Chapter 18 Section 18.4 Another Notation for Line Integrals.

Slides:



Advertisements
Similar presentations
The divergence of E If the charge fills a volume, with charge per unit volume . R Where d is an element of volume. For a volume charge:
Advertisements

Section 18.4 Path-Dependent Vector Fields and Green’s Theorem.
09-1 Physics I Class 09 Potential Energy and Conservation of Energy.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 21.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 14.
12-1 Physics I Class 12 Conservative Forces and Potential Energy.
EEE340Lecture Helmholtz’s Theorem Helmholtz’s Theorem: A vector field (vector point function) is determined to within an additive constant if.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 22.
22-1 Physics I Class 22 Electric Potential Work Integral in Multiple Dimensions (Review)
20-1 Physics I Class 20 Electric Potential Work Integral in Multiple Dimensions (Review)
Quiz #1 30/30 congratulations 1)AL-AMER, AHMAD ADNAN MOHA 2)AL-AGEELI, AHMAD IBRAHIM 3)AL-GARNI, BANDAR HASSAN S 4)AL-ARJANI, ALI SAEED ABDU 5)AL-BUGMI,
Line integrals (10/22/04) :vector function of position in 3 dimensions. :space curve With each point P is associated a differential distance vector Definition.
12-1 Physics I Class 12 Potential Energy and Conservation of Energy.
Prof. David R. Jackson ECE Dept. Fall 2014 Notes 4 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM Group University of Houston 1.
MA Day 51 – March 26, 2013 Section 13.1: (finish) Vector Fields Section 13.2: Line Integrals.
1 April 14 Triple product 6.3 Triple products Triple scalar product: Chapter 6 Vector Analysis A B C + _.
Linear Momentum and Collisions المحاضرة العاشرة. Linear Momentum and Collisions Chapter 9.
WORK The work dW done on a particle displaced along differential path dr, by an object exerting force F is defined as A B F dr The SI unit of work is 1J.
MA Day 55 – April 4, 2013 Section 13.3: The fundamental theorem for line integrals – Review theorems – Finding Potential functions – The Law of.
Chapter 15 Vector Analysis. Copyright © Houghton Mifflin Company. All rights reserved.15-2 Definition of Vector Field.
Section 18.1 The Idea of a Line Integral. If you can imagine having a boat in our gulf stream example from last chapter, depending on which direction.
Vector Calculus 13. The Fundamental Theorem for Line Integrals 13.3.
1. CIRCUIT TERMINOLOGY CIRCUITS by Ulaby & Maharbiz.
Dr. Hugh Blanton ENTC Energy & Potential Dr. Blanton - ENTC Energy & Potential 3 The work done, or energy expended, in moving any object.
EMLAB Chapter 4. Potential and energy 1. EMLAB 2 Solving procedure for EM problems Known charge distribution Coulomb’s law Known boundary condition Gauss’
Dr. Wang Xingbo Fall , 2005 Mathematical & Mechanical Method in Mechanical Engineering.
Advanced Higher Physics Electric Potential. Electric Potential 1 V = work done / q(measured in J C -1 ) Defined as ‘the work done per unit positive charge.
Lecture 3: Line Integrals We start with two (atypical) examples where integrand is (i) a scalar field, integrated w.r.t. a scalar In general, it’s the.
Chapter 16 – Vector Calculus 16.3 The Fundamental Theorem for Line Integrals 1 Objectives:  Understand The Fundamental Theorem for line integrals  Determine.
MA Day 53 – April 2, 2013 Section 13.2: Finish Line Integrals Begin 13.3: The fundamental theorem for line integrals.
Chapter 7: Linear Momentum Along with conservation of energy, we will now include other conserved quantities of linear and angular momentum. Linear momentum.
Main Menu Salas, Hille, Etgen Calculus: One and Several Variables Copyright 2003 © John Wiley & Sons, Inc. All rights reserved. Line Integrals a. Definition.
 From our studies of work and energy (Chaps. 7 & 8), we know that when a force acts on an object and displaces it, work is done on the object  This also.
Copyright © 2011 Pearson Education, Inc. Publishing as Pearson Addison-Wesley Chapter 14 Vector Calculus.
Work, Energy and Power Ms Houts AP Physics C Chapters 7 & 8.
The Fundamental Theorem for Line Integrals
Section 18.3 Gradient Fields and Path- Independent Fields.
1 Electric Potential Reading: Chapter 29 Chapter 29.
Constant Electromagnetic Field Section 19. Constant fields E and H are independent of time t.  and A can be chosen time independent, too.
Impulse and Momentum. Definition of Linear Momentum The linear momentum of an object is defined to be the product of its _____ and its ________ Linear.
Problem 3 p. 45 Electric potential on ring’s axis From Chapter 2:
CHAPTER 14 Vector Calculus Slide 2 © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 14.1VECTOR FIELDS 14.2LINE INTEGRALS.
Chapter 25 Electric Potential.
Conservative and Non- Conservative Forces Hey—where did the energy go? § 7.3.
6. Work and Energy Work Definitions: This is line integral Example: Find work done by a force on a particle that is moving from the origin to the point.
1 Honors Physics 1 Class 10 Fall 2013 Potential Energy Partial Derivatives The Gradient.
Chapter 6 Vector Analysis
Integration in Vector Fields
Force as gradient of potential energy
Section 3.7 – Potential Energy
Notes 4 ECE 3318 Applied Electricity and Magnetism Spring 2017
16.3 Vector Fields Understand the concept of a vector field
Chapter 25 Electric Potential.
Physics I Class 20 Electric Potential.
Properties of Gradient Fields
Math 265 Created by Educational Technology Network
Chapter 6 Vector Analysis
Potential Energy and Conservation of Energy
Christopher Crawford PHY
Instructor: Dr. Tatiana Erukhimova
Chapter 29 Electric Potential Reading: Chapter 29.
Copyright © Cengage Learning. All rights reserved.
ECE 329 Problems HKN Spring 2017 Exam 1.
Electric Potential.
Chapter 17: Line Integrals and Surface Integrals
Energy Transformations and Conservation
Electricity and Magnetism
Electricity and Magnetism
Physics 319 Classical Mechanics
Presentation transcript:

Chapter 18 Section 18.4 Another Notation for Line Integrals

Path Independence An integral is said to be path independent (or independent of path) if any two paths with the same initial and terminal points have the value of the integral over those paths equal. Conservative Vector Fields A vector field is conservative if energy is conserved along any path in the vector field. That is the energy expended moving to any position along any path is equal to the energy required to return to the same position along any other path possibly different path. The function that has the vector field as its gradient represents the potential energy and is called the potential function.

All of these have analogues statements for 3 dimensions.

x y