The rotation of a particle about an axis is specified by 2 pieces of information
|
|
- Barnard Caldwell
- 5 years ago
- Views:
Transcription
1 1 How to specify rotational motion The rotation of a particle about an axis is specified by 2 pieces of information 1) The direction of the axis of rotation 2) A magnitude of how fast the particle is "going round" the axis of rotation. Question : What mathematical object has both direction and magnitude? Answer :
2 Hence we may specify rotational motion by a single angular velocity vector such that a) The magnitude = angular speed b) points in the direction of the axis of rotation Question : Is this enough? Answer :
3 2. Right - hand convention 1) Take the right hand. 2) Wrap fingers in the direction of rotation. 3) Thumb points in direction of the angular velocity vector. Exercise : Which way does point?
4 3. Rotational motion in 3-d Question : In circular motion v = R. How do we generalize to 3-d? Z A R O r(t) Y P X
5 Z A R P O r(t) Y 1) R = AP = r sin X 2) speed of P, v = R = r sin 3) v is perpendicular to r and
6 Hence (using right hand convention) for rotational motion v = dr / dt = x r This is the generalization of the formula for circular motion
7 Common misconceptions 1. 3d - all quantities are vectors! v = x r 2.. Vector cross product not scalar multiplication! a) Order is important b) v x r 3. Position vector not radius of circle! Advice : Purge scalar formula v = r from memory
8 Exercise : For circular motion in the XY plane the position vector r(t) = {R cos t, R sin t, 0} Y a) Find the angular velocity vector b) Using find the velocity vector v X a) = b) v = x r Note : Compare with dr/dt
9 4 Rotating axes system Definition An axes system oxyz is said to be rotating with respect to a fixed axes system OXYZ if Z 1) The origin of both axes systems coincide 2) The orientation of the ox, oy and oz axes are all changing with the same angular velocity vector. x O = o z y Y Question : What happens if they don t? X
10 Implications 1) Since the orientation of the oxyz changes cannot ignore di/dt, dj/dt and dk/dt 2) What s di/dt, dj/dt and dk/dt? Hint : dr/dt = v = x r for rotation Hence di / dt = dj / dt = dk / dt = x i x j x k
11 5 Differentiating a vector expressed in terms of a rotating frame Given basis vectors of rotating frame i, j, k position vector of a particle P, r(t) = x(t) i + y(t) j + z(t) k angular velocity vector of the rotating frame (t) = x (t) i + y (t) j + z (t) k Show that the absolute velocity of P is dr/dt = x ' (t) i + y ' (t) j + z ' (t) k + x r Question : Does this make sense? What happens if is 0?
12 1. Position vector r(t) = x(t) i + y(t) j + z(t) k 2. Absolute velocity v = dr(t) / dt = dx/dt i + x di/dt + dy/dt j + y dj/dt + dz/dt k + z dk/dt 3. Use di/dt = x i dj/dt = x j dk/dt = x k
13 Substituting... v = dx/dt i + x ( x i) + dy/dt j + y ( x j) + dz/dt k + z ( x k) 4) Regroup terms v = dx/dt i + dy/dt j + + dz/dt k + x (xi + y j + z k) 5. Hence v = r + x r
14 6 How to find absolute acceleration for a rotating frame Denote r ' (t) = x ' (t) i + y ' (t) j + z ' (t) k r '' (t) = x '' (t) i + y '' (t) j + z '' (t) k where i, j, k are the basis vectors of a rotating frame Show that the absolute acceleration d 2 r/dt 2 = r '' + ' x r + x ( x r ) + 2 x r '
15 v = dr/dt = r + x r a = dv/dt = v + x v = (r ' + ( x r ) ) + x (r ' + ( x r ) ) = r '' + ' x r + 2 x r ' + x ( x r )
16 Exercise : Circular motion using rotating axes The particle P rotates about the OZ axis with angular speed (t) rad/s. OP = R m. The axes i j k rotates with the particle. a) Find the absolute velocity and acceleration of P using the rotating axes axes i j k. J b) Compare the derivation with j the one using the (t) rad/s fixed axes I J K. i P O = o R I Fixed
17 J j (t) rad/s i rotating R O = o I Fixed 1. Position vector r = 2. Angular velocity = 3. Absolute velocity v = dr/dt = r + x r =
18 4. Absolute acceleration a = dv/dt = v + x v = = Identify the terms
CURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS
CURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS Today s Objectives: Students will be able to: 1. Describe the motion of a particle traveling along a curved path. 2. Relate kinematic quantities in
More informationCURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS
CURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS Today s Objectives: Students will be able to: 1. Describe the motion of a particle traveling along a curved path. 2. Relate kinematic quantities in
More informationCURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS
CURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS Today s Objectives: Students will be able to: 1. Describe the motion of a particle traveling along a curved path. 2. Relate kinematic quantities in
More informationCURVILINEAR MOTION: RECTANGULAR COMPONENTS (Sections )
CURVILINEAR MOTION: RECTANGULAR COMPONENTS (Sections 12.4-12.5) Today s Objectives: Students will be able to: a) Describe the motion of a particle traveling along a curved path. b) Relate kinematic quantities
More informationThe Calculus of Vec- tors
Physics 2460 Electricity and Magnetism I, Fall 2007, Lecture 3 1 The Calculus of Vec- Summary: tors 1. Calculus of Vectors: Limits and Derivatives 2. Parametric representation of Curves r(t) = [x(t), y(t),
More informationCURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS APPLICATIONS
CURVILINEAR MOTION: GENERAL & RECTANGULAR COMPONENTS Today s Objectives: Students will be able to: 1. Describe the motion of a particle traveling along a curved path. 2. Relate kinematic quantities in
More informationMotion in Two or Three Dimensions
Chapter 3 Motion in Two or Three Dimensions PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 3 To use vectors
More informationFind the slope of the curve at the given point P and an equation of the tangent line at P. 1) y = x2 + 11x - 15, P(1, -3)
Final Exam Review AP Calculus AB Find the slope of the curve at the given point P and an equation of the tangent line at P. 1) y = x2 + 11x - 15, P(1, -3) Use the graph to evaluate the limit. 2) lim x
More informationMATH 280 Multivariate Calculus Fall Integrating a vector field over a curve
MATH 280 Multivariate alculus Fall 2012 Definition Integrating a vector field over a curve We are given a vector field F and an oriented curve in the domain of F as shown in the figure on the left below.
More informationAn Overview of Mechanics
An Overview of Mechanics Mechanics: The study of how bodies react to forces acting on them. Statics: The study of bodies in equilibrium. Dynamics: 1. Kinematics concerned with the geometric aspects of
More informationTangent and Normal Vector - (11.5)
Tangent and Normal Vector - (.5). Principal Unit Normal Vector Let C be the curve traced out by the vector-valued function rt vector T t r r t t is the unit tangent vector to the curve C. Now define N
More informationOHSx XM521 Multivariable Differential Calculus: Homework Solutions 14.1
OHSx XM5 Multivariable Differential Calculus: Homework Solutions 4. (8) Describe the graph of the equation. r = i + tj + (t )k. Solution: Let y(t) = t, so that z(t) = t = y. In the yz-plane, this is just
More informationMath 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.
Math 234 What you should know on day one August 28, 2001 1 You should be able to use general principles like Length = ds, Area = da, Volume = dv For example the length of the semi circle x = cos t, y =
More informationMTHE 227 Problem Set 2 Solutions
MTHE 7 Problem Set Solutions 1 (Great Circles). The intersection of a sphere with a plane passing through its center is called a great circle. Let Γ be the great circle that is the intersection of the
More information3 = arccos. A a and b are parallel, B a and b are perpendicular, C a and b are normalized, or D this is always true.
Math 210-101 Test #1 Sept. 16 th, 2016 Name: Answer Key Be sure to show your work! 1. (20 points) Vector Basics: Let v = 1, 2,, w = 1, 2, 2, and u = 2, 1, 1. (a) Find the area of a parallelogram spanned
More informationPHYS 211 Lecture 9 - Examples of 3D motion 9-1
PHYS 211 Lecture 9 - Examples of 3D motion 9-1 Lecture 9 - Examples of 3D motion Text: Fowles and Cassiday, Chap. 4 In one dimension, the equations of motion to be solved are functions of only one position
More informationBasics of rotational motion
Basics of rotational motion Motion of bodies rotating about a given axis, like wheels, blades of a fan and a chair cannot be analyzed by treating them as a point mass or particle. At a given instant of
More informationName: ID: Math 233 Exam 1. Page 1
Page 1 Name: ID: This exam has 20 multiple choice questions, worth 5 points each. You are allowed to use a scientific calculator and a 3 5 inch note card. 1. Which of the following pairs of vectors are
More informationChapter 4. Motion in Two Dimensions
Chapter 4 Motion in Two Dimensions Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail Will treat projectile motion and uniform circular motion
More informationOverview of vector calculus. Coordinate systems in space. Distance formula. (Sec. 12.1)
Math 20C Multivariable Calculus Lecture 1 1 Coordinates in space Slide 1 Overview of vector calculus. Coordinate systems in space. Distance formula. (Sec. 12.1) Vector calculus studies derivatives and
More informationIntroduction to Vector Functions
Introduction to Vector Functions Differentiation and Integration Philippe B. Laval KSU Today Philippe B. Laval (KSU) Vector Functions Today 1 / 14 Introduction In this section, we study the differentiation
More informationChapter 4. Motion in Two Dimensions
Chapter 4 Motion in Two Dimensions Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail Will treat projectile motion and uniform circular motion
More informationAnnouncements. Introduction and Rectilinear Kinematics: Continuous Motion - Sections
Announcements Week-of-prayer schedule (10:45-11:30) Introduction and Rectilinear Kinematics: Continuous Motion - Sections 12.1-2 Today s Objectives: Students will be able to find the kinematic quantities
More informationTopic 2-2: Derivatives of Vector Functions. Textbook: Section 13.2, 13.4
Topic 2-2: Derivatives of Vector Functions Textbook: Section 13.2, 13.4 Warm-Up: Parametrization of Circles Each of the following vector functions describe the position of an object traveling around the
More informationChapter 4. Motion in Two Dimensions
Chapter 4 Motion in Two Dimensions Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail Will treat projectile motion and uniform circular motion
More informationSection 4.3 Vector Fields
Section 4.3 Vector Fields DEFINITION: A vector field in R n is a map F : A R n R n that assigns to each point x in its domain A a vector F(x). If n = 2, F is called a vector field in the plane, and if
More informationVECTORS. Given two vectors! and! we can express the law of vector addition geometrically. + = Fig. 1 Geometrical definition of vector addition
VECTORS Vectors in 2- D and 3- D in Euclidean space or flatland are easy compared to vectors in non- Euclidean space. In Cartesian coordinates we write a component of a vector as where the index i stands
More informationCURVILINEAR MOTION: CYLINDRICAL COMPONENTS
CURVILINEAR MOTION: CYLINDRICAL COMPONENTS Today s Objectives: Students will be able to: 1 Determine velocity and acceleration components using cylindrical coordinates In-Class Activities: Check Homework
More informationChapter 14: Vector Calculus
Chapter 14: Vector Calculus Introduction to Vector Functions Section 14.1 Limits, Continuity, Vector Derivatives a. Limit of a Vector Function b. Limit Rules c. Component By Component Limits d. Continuity
More informationMath 2433 Notes Week The Dot Product. The angle between two vectors is found with this formula: cosθ = a b
Math 2433 Notes Week 2 11.3 The Dot Product The angle between two vectors is found with this formula: cosθ = a b a b 3) Given, a = 4i + 4j, b = i - 2j + 3k, c = 2i + 2k Find the angle between a and c Projection
More informationSOLUTIONS TO SECOND PRACTICE EXAM Math 21a, Spring 2003
SOLUTIONS TO SECOND PRACTICE EXAM Math a, Spring 3 Problem ) ( points) Circle for each of the questions the correct letter. No justifications are needed. Your score will be C W where C is the number of
More informationChapter 4. Motion in Two Dimensions. With modifications by Pinkney
Chapter 4 Motion in Two Dimensions With modifications by Pinkney Kinematics in Two Dimensions covers: the vector nature of position, velocity and acceleration in greater detail projectile motion a special
More informationPLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION Today s Objectives : Students will be able to: 1. Analyze the kinematics of a rigid body undergoing planar translation or rotation about a fixed axis. In-Class
More information5.2 LENGTHS OF CURVES & AREAS OF SURFACES OF REVOLUTION
5.2 Arc Length & Surface Area Contemporary Calculus 1 5.2 LENGTHS OF CURVES & AREAS OF SURFACES OF REVOLUTION This section introduces two additional geometric applications of integration: finding the length
More informationChapter 4. Motion in Two Dimensions. Professor Wa el Salah
Chapter 4 Motion in Two Dimensions Kinematics in Two Dimensions Will study the vector nature of position, velocity and acceleration in greater detail. Will treat projectile motion and uniform circular
More informationRotational Motion and Torque
Rotational Motion and Torque Introduction to Angular Quantities Sections 8- to 8-2 Introduction Rotational motion deals with spinning objects, or objects rotating around some point. Rotational motion is
More informationExam 3. MA 114 Exam 3 Fall Multiple Choice Questions. 1. Find the average value of the function f (x) = 2 sin x sin 2x on 0 x π. C. 0 D. 4 E.
Exam 3 Multiple Choice Questions 1. Find the average value of the function f (x) = sin x sin x on x π. A. π 5 π C. E. 5. Find the volume of the solid S whose base is the disk bounded by the circle x +
More informationPractice Problems for Exam 3 (Solutions) 1. Let F(x, y) = xyi+(y 3x)j, and let C be the curve r(t) = ti+(3t t 2 )j for 0 t 2. Compute F dr.
1. Let F(x, y) xyi+(y 3x)j, and let be the curve r(t) ti+(3t t 2 )j for t 2. ompute F dr. Solution. F dr b a 2 2 F(r(t)) r (t) dt t(3t t 2 ), 3t t 2 3t 1, 3 2t dt t 3 dt 1 2 4 t4 4. 2. Evaluate the line
More informationDepartment of Physics, Korea University
Name: Department: Notice +2 ( 1) points per correct (incorrect) answer. No penalty for an unanswered question. Fill the blank ( ) with (8) if the statement is correct (incorrect).!!!: corrections to an
More informationIntroduction to Vector Functions
Introduction to Vector Functions Limits and Continuity Philippe B Laval KSU Spring 2012 Philippe B Laval (KSU) Introduction to Vector Functions Spring 2012 1 / 14 Introduction In this section, we study
More informationExam 1 Review SOLUTIONS
1. True or False (and give a short reason): Exam 1 Review SOLUTIONS (a) If the parametric curve x = f(t), y = g(t) satisfies g (1) = 0, then it has a horizontal tangent line when t = 1. FALSE: To make
More informationMOTION IN TWO OR THREE DIMENSIONS
MOTION IN TWO OR THREE DIMENSIONS 3 Sections Covered 3.1 : Position & velocity vectors 3.2 : The acceleration vector 3.3 : Projectile motion 3.4 : Motion in a circle 3.5 : Relative velocity 3.1 Position
More informationFirst Year Physics: Prelims CP1. Classical Mechanics: Prof. Neville Harnew. Problem Set III : Projectiles, rocket motion and motion in E & B fields
HT017 First Year Physics: Prelims CP1 Classical Mechanics: Prof Neville Harnew Problem Set III : Projectiles, rocket motion and motion in E & B fields Questions 1-10 are standard examples Questions 11-1
More informationHyperbolic Analytic Geometry
Chapter 6 Hyperbolic Analytic Geometry 6.1 Saccheri Quadrilaterals Recall the results on Saccheri quadrilaterals from Chapter 4. Let S be a convex quadrilateral in which two adjacent angles are right angles.
More information(1) Recap of Differential Calculus and Integral Calculus (2) Preview of Calculus in three dimensional space (3) Tools for Calculus 3
Math 127 Introduction and Review (1) Recap of Differential Calculus and Integral Calculus (2) Preview of Calculus in three dimensional space (3) Tools for Calculus 3 MATH 127 Introduction to Calculus III
More informationSemester University of Sheffield. School of Mathematics and Statistics
University of Sheffield School of Mathematics and Statistics MAS140: Mathematics (Chemical) MAS152: Civil Engineering Mathematics MAS152: Essential Mathematical Skills & Techniques MAS156: Mathematics
More informationAP Calculus Chapter 3 Testbank (Mr. Surowski)
AP Calculus Chapter 3 Testbank (Mr. Surowski) Part I. Multiple-Choice Questions (5 points each; please circle the correct answer.). If f(x) = 0x 4 3 + x, then f (8) = (A) (B) 4 3 (C) 83 3 (D) 2 3 (E) 2
More informationRIGID BODY MOTION (Section 16.1)
RIGID BODY MOTION (Section 16.1) There are cases where an object cannot be treated as a particle. In these cases the size or shape of the body must be considered. Rotation of the body about its center
More informationCircular motion. Aug. 22, 2017
Circular motion Aug. 22, 2017 Until now, we have been observers to Newtonian physics through inertial reference frames. From our discussion of Newton s laws, these are frames which obey Newton s first
More informationPhysics 201, Lecture 8
Physics 01, Lecture 8 Today s Topics q Physics 01, Review 1 q Important Notes: v v v v This review is not designed to be complete on its own. It is not meant to replace your own preparation efforts Exercises
More informationProperties of surfaces II: Second moment of area
Properties of surfaces II: Second moment of area Just as we have discussing first moment of an area and its relation with problems in mechanics, we will now describe second moment and product of area of
More informationUNIT NUMBER 8.2. VECTORS 2 (Vectors in component form) A.J.Hobson
JUST THE MATHS UNIT NUMBER 8.2 VECTORS 2 (Vectors in component form) by A.J.Hobson 8.2.1 The components of a vector 8.2.2 The magnitude of a vector in component form 8.2.3 The sum and difference of vectors
More informationDownloaded from 3. Motion in a straight line. Study of motion of objects along a straight line is known as rectilinear motion.
3. Motion in a straight line IMPORTANT POINTS Study of motion of objects along a straight line is known as rectilinear motion. If a body does not change its position with time it is said to be at rest.
More informationHandout 6: Rotational motion and moment of inertia. Angular velocity and angular acceleration
1 Handout 6: Rotational motion and moment of inertia Angular velocity and angular acceleration In Figure 1, a particle b is rotating about an axis along a circular path with radius r. The radius sweeps
More informationCALCULUS 3 February 6, st TEST
MATH 400 (CALCULUS 3) Spring 008 1st TEST 1 CALCULUS 3 February, 008 1st TEST YOUR NAME: 001 A. Spina...(9am) 00 E. Wittenbn... (10am) 003 T. Dent...(11am) 004 J. Wiscons... (1pm) 005 A. Spina...(1pm)
More information9.5. Lines and Planes. Introduction. Prerequisites. Learning Outcomes
Lines and Planes 9.5 Introduction Vectors are very convenient tools for analysing lines and planes in three dimensions. In this Section you will learn about direction ratios and direction cosines and then
More informationChapter 10: Rotation. Chapter 10: Rotation
Chapter 10: Rotation Change in Syllabus: Only Chapter 10 problems (CH10: 04, 27, 67) are due on Thursday, Oct. 14. The Chapter 11 problems (Ch11: 06, 37, 50) will be due on Thursday, Oct. 21 in addition
More information1.1 Single Variable Calculus versus Multivariable Calculus Rectangular Coordinate Systems... 4
MATH2202 Notebook 1 Fall 2015/2016 prepared by Professor Jenny Baglivo Contents 1 MATH2202 Notebook 1 3 1.1 Single Variable Calculus versus Multivariable Calculus................... 3 1.2 Rectangular Coordinate
More informationJUST THE MATHS UNIT NUMBER INTEGRATION APPLICATIONS 10 (Second moments of an arc) A.J.Hobson
JUST THE MATHS UNIT NUMBER 13.1 INTEGRATION APPLICATIONS 1 (Second moments of an arc) by A.J.Hobson 13.1.1 Introduction 13.1. The second moment of an arc about the y-axis 13.1.3 The second moment of an
More informationMathematics Engineering Calculus III Fall 13 Test #1
Mathematics 2153-02 Engineering Calculus III Fall 13 Test #1 Instructor: Dr. Alexandra Shlapentokh (1) Which of the following statements is always true? (a) If x = f(t), y = g(t) and f (1) = 0, then dy/dx(1)
More informationA B Ax Bx Ay By Az Bz
Lecture 5.1 Dynamics of Rotation For some time now we have been discussing the laws of classical dynamics. However, for the most part, we only talked about examples of translational motion. On the other
More informationMath 241, Exam 1 Information.
Math 241, Exam 1 Information. 2/13/13, LC 310, 11:15-12:05. Exam 1 will be based on: Sections 12.1-12.5, 14.2. The corresponding assigned homework problems (see http://www.math.sc.edu/ boylan/sccourses/241sp13/241.html)
More informationNormal Force. W = mg cos(θ) Normal force F N = mg cos(θ) F N
Normal Force W = mg cos(θ) Normal force F N = mg cos(θ) Note there is no weight force parallel/down the include. The car is not pressing on anything causing a force in that direction. If there were a person
More informationEngineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Kinematics
Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Kinematics Module 10 - Lecture 24 Kinematics of a particle moving on a curve Today,
More informationINTEGRAL CALCULUS DIFFERENTIATION UNDER THE INTEGRAL SIGN: Consider an integral involving one parameter and denote it as
INTEGRAL CALCULUS DIFFERENTIATION UNDER THE INTEGRAL SIGN: Consider an integral involving one parameter and denote it as, where a and b may be constants or functions of. To find the derivative of when
More informationINTRODUCTION & RECTILINEAR KINEMATICS: CONTINUOUS MOTION
INTRODUCTION & RECTILINEAR KINEMATICS: CONTINUOUS MOTION (Sections 12.1-12.2) Today s Objectives: Students will be able to find the kinematic quantities (position, displacement, velocity, and acceleration)
More informationMath 461 Homework 8. Paul Hacking. November 27, 2018
Math 461 Homework 8 Paul Hacking November 27, 2018 (1) Let S 2 = {(x, y, z) x 2 + y 2 + z 2 = 1} R 3 be the sphere with center the origin and radius 1. Let N = (0, 0, 1) S 2 be the north pole. Let F :
More informationVector Calculus, Maths II
Section A Vector Calculus, Maths II REVISION (VECTORS) 1. Position vector of a point P(x, y, z) is given as + y and its magnitude by 2. The scalar components of a vector are its direction ratios, and represent
More information43.1 Vector Fields and their properties
Module 15 : Vector fields, Gradient, Divergence and Curl Lecture 43 : Vector fields and their properties [Section 43.1] Objectives In this section you will learn the following : Concept of Vector field.
More informationMath 461 Homework 8 Paul Hacking November 27, 2018
(1) Let Math 461 Homework 8 Paul Hacking November 27, 2018 S 2 = {(x, y, z) x 2 +y 2 +z 2 = 1} R 3 be the sphere with center the origin and radius 1. Let N = (0, 0, 1) S 2 be the north pole. Let F : S
More informationProblem Set. Assignment #1. Math 3350, Spring Feb. 6, 2004 ANSWERS
Problem Set Assignment #1 Math 3350, Spring 2004 Feb. 6, 2004 ANSWERS i Problem 1. [Section 1.4, Problem 4] A rocket is shot straight up. During the initial stages of flight is has acceleration 7t m /s
More informationChapter 10: Rotation
Chapter 10: Rotation Review of translational motion (motion along a straight line) Position x Displacement x Velocity v = dx/dt Acceleration a = dv/dt Mass m Newton s second law F = ma Work W = Fdcosφ
More informationf. D that is, F dr = c c = [2"' (-a sin t)( -a sin t) + (a cos t)(a cost) dt = f2"' dt = 2
SECTION 16.4 GREEN'S THEOREM 1089 X with center the origin and radius a, where a is chosen to be small enough that C' lies inside C. (See Figure 11.) Let be the region bounded by C and C'. Then its positively
More informationWinmeen Tnpsc Group 1 & 2 Study Materials
10. Motion - 2 1. What is datum? We take a point on the ground and we measure all distances with respect to this point which we call the datum. 2. What is frame of reference? The three imaginary lines
More informationChap. 3: Kinematics (2D) Recap: Kinematics (1D) 1. Vector Kinematics 2. Projectile Motion 3. Uniform Circular Motion 4.
Chap. 3: Kinematics (2D) Recap: Kinematics (1D) 1. Vector Kinematics 2. Projectile Motion 3. Uniform Circular Motion 4. Relative Velocity 1 Last, This and Next Weeks [Last Week] Chap. 1 and Chap. 2 [This
More informationDEPARTMENT OF MATHEMATICS AND STATISTICS UNIVERSITY OF MASSACHUSETTS. MATH 233 SOME SOLUTIONS TO EXAM 1 Fall 2018
DEPARTMENT OF MATHEMATICS AND STATISTICS UNIVERSITY OF MASSACHUSETTS MATH SOME SOLUTIONS TO EXAM 1 Fall 018 Version A refers to the regular exam and Version B to the make-up 1. Version A. Find the center
More informationFROM NEWTON TO KEPLER. One simple derivation of Kepler s laws from Newton s ones.
italian journal of pure and applied mathematics n. 3 04 (393 400) 393 FROM NEWTON TO KEPLER. One simple derivation of Kepler s laws from Newton s ones. František Mošna Department of Mathematics Technical
More informationName: SOLUTIONS Date: 11/9/2017. M20550 Calculus III Tutorial Worksheet 8
Name: SOLUTIONS Date: /9/7 M55 alculus III Tutorial Worksheet 8. ompute R da where R is the region bounded by x + xy + y 8 using the change of variables given by x u + v and y v. Solution: We know R is
More informationTangent and Normal Vectors
Tangent and Normal Vectors MATH 311, Calculus III J. Robert Buchanan Department of Mathematics Fall 2011 Navigation When an observer is traveling along with a moving point, for example the passengers in
More informationThe first term involves the cross product of two parallel vectors and so it vanishes. We then get
Physics 3550 Angular Momentum. Relevant Sections in Text: 3.4, 3.5 Angular Momentum You have certainly encountered angular momentum in a previous class. The importance of angular momentum lies principally
More informationLecture for Week 6 (Secs ) Derivative Miscellany I
Lecture for Week 6 (Secs. 3.6 9) Derivative Miscellany I 1 Implicit differentiation We want to answer questions like this: 1. What is the derivative of tan 1 x? 2. What is dy dx if x 3 + y 3 + xy 2 + x
More informationForce Due to Magnetic Field You will use
Force Due to Magnetic Field You will use Units: 1 N = 1C(m/s) (T) A magnetic field of one tesla is very powerful magnetic field. Sometimes it may be convenient to use the gauss, which is equal to 1/10,000
More informationMATH1013 Calculus I. Derivatives II (Chap. 3) 1
MATH1013 Calculus I Derivatives II (Chap. 3) 1 Edmund Y. M. Chiang Department of Mathematics Hong Kong University of Science & Technology October 16, 2013 2013 1 Based on Briggs, Cochran and Gillett: Calculus
More informationChapter 4 - Motion in 2D and 3D
Never confuse motion with action. - Benjamin Franklin David J. Starling Penn State Hazleton PHYS 211 Position, displacement, velocity and acceleration can be generalized to 3D using vectors. x(t) r(t)
More informationAngles and Applications
CHAPTER 1 Angles and Applications 1.1 Introduction Trigonometry is the branch of mathematics concerned with the measurement of the parts, sides, and angles of a triangle. Plane trigonometry, which is the
More informationLecture D4 - Intrinsic Coordinates
J. Peraire 16.07 Dynamics Fall 2004 Version 1.1 Lecture D4 - Intrinsic Coordinates In lecture D2 we introduced the position, velocity and acceleration vectors and referred them to a fixed cartesian coordinate
More informationRotational Kinematics
Rotational Kinematics Rotational Coordinates Ridged objects require six numbers to describe their position and orientation: 3 coordinates 3 axes of rotation Rotational Coordinates Use an angle θ to describe
More informationVectors. J.R. Wilson. September 28, 2017
Vectors J.R. Wilson September 28, 2017 This chapter introduces vectors that are used in many areas of physics (needed for classical physics this year). One complication is that a number of different forms
More informationKinematics. Chapter Multi-Body Systems
Chapter 2 Kinematics This chapter first introduces multi-body systems in conceptual terms. It then describes the concept of a Euclidean frame in the material world, following the concept of a Euclidean
More informationPhysics 114A Introduction to Mechanics (without calculus)
Physics 114A Introduction to Mechanics (without calculus) A course about learning basic physics concepts and applying them to solve real-world, quantitative, mechanical problems Lecture 6 Review of Vectors
More informationPhysics I (Navitas) EXAM #1 Fall 2015
95.141 Physics I (Navitas) EXAM #1 Fall 2015 Name, Last Name First Name Student Identification Number: Write your name at the top of each page in the space provided. Answer all questions, beginning each
More informationDifferential Vector Calculus
Contents 8 Differential Vector Calculus 8. Background to Vector Calculus 8. Differential Vector Calculus 7 8.3 Orthogonal Curvilinear Coordinates 37 Learning outcomes In this Workbook you will learn about
More informationVectors and 2D Kinematics. AIT AP Physics C
Vectors and 2D Kinematics Coordinate Systems Used to describe the position of a point in space Coordinate system consists of a fixed reference point called the origin specific axes with scales and labels
More informationMotion Part 4: Projectile Motion
Motion Part 4: Projectile Motion Last modified: 28/03/2017 CONTENTS Projectile Motion Uniform Motion Equations Projectile Motion Equations Trajectory How to Approach Problems Example 1 Example 2 Example
More information5.1. Accelerated Coordinate Systems:
5.1. Accelerated Coordinate Systems: Recall: Uniformly moving reference frames (e.g. those considered at 'rest' or moving with constant velocity in a straight line) are called inertial reference frames.
More information9.4 CALCULUS AND PARAMETRIC EQUATIONS
9.4 Calculus with Parametric Equations Contemporary Calculus 1 9.4 CALCULUS AND PARAMETRIC EQUATIONS The previous section discussed parametric equations, their graphs, and some of their uses for visualizing
More informationMATH 32A: MIDTERM 2 REVIEW. sin 2 u du z(t) = sin 2 t + cos 2 2
MATH 3A: MIDTERM REVIEW JOE HUGHES 1. Curvature 1. Consider the curve r(t) = x(t), y(t), z(t), where x(t) = t Find the curvature κ(t). 0 cos(u) sin(u) du y(t) = Solution: The formula for curvature is t
More informationPhysics 141 Rotational Motion 1 Page 1. Rotational Motion 1. We're going to turn this team around 360 degrees.! Jason Kidd
Physics 141 Rotational Motion 1 Page 1 Rotational Motion 1 We're going to turn this team around 360 degrees.! Jason Kidd Rigid bodies To a good approximation, a solid object behaves like a perfectly rigid
More informationUNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH
UNIVERSITY of LIMERICK OLLSCOIL LUIMNIGH College of Informatics and Electronics END OF SEMESTER ASSESSMENT PAPER MODULE CODE: MS4613 SEMESTER: Autumn 2002/03 MODULE TITLE: Vector Analysis DURATION OF EXAMINATION:
More information3.2 Systems of Two First Order Linear DE s
Agenda Section 3.2 Reminders Lab 1 write-up due 9/26 or 9/28 Lab 2 prelab due 9/26 or 9/28 WebHW due 9/29 Office hours Tues, Thurs 1-2 pm (5852 East Hall) MathLab office hour Sun 7-8 pm (MathLab) 3.2 Systems
More information