Physics 2B. Lecture 24B. Gauss 10 Deutsche Mark

Similar documents
Electric Flux. If we know the electric field on a Gaussian surface, we can find the net charge enclosed by the surface.

Look over. Examples 11, 12, 2/3/2008. Read over Chapter 23 sections 1-9 Examples 1, 2, 3, 6. 1) What a Gaussian surface is.

PHYSICS. Chapter 24 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT

Gauss s Law. Lecture 3. Chapter Course website:

Chapter 22 Gauss s Law

3/22/2016. Chapter 27 Gauss s Law. Chapter 27 Preview. Chapter 27 Preview. Chapter Goal: To understand and apply Gauss s law. Slide 27-2.

Gauss s Law. Lecture 4. Chapter 27. Channel 61 (clicker) Physics II

Physics 202, Lecture 3. The Electric Field

Electric Flux and Gauss s Law

PHY102 Electricity Topic 3 (Lectures 4 & 5) Gauss s Law

Motion of a charged particle in an electric field. Electric flux

Chapter 23. Gauss Law. Copyright 2014 John Wiley & Sons, Inc. All rights reserved.

Gauss s Law. Chapter 22. Electric Flux Gauss s Law: Definition. Applications of Gauss s Law

Chapter 24. Gauss s Law

Electric Field Lines. lecture 4.1.1

Lecture 4-1 Physics 219 Question 1 Aug Where (if any) is the net electric field due to the following two charges equal to zero?

PH 222-2C Fall Gauss Law. Lectures 3-4. Chapter 23 (Halliday/Resnick/Walker, Fundamentals of Physics 8 th edition)

Phys102 General Physics II. Chapter 24: Gauss s Law

Chapter 21: Gauss law Tuesday September 13 th. Gauss law and conductors Electrostatic potential energy (more likely on Thu.)

Chapter 24. Gauss s Law

Questions Chapter 23 Gauss' Law

CH 23. Gauss Law. A. Gauss law relates the electric fields at points on a (closed) Gaussian surface to the net charge enclosed by that surface.

Chapter 2 Gauss Law 1

Chapter 23. Gauss s Law

The Basic Definition of Flux

IMPORTANT: LABS START NEXT WEEK

Ch 24 Electric Flux, & Gauss s Law

Lecture 3. Electric Field Flux, Gauss Law

Quiz. Chapter 15. Electrical Field. Quiz. Electric Field. Electric Field, cont. 8/29/2011. q r. Electric Forces and Electric Fields

24 Gauss s Law. Gauss s Law 87:

Lecture 3. Electric Field Flux, Gauss Law. Last Lecture: Electric Field Lines

Gauss s Law. Phys102 Lecture 4. Key Points. Electric Flux Gauss s Law Applications of Gauss s Law. References. SFU Ed: 22-1,2,3. 6 th Ed: 16-10,+.

Chapter 21 Chapter 23 Gauss Law. Copyright 2014 John Wiley & Sons, Inc. All rights reserved.

Chapter 22: Gauss s Law

Gauss s Law. Name. I. The Law: , where ɛ 0 = C 2 (N?m 2

Chapter 23: Gauss Law. PHY2049: Chapter 23 1

Essential University Physics

Gauss s Law. The first Maxwell Equation A very useful computational technique This is important!

How to define the direction of A??

Physics 202, Exam 1 Review

Physics 1B Electricity & Magne4sm

Module 2 : Electrostatics Lecture 7 : Electric Flux

More Gauss, Less Potential

IClicker question. We have a negative charge q=-e. How electric field is directed at point X? q=-e (negative charge) X A: B: C: D: E: E=0

E. not enough information given to decide

Physics 9 WS E3 (rev. 1.0) Page 1

Chapter 24. Gauss s Law

LECTURE 15 CONDUCTORS, ELECTRIC FLUX & GAUSS S LAW. Instructor: Kazumi Tolich

Electric Flux. To investigate this, we have to understand electric flux.

Physics Lecture: 09

Gauss s Law & Potential

AP Physics C - E & M

Chapter 28. Gauss s Law

Potential & Potential Energy

Worksheet for Exploration 24.1: Flux and Gauss's Law

Physics 202, Exam 1 Review

Chapter (2) Gauss s Law

Electricity & Magnetism Lecture 4: Gauss Law

Chapter 22 Gauss s law. Electric charge and flux (sec &.3) Gauss s Law (sec &.5) Charges on conductors (sec. 22.6)

PHYS 1441 Section 002 Lecture #6

Quiz Fun! This box contains. 1. a net positive charge. 2. no net charge. 3. a net negative charge. 4. a positive charge. 5. a negative charge.

Electric Field and Gauss s law. January 17, 2014 Physics for Scientists & Engineers 2, Chapter 22 1

Electric Field Lines

Physics Lecture 13

Phys 2102 Spring 2002 Exam 1

week 3 chapter 28 - Gauss s Law

Electric flux. Electric Fields and Gauss s Law. Electric flux. Flux through an arbitrary surface

Electrostatics. Electrical properties generated by static charges. Introduction

Chapter 22 Gauss s Law. Copyright 2009 Pearson Education, Inc.

Chapter 2. Electrostatics. Introduction to Electrodynamics, 3 rd or 4 rd Edition, David J. Griffiths

Chapter 24 Gauss Law

Chapter 21: Gauss s Law

2 Which of the following represents the electric field due to an infinite charged sheet with a uniform charge distribution σ.

Chapter 22 Gauss s Law. Copyright 2009 Pearson Education, Inc.

Gauss s Law. 3.1 Quiz. Conference 3. Physics 102 Conference 3. Physics 102 General Physics II. Monday, February 10th, Problem 3.

Lecture 9 Electric Flux and Its Density Gauss Law in Integral Form

Gauss Law 1. Name Date Partners GAUSS' LAW. Work together as a group on all questions.

Lecture 13. PHYC 161 Fall 2016

Course Updates. Reminders: 1) Quiz today. 2) Written problems: 21.96, 22.6, 22.58, ) Complete Chapter 22 (all this information on web page)

free space (vacuum) permittivity [ F/m]

1. ELECTRIC CHARGES AND FIELDS

Reading: Chapter 28. 4πε r. For r > a. Gauss s Law

FLUX OF VECTOR FIELD INTRODUCTION

Chapter 4. Electrostatic Fields in Matter

Conductors: External Electric Field 1/28/2018 1

University Physics (Prof. David Flory) Chapt_24 Sunday, February 03, 2008 Page 1

Chapter 24. Gauss s Law

Flux. Flux = = va. This is the same as asking What is the flux of water through the rectangle? The answer depends on:

Physics 202: Spring 1999 Solution to Homework Assignment #3

3: Gauss s Law July 7, 2008

AP Physics C. Gauss s Law. Free Response Problems

PHYS102 - Gauss s Law.

Welcome. to Electrostatics

Physics 11b Lecture #3. Electric Flux Gauss s Law

Chapter 15. Electric Forces and Electric Fields

Chapter 15. Electric Forces and Electric Fields

Fall 2004 Physics 3 Tu-Th Section

Experiment III Electric Flux

A) 1, 2, 3, 4 B) 4, 3, 2, 1 C) 2, 3, 1, 4 D) 2, 4, 1, 3 E) 3, 2, 4, 1. Page 2

Electric Flux and Gauss Law

Transcription:

Physics 2B Lecture 24B Gauss 10 Deutsche Mark

Electric Flux Flux is the amount of something that flows through a given area. Electric flux, Φ E, measures the amount of electric field lines that passes through a given area. If I were to measure the flux originating from this Van de Graaff generator through this surface, what would I have to take into account? How big the area is. How strong the electric field is. The angle between the area and the electric field.

Electric Flux In order to better understand the angle between E and A, we define the direction of the area A by a normal to A. Electric flux will depend on E, A, and θ (where θ is the angle between E and the normal to A). For a uniform electric field:

Electric Flux Unfortunately, all electric fields are not uniform: In this case, we look at a small area element da and measure the electric flux through it. To get the entire flux over the surface we need to sum up all the small area elements (integrate):

Electric Flux An imaginary sheet is known as an open surface. This is because nothing can possibly be enclosed by it. It is far more useful to deal with the electric flux from what is known as a closed surface. A closed surface is one that encloses a small volume and has no openings (it distinctly divides a space into inside and outside regions). Examples of a closed surface are spheres, boxes, and cylinders.

Electric Flux In electrostatics, a closed surface that an electric field passes through is known as a Gaussian surface. Note: a Gaussian is an imaginary surface; it does not necessarily coincide with a physical object. The convention becomes that lines exiting the surface are positive and the lines entering are considered negative.

Gauss Law If we try to find the electric flux through the Gaussian surface we change our integral to: where the loop on the integral sign means we take the integration over the entire closed surface. Gauss Law states that the electric flux through any closed surface is equal to the net charge, Q inside, inside the surface divided by the constant ε o. where ε o = 8.85x10 12 C 2 /(Nm 2 ) and is called the permittivity of free space.

Gauss Law What if there were no charges present inside the closed Gaussian surface, what would the electric flux be? The amount of field lines that enter the surface equal the amount of field lines that leave the surface. This leads to a net electric flux of zero. But if a net positive charge is present, then there is a source of electric field lines and the electric flux cannot be zero.

Applications of Gauss Law The power of Gauss Law is to use the net charge enclosed in a surface to find the electric field at a certain distance (or vice versa). The trick comes in finding a proper Gaussian surface. If you are looking for the electric field from a configuration of charges, you would like to choose a surface in which the electric field is constant (in magnitude) at all points on the surface. This allows you to pull E out of the integral.

Gauss Law Example Use Gauss Law to find the electric field a distance r from a lone positive point charge +q. Answer Define a coordinate system. Choose the point charge as r = 0. Any outward distance would be positive.

Gauss Law Answer If we are going to use Gauss Law we must choose a Gaussian surface. Since this problem has spherical symmetry (it doesn t matter which direction you travel outward), use a spherical Gaussian surface. Next, apply Gauss s Law. How much charge is located inside the Gaussian sphere? +q.

Gauss Law Answer Next turning to the definition of electric flux. Since the electric field is constant in magnitude at all points on the Gaussian surface and da is always parallel to E, we can pull it out of the integral. Taking the surface integral:

Answer Equate the two terms: Gauss Law This corresponds to our original Coulomb s Law and validates the results.

Example What is the electric field, E, a distance L above an infinite thin sheet of charge with surface density, σ. Gauss Law Answer Choose an appropriate Gaussian surface. Take a cylindrical surface with length L and faces of area A.

Answer Gauss Law The electric field is perpendicular to both faces of the cylinder. So the total flux through both faces is: There is no flux through the wall of the cylinder because the field vectors are tangent to the wall. Leaving the net flux to be (LHS of Gauss Law):

Answer Gauss Law Next, we should find the amount of charge contained in the Gaussian surface. The surface charge density will be: That is charge enclosed by the Gaussian surface (RHS of Gauss Law).

Gauss Law There are three fundamental symmetries that you exploit in order to use Gauss Law to solve for a given electric field: Planar, Cylindrical, and Spherical.

For Next Time (FNT) Study for Quiz 1 Start reading Chapter 25