Electricity and Magnetism

Slides:



Advertisements
Similar presentations
Chapter 21 Electric Charge and Electric Field. Charles Allison © 2000 Question An  particle with a charge +2e and a mass of 4m p is on a collision course.
Advertisements

Electric Charges and Electric Fields
AP Physics C Montwood High School R. Casao
CHAPTER 23 : ELECTRIC FIELDS
Chapter 24 Gauss’s Law.
Electric Charge, Force, and Field
Chapter 24 Gauss’s Law.
Chapter 24 Gauss’s Law.
Physics for Scientists and Engineers II, Summer Semester 2009 Lecture 2: May 20 th 2009 Physics for Scientists and Engineers II.
Chapter 23 Summer 1996, Near the University of Arizona Chapter 23 Electric Fields.
Physics 1502: Lecture 2 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Chapter 21 & 22 Electric Charge Coulomb’s Law This force of repulsion or attraction due to the charge properties of objects is called an electrostatic.
Question A) B) C) D) E An electric field polarizes a metal block as shown.
Magnetic Forces and Fields. Magnetic Force Right Hand Rule: Cross Product.
Chapter 22 Gauss’s Law. Charles Allison © Motion of a Charged Particle in an Electric Field The force on an object of charge q in an electric.
Chapter 22: Electric Fields
Gauss’s law : introduction
1 Electric Field – Continuous Charge Distribution As the average separation between source charges is smaller than the distance between the charges and.
Electricity and Magnetism Review 1: Units 1-6
Copyright © 2009 Pearson Education, Inc. Lecture 4 – Electricity & Magnetism (Electrostatics) a. Electric Charge, Electric Field & Gauss’ Law.
1 Gauss’s Law For r > a Reading: Chapter Gauss’s Law Chapter 28.
Electric Forces and Fields: Coulomb’s Law
ELEC 3105 Lecture 1 Coulomb. 4. Electrostatics Applied EM by Ulaby, Michielssen and Ravaioli.
Previous Lectures: Introduced to Coulomb’s law Learnt the superposition principle Showed how to calculate the electric field resulting from a series of.
Chapter 24 Gauss’s Law. Let’s return to the field lines and consider the flux through a surface. The number of lines per unit area is proportional to.
Lecture 5 R 2R2R Yesterday we introduced electric field lines Today we will cover some extra topics on Electric Fields before going on to Electric Flux.
PHYS 241 Exam 1 Review Kevin Ralphs. Overview General Exam Strategies Concepts Practice Problems.
Physics 2113 Lecture 08: MON 02 FEB Electric Fields III Physics 2113 Jonathan Dowling Charles-Augustin de Coulomb ( )
Electric field Chapter 22 Week-2 Electric Fields In this chapter we will introduce the concept of an electric field. As long as charges are stationary.
Copyright © 2009 Pearson Education, Inc. Chapter 22 Gauss’s Law.
Question. Question A) B) C) D) E An electric field polarizes a metal.
Electric Field-Intro Electric force is a field force. Field forces can act through space, i.e. requires no physical contact. Faraday developed the concept.
ELECTROMAGNETIS M LECTURE#04 Instructor: Muhammad Mateen Yaqoob.
Chapter 24 Gauss’s Law. Intro Gauss’s Law is an alternative method for determining electric fields. While it stem’s from Coulomb’s law, Gauss’s law is.
Physics 2102 Lecture: 03 TUE 26 JAN
Electric Potential Chapter 25 The Electric Potential
Electric Potential.
Electrostatics Chapter Properties of Physical Objects Mass/Inertial: – Gravity mass: inertia in gravitational interaction – Kinetic mass: inertia.
Conductor, insulator and ground. Force between two point charges:
3/21/20161 ELECTRICITY AND MAGNETISM Phy 220 Chapter2: Gauss’s Law.
Chapter 22 Electric Fields The Electric Field: The Electric Field is a vector field. The electric field, E, consists of a distribution of vectors,
Charles Allison © 2000 Chapter 22 Gauss’s Law.. Charles Allison © 2000 Problem 57.
Review on Coulomb’s Law and the electric field definition
Electric Fields Due to Continuous Charge Distributions
Electric Forces and Fields AP Physics C. Electrostatic Forces (F) (measured in Newtons) q1q1 q2q2 k = 9 x 10 9 N*m 2 /C 2 This is known as “Coulomb’s.
Chapter 25 Electric Potential.
Copyright © 2009 Pearson Education, Inc. Applications of Gauss’s Law.
Electric Fields Due to Continuous Charge Distributions
ELEC 3105 Lecture 1 Coulomb.
Problem-Solving Guide for Gauss’s Law
Gauss’s Law ENROLL NO Basic Concepts Electric Flux
Chapter 22 Electric Fields.
Review Physics /10/2018 Lecture XXIV.
Physics 122B Electricity and Magnetism
PHYS 1444 – Section 003 Lecture #5
ELECTRIC FIELD ELECTRIC FLUX Lectures 3, 4 & 5 a a R 2R
Reading: Chapter 28 For r > a Gauss’s Law.
ELECTRIC FIELD ELECTRIC FLUX Lectures 3, 4 & 5 a a R 2R
AP Physics C: Electricity & Magnetism – Charges & Electric Field
The Electric Field Chapter 23.
A charge distribution lies along a segment of the positive x axis
Physics 2102 Lecture: 04 WED 21 JAN
Lecture 19 Maxwell equations E: electric field intensity
Physics 2113 Lecture 07: WED 09 SEP
We, the course instructors,
Chapter 22 Gauss’s Law Chapter 22 opener. Gauss’s law is an elegant relation between electric charge and electric field. It is more general than Coulomb’s.
Electric Fields From Continuous Distributions of Charge
Chapter 22 Gauss’s Law Chapter 22 opener. Gauss’s law is an elegant relation between electric charge and electric field. It is more general than Coulomb’s.
Physics 122B Electricity and Magnetism
Coulomb’s Law Performing electric field calculations on charge distributions in an X-Y coordinate Plane.
Presentation transcript:

Electricity and Magnetism Chapter 26 Electricity and Magnetism Electric Field: Continuous Charge Distribution

Find electric field at point P. Continuous Charge Distribution P

Electric Field: Continuous Charge Distribution In this situation, the system of charges can be modeled as continuous The system of closely spaced charges is equivalent to a total charge that is continuously distributed along some line, over some surface, or throughout some volume

Electric Field: Continuous Charge Distribution The total electric charge is Q. What is the electric field at point P ? P P linear volume Q P Q surface Q

Continuous Charge Distribution: Charge Density The total electric charge is Q. Volume V Linear, length L Q Amount of charge in a small volume dl: Q Amount of charge in a small volume dV: Linear charge density Volume charge density Surface, area A Amount of charge in a small volume dA: Q Surface charge density

Electric Field: Continuous Charge Distribution Procedure: Divide the charge distribution into small elements, each of which contains Δq Calculate the electric field due to one of these elements at point P Evaluate the total field by summing the contributions of all the charge elements Symmetry: take advantage of any symmetry to simplify calculations For the individual charge elements Because the charge distribution is continuous

Electric Field: Symmetry no symmetry no symmetry no symmetry

Electric Field: Symmetry The symmetry gives us the direction of resultant electric field

Electric Field: Continuous Charge Distribution What is the electric field at point P ? - linear charge density

1. Symmetry determines the direction of the electric field. What is the electric field at point P ? - linear charge density 1. Symmetry determines the direction of the electric field.

What is the electric field at point P ? - linear charge density 2. Divide the charge distribution into small elements, each of which contains Δq

What is the electric field at point P ? - linear charge density 3. Evaluate the total field by summing the contributions of all the charge elements Δq Replace Sum by Integral

4. Evaluate the integral What is the electric field at point P ? - linear charge density 4. Evaluate the integral

What is the electric field at point P ? - linear charge density From symmetry Replace the Sum by Integral

1. Symmetry determines the direction of the electric field. What is the electric field at point P ? - surface charge density 1. Symmetry determines the direction of the electric field.

What is the electric field at point P ? - surface charge density 2. Divide the charge distribution into small elements, each of which contains Δq 3. Evaluate the total field by summing the contributions of all the charge elements Δq Approach A: straightforward at point (x,y)

Approach A What is the electric field at point P ? - surface charge density Replace the Sum by Integral at point

Approach A What is the electric field at point P ? - surface charge density Evaluate the Integral at point

Approach B What is the electric field at point P ? - surface charge density Charge of the ring Linear density of the ring Ring of width Length of the ring

Electric Field: Symmetry no symmetry no symmetry no symmetry

no symmetry, but we know and

no symmetry We do not know the direction of electric field at point P We need to find x and y component of electric field Then Then

no symmetry We do not know the direction of electric field at point P We need to find x and y component of electric field the symmetry tells us that one of the component is 0, so we do not need to calculate it.

Important Example Find electric field

Important Example Find electric field

Important Example

Motion of Charged Particle

Motion of Charged Particle When a charged particle is placed in an electric field, it experiences an electrical force If this is the only force on the particle, it must be the net force The net force will cause the particle to accelerate according to Newton’s second law - Coulomb’s law - Newton’s second law

Motion of Charged Particle What is the final velocity? - Coulomb’s law - Newton’s second law Motion in x – with constant velocity Motion in x – with constant acceleration - travel time After time t the velocity in y direction becomes then