y 2 ), the vector represented by # AB is # AB =,

HOMEWORK PROBLEMS FROM STRANG S LINEAR ALGEBRA AND ITS APPLICATIONS (4TH EDITION)

F F. proj cos( ) v. v proj v

xvi xxiii xxvi Construction of the Real Line 2 Is Every Real Number Rational? 3 Problems Algebra of the Real Numbers 7

Exercise Solutions for Introduction to 3D Game Programming with DirectX 10

Summer Mathematics Prep

Phys 221. Chapter 3. Vectors A. Dzyubenko Brooks/Cole

MATH 109 TOPIC 3 RIGHT TRIANGLE TRIGONOMETRY. 3a. Right Triangle Definitions of the Trigonometric Functions

OpenStax-CNX module: m Vectors. OpenStax College. Abstract

Math 259 Winter Solutions to Homework # We will substitute for x and y in the linear equation and then solve for r. x + y = 9.

Chapter 7 Introduction to vectors

The Cross Product. In this section, we will learn about: Cross products of vectors and their applications.

27 ft 3 adequately describes the volume of a cube with side 3. ft F adequately describes the temperature of a person.

Section 13.4 The Cross Product

9709 MATHEMATICS. 9709/32 Paper 3 (Pure Mathematics), maximum raw mark 75

Introduction to Vector Functions

Partial Fractions. Combining fractions over a common denominator is a familiar operation from algebra: 2 x 3 + 3

CALCULUS AB/BC SUMMER REVIEW PACKET

ADDITIONAL MATHEMATICS

EGR 1301 Introduction to Static Analysis

EXAM 1. OPEN BOOK AND CLOSED NOTES.

Unit #17: Spring Trig Unit. A. First Quadrant Notice how the x-values decrease by while the y-values increase by that same amount.

GCE214 Applied Mechanics-Statics. Lecture 04: 27/09/2017

SECTION 6.3: VECTORS IN THE PLANE

Trigonometry I. Pythagorean theorem: WEST VIRGINIA UNIVERSITY Physics

MATHEMATICS (SET -3) Labour cost Z 300x 400y (to be minimized) The constraints are: SECTION - A 1. f (x) is continuous at x 3 f (3) lim f (x)

Rigid Body Dynamics, SG2150 Solutions to Exam,

or i 2 = -1 i 4 = 1 Example : ( i ),, 7 i and 0 are complex numbers. and Imaginary part of z = b or img z = b

Physics Dynamics: Forces. Science and Mathematics Education Research Group

Chapter 2 A Mathematical Toolbox

VECTORS IN THREE DIMENSIONS

Omm Al-Qura University Dr. Abdulsalam Ai LECTURE OUTLINE CHAPTER 3. Vectors in Physics

Analytic Trigonometry. Copyright Cengage Learning. All rights reserved.

TRIGONOMETRY INTRODUCTION. Objectives. SESSION 1-5 ANGLES A positive angle measures a rotation in an anticlockwise direction.

Vectors. Examples of vectors include: displacement, velocity, acceleration, and force. Examples of scalars include: distance, speed, time, and volume.

e x for x 0. Find the coordinates of the point of inflexion and justify that it is a point of inflexion. (Total 7 marks)

Lecture Notes 3

Equality: Two matrices A and B are equal, i.e., A = B if A and B have the same order and the entries of A and B are the same.

Congruence Axioms. Data Required for Solving Oblique Triangles

7.2 Matrix Algebra. DEFINITION Matrix. D 21 a 22 Á a 2n. EXAMPLE 1 Determining the Order of a Matrix d. (b) The matrix D T has order 4 * 2.

Engineering Mechanics: Statics in SI Units, 12e Force Vectors

STEP II, ax y z = 3, 2ax y 3z = 7, 3ax y 5z = b, (i) In the case a = 0, show that the equations have a solution if and only if b = 11.

Physics 40 HW#3 Chapter 3 Problems from Knight you should do (but don t turn in): Ch 3 Problems: 7, 10, 15, 23, 33, 37, 40, 42, 43

Calculus with Analytic Geometry I Exam 10, Take Home Friday, November 8, 2013 Solutions.

General Physics I, Spring Vectors

Transcription:

Solutions Complete solutions to Miscellaneous Exercise. The unit vector, u, can be obtained by using (.5. u= ( 5i+ 7j+ 5 + 7 + 5 7 = ( 5i + 7j+ = i+ j+ 8 8 8 8. (i We have ( 3 ( 6 a+ c= i+ j + i j = i+ 3 j+ 6 = i+ j 7 (ii Similarly a+ b+ c+ d= i+ 3j + 7i+ + i j 6 + i j ( (iii ab = ( i+ 3j ( 7i+ = ( 7 + ( 3 + ( = = + 7 + i+ 3+ j+ + 6 = i+ j 6 (iv Since b a = a b = (v We first obtain b + c and then find the scalar product of a and b + c : b+ c= 7i+ + i j 6 = 7 i+ j+ 6 = 6i j+ 6 ( ( ( ( ( ( a b+ c = i+ 3j 6i j+ 6 = 6 + 3 + 6 = 3 (vi The unit vector, a ˆ, in the direction of a can be found by using (.5. aˆ = ( i+ 3j = ( i+ 3j + 3 + 4 ( Next we find the scalar product c d cd = i j 6 i j = + + 66= 55 ( ( Hence we have ( cda 55 55 3 55 ˆ = 55 ( 3 9.4 44. 4.7 4 i + j = + = + 4 i 4 j 4 i j (vii We have already found a + b + c + d in part (ii, so the magnitude is ( a+ b+ c+ d = i+ j = + + = 6 6.9 3. Let θ be the angle between v and a. We use cos( θ = va (* va Evaluating each of the components of (*: va = 4i 8j+ 4 i+ j+ 4 = 8 8+ 6= ( ( ( ( v = 4i 8j+ 4 = 4 + 8 + 4 = 96 a = i+ j+ 4 = + + 4 = Substituting these into (* gives cos( θ =, taing inverse cos θ ( = cos = 9 The velocity vector is perpendicular to the acceleration vector. (.5 u = a + b + c ( ai + bj + c

Solutions 4. Similar to solution 3. Use (* of solution 3: v a= 6i+ j 3i+ 7j = 6 3 + 7 = 3 ( v = i+ j = + = 6 6 4 a = i+ j = + = 3 7 3 7 58 Substituting these into (* 3-3 cos ( θ = which gives θ= cos = 48.37 4 58 4 58 5. We first place each force into polar form: 8 ( 45 and 7.6 5 Converting these forces into i and j components via calculator 8 ( 45 =.73i.73j 7.6 5 = 6.58i + 3.8j and adding gives the resultant force R as R = (.73 6.58 i+ (.73+ 3.8 j = 6.5i 8.93j 55.46 =.84 ( 55.46.84N 6. Similar to solution 5. Putting each force into polar form 5 5, 7.8 ( 45 and 3.6( 9 and then using a calculator gives the resultant force R as R = 5.34 8.9 5.34N R 8. 9 7. y using trigonometry we have F = 39.5cos( 53 x = 3.77 N (horizontal F = 39.5sin ( 53 y = 3.55 N (vertically down 8. dding each component i, j and separately gives: (a R = ( 3 + 6 + 3i + ( + 64 + 8j + ( 7 + +9 + = 63i + 69j + 48 (b R = ( +6 + 47 + i + ( + 99 + 84 + 4j + ( +9 + 88 + 3 = 86i + 5j + 9. Using (.5 we have wor done = ( i + j + 3 ( 5i + j = 5 + = 35J. We have O = i + 3j + 7 and O = 7i j + 37 Thus O = O O = O O = 7i j+ 37 i+ 3j+ 7 = 5i 4j+ 3 ( ( (.5 wor done = F r

Solutions 3 pplying (.5 gives wor done = i 7j+ 5i 4j+ 3 ( ( ( ( ( ( = 5 + 7 4 + 3 = 468 J. (a The position vectors in i, j and components of and are y (.5 we have wor done (b Similarly we have O = i + 7 j+, O = 3i+ 4j O ( ( = O O = 3i + 4j i+ 7j+ = i 3j = ( 3i j ( i 3j = 6 + 3 + 4 = 3J. O = 3i + 4j+ 3, O = 6i+ 7j 7 = O O = 6i+ 7j 7 3i+ 4j+ 3 = 3i+ 3j ( ( y (.5 wor done = i+ j 7 3i+ 3j = 6 + 3+ 7 = 49J (. We have = O O O = ( 3i + j+ 8 ( i 3j+ 7 F = i+ 4j+ Let M be the moment then by (.5 i j M = ( i+ 4j+ ( 5i j = det 4 5 4 4 = i det j det + det 5 5 = i ( 4+ j( 5 + ( = 3i+ 6j The magnitude of M is M = 3i+ 6j = 3 + 6 + =.5 N m 3. We have O ( ( = i + j + 3, O = 5i + j = O O = 5i+ j i+ j+ 3 = ( 5+ i + ( j+ ( 3 = 6i j 5 O ( ( The unit vector, u, in the direction of (.5 Wor done = F r (.5 Moment = r F is obtained by using:

Solutions 4 Thus u= i j = 6 ( ( 6 + + 5 ( 6 5 ( 6i j 5 39 6 5 9.7 4.95 4.77 N 6 F= ( i j = ( i j 4. We need to find F r + F r + F r 3 3 ( Each vector product is evaluated by using (.4: F r = ( i+ 3j 6 ( i+ j+ i j 3 6 6 3 = det 3 6 = i det j det + det = i 8 j 4 + 4 = 8i 4j 4 Similarly F r = 7i+ j+ 5 3i j ( ( i j 5 7 5 7 = det 7 5 = i det j det + det 3 3 3 = i 8 j 8 + 8 = 8i+ 8j+ 8 lso F3 r3 = j+ 3 i+ j ( ( i j 3 3 = det 3 = i det j det + det = i( 6 j( 6 + ( 4 = 6i+ 6j 4 Substituting these into ( : 8i 4j 4 + 8i+ 8j+ 8 + 6i+ 6j 4 = i+ j+ = 5. We have by (.4 i j r s= ( ai+ b ( ci+ d = det a b c d b a b a = i det j det + det d c d c = j + = ( ad cb j( cb ad i j a + b + c d + e + f = a b c d e f (.4 ( i j ( i j det

Solutions 5 6. Since the vectors are 9 to each other we have cos( 9 = = ab ab Thus the numerator, a b, must be zero. ab = i 3j+ x 3i+ j+ x = 6 3+ x = ( ( Rearranging and solving the quadratic x 9= = 9 x = 9 = 3, 3 The vectors a and b are 9 to each other if x = 3 or x = 3. 7. We need to write the exact value of cos( 45 : cos( 45 = We have ab = ab Rearranging gives ( x ab = ab (* We evaluate each component of (* ab = i+ j+ xi+ j = x+ = x+ ( ( Substituting these into (* gives Squaring both sides Rearranging Hence a = i+ j+ = + + = 3 ( b = xi+ j = x + + = x + ( x x + = 3 + ( x+ = ( x + ( x x x 9 4 + 4 + = 9 + 8 + + = + 8x 8x 9x 9x 8x 8x+ 8 = x 8x+ 6= ( x 8 4 = gives x=4 x = 4 gives an angle of 45 between the two vectors.