Patterns of Fields in Space

Slides:



Advertisements
Similar presentations
Conductors in Electrostatic Equilibrium
Advertisements

Announcements Monday guest lecturer: Dr. Fred Salsbury. Solutions now available online. Will strive to post lecture notes before class. May be different.
Lecture 6 Problems.
Continuous Charge Distributions
Conductors in Electrostatic Equilibrium
Week #3 Gauss’ Law September 7, What’s up Doc?? At this moment I do not have quiz grades unless I get them at the last minute. There was a short.
Copyright © 2009 Pearson Education, Inc. Chapter 21 Electric Charge and Electric Field.
Physics 2102 Lecture 4 Gauss’ Law II Physics 2102 Jonathan Dowling Carl Friedrich Gauss Version: 1/23/07 Flux Capacitor (Operational)
Chapter 23: Gauss’s Law Gauss’s Law is an alternative formulation of the relation between an electric field and the sources of that field in terms of electric.
4. Gauss’s law Units: 4.1 Electric flux Uniform electric field
Cut the charge distribution into pieces for which the field is known
Chapter 22 Patterns of Fields in Space Electric flux Gauss’s law Ampere’s law Maxwell equations.
From Chapter 23 – Coulomb’s Law
Gauss’ Law.
Divide shell into rings of charge, each delimited by the angle  and the angle  Use polar coordinates  r  Distance from center: d  r  Rcos.
Chapter 22 Patterns of Fields in Space Electric flux Gauss’s law Ampere’s law Maxwell equations.
Patterns of Fields in Space
a b c Gauss’ Law … made easy To solve the above equation for E, you have to be able to CHOOSE A CLOSED SURFACE such that the integral is TRIVIAL. (1)
Summer July Lecture 3 Gauss’s Law Chp. 24 Cartoon - Electric field is analogous to gravitational field Opening Demo - Warm-up problem Physlet /webphysics.davidson.edu/physletprob/webphysics.davidson.edu/physletprob.
Chapter 24 Gauss’s Law.
General Physics 2, Lec 5, By/ T.A. Eleyan 1 Additional Questions (Gauss’s Law)
Gauss’s law : introduction
Chapter 22 Gauss’s Law.
Chapter 21 Gauss’s Law. Electric Field Lines Electric field lines (convenient for visualizing electric field patterns) – lines pointing in the direction.
Summer July Lecture 3 Gauss’s Law Chp. 24 Cartoon - Electric field is analogous to gravitational field Opening Demo - Warm-up problem Physlet /webphysics.davidson.edu/physletprob/webphysics.davidson.edu/physletprob.
Chapter 24 Review on Chapter 23 From Coulomb's Law to Gauss’s Law
1 Lecture 3 Gauss’s Law Ch. 23 Physlet ch9_2_gauss/default.html Topics –Electric Flux –Gauss’
Copyright © 2009 Pearson Education, Inc. Chapter 22 Gauss’s Law.
ELECTRICITY PHY1013S GAUSS’S LAW Gregor Leigh
Tue. Feb. 3 – Physics Lecture #26 Gauss’s Law II: Gauss’s Law, Symmetry, and Conductors 1. Electric Field Vectors and Electric Field Lines 2. Electric.
د/ بديع عبدالحليم د/ بديع عبدالحليم
Physics 2102 Gauss’ law Physics 2102 Gabriela González Carl Friedrich Gauss
Patterns of Fields: Gauss’ Law, Ampere’s Law M&I Chapter 22.
Last Time Magnetic Torque Magnetic Dipole in a B-Field: Potential Energy 1.
Flux and Gauss’s Law Spring Last Time: Definition – Sort of – Electric Field Lines DIPOLE FIELD LINK CHARGE.
Copyright © 2009 Pearson Education, Inc. Applications of Gauss’s Law.
Slide 1Fig 24-CO, p.737 Chapter 24: Gauss’s Law. Slide 2 INTRODUCTION: In the preceding chapter we showed how to use Coulomb’s law to calculate the electric.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
24.2 Gauss’s Law.
Chapter 22 Gauss’s Law Electric charge and flux (sec & .3)
4. Gauss’s law Units: 4.1 Electric flux Uniform electric field
Gauss’s Law Basic Concepts Electric Flux Gauss’s Law
Physics 2102 Lecture: 04 THU 28 JAN
Electric flux To state Gauss’s Law in a quantitative form, we first need to define Electric Flux. # of field lines N = density of field lines x “area”
Physics 212 Lecture 4 Gauss’ Law.
Physics 2102 Lecture: 06 MON 26 JAN 08
Gauss’s Law Gauss’s law uses symmetry to simplify electric field calculations. Gauss’s law also gives us insight into how electric charge distributes itself.
Gauss’s Law ENROLL NO Basic Concepts Electric Flux
Electric Flux & Gauss Law
4. Gauss’s law Units: 4.1 Electric flux Uniform electric field
Chapter 22 Gauss’s Law.
Electric flux To state Gauss’s Law in a quantitative form, we first need to define Electric Flux. # of field lines N = density of field lines x “area”
Reading: Chapter 28 For r > a Gauss’s Law.
Flux and Gauss’s Law Spring 2009.
Last Lectures This lecture Gauss’s law Using Gauss’s law for:
TOPIC 3 Gauss’s Law.
Chapter 21 Gauss’s Law.
Flux Capacitor (Schematic)
C. less, but not zero. D. zero.
Physics 2113 Lecture: 11 MON 09 FEB
Chapter 22 Gauss’s Law HW 4: Chapter 22: Pb.1, Pb.6, Pb.24,
Last Lectures This lecture Gauss’s law Using Gauss’s law for:
Question for the day Can the magnitude of the electric charge be calculated from the strength of the electric field it creates?
4. Gauss’s law Units: 4.1 Electric flux Uniform electric field
Chapter 24 - Summary Gauss’s Law.
Norah Ali Al-moneef King Saud university
Electric flux To state Gauss’s Law in a quantitative form, we first need to define Electric Flux. # of field lines N = density of field lines x “area”
Using Gauss’ Law From flux to charge.
Magnetic Forces in Moving Reference Frames
Gauss’s Law: applications
Presentation transcript:

Patterns of Fields in Space Chapter 22 Patterns of Fields in Space Electric flux Gauss’s law Ampere’s law Maxwell equations

Patterns of Fields in Space What is in the box? no charges? vertical charged plate? Gauss’s law: If we know the field distribution on closed surface we can tell what is inside.

Electric Flux: Surface Area flux through small area: Definition of electric flux on a surface:

Adding up the Flux

Gauss’s Law Features: 1. Proportionality constant 2. Size and shape independence 3. Independence on number of charges inside 4. Charges outside contribute zero

1. Gauss’s Law: Proportionality Constant For negative charge cos is negative What if charge is negative? Works at least for one charge and spherical surface

2. Gauss’s Law: The Size of the Surface universe would be much different if exponent was not exactly 2!

3. Gauss’s Law: The Shape of the Surface All elements of the outer surface can be projected onto corresponding areas on the inner sphere with the same flux

4. Gauss’s Law: Outside Charges – Outside charges contribute 0 to total flux

5. Gauss’s Law: Superposition

Gauss’s Law Is it a law or a theorem? Can derive one from another Last shown. Gauss’s law is more universal: works at relativistic speeds

Clicker Question What is the net electric flux on the box? 0 V*m

Applications of Gauss’s Law Knowing E can conclude what is inside Knowing charges inside can conclude what is E

The Electric Field of a Large Plate Symmetry: Field must be perpendicular to surface Eleft=Eright Start here. Could be a sheet of charge or a metal plate with charge Q/A on each side. Assumption: we are finding the field in a region far from the plate edges.

The Electric Field of a Uniform Spherical Shell of Charge Symmetry: Field should be radial The same at every location on spherical surface A. Outer sphere: B. Inner sphere:

The Electric Field of a Uniform Cube Is Gauss’s law still valid? Can we find E using Gauss’s law?

Clicker Question What is the electric flux through the area A? E = 100 V/m q = 30o DA = 2 m2 100 V*m 173 V*m 50 V*m 87 V*m c

Gauss’s Law: Properties of Metal Can we have excess charge inside a metal that is in static equilibrium? Proof by contradiction: =0

Gauss’s Law: Hole in a Metal =0 What is electric field inside the hole? = Less formal: imagine solid piece of metal. remove some (hole) – there are no excess charges, no field – so nothing changes. Is the metal itself as shown electrically neutral? No, apparently, it has a net + charge. No charges on the surface of an empty hole E is zero inside a hole

Gauss’s Law: Screening Similar to a hole in the metal

Gauss’s Law: Charges Inside a Hole =0 +5nC

Gauss’s Law: Circuits Can we have excess charge inside in steady state? We already have established that in steady state for a uniform conductor, the E-field is the same magnitude and follows the wire. Thus, Gauss’s law gives no net flux and hence no net charge contained within the conductor. But current carriers are all negative. Where does the positive charge reside?

Gauss’s Law: Junction Between two Wires i1=i2 n1Au1E1 = n2Au2E2 There is negative charge along the interface! n2<n1 u2<u1 Take Gaussian surface just inside the conductor since we are not interested in surface charges. We’ve already shown that within each uniform conductor there is no charge.