Last Lectures This lecture Gauss’s law Using Gauss’s law for:

Slides:



Advertisements
Similar presentations
Announcements Monday guest lecturer: Dr. Fred Salsbury. Solutions now available online. Will strive to post lecture notes before class. May be different.
Advertisements

Applications of Gauss’s Law
Lecture 6 Problems.
Continuous Charge Distributions
Conductors in Electrostatic Equilibrium
Physics 2102 Lecture 4 Gauss’ Law II Physics 2102 Jonathan Dowling Carl Friedrich Gauss Version: 1/23/07 Flux Capacitor (Operational)
Hw: All Chapter 5 problems and exercises. Test 1 results Average 75 Median 78 >90>80>70>60>50
A Charged, Thin Sheet of Insulating Material
Electricity and Magnetism
Hw: All Chapter 5 problems and exercises. Outline Applications of Gauss’s Law - The single Fixed Charge -Field of a sphere of charge -Field of a spherical.
From Chapter 23 – Coulomb’s Law
Short Version : 21. Gauss’s Law Electric Field Lines Electric field lines = Continuous lines whose tangent is everywhere // E. They begin at +
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.
Electric Field Lines - a “map” of the strength of the electric field. The electric field is force per unit charge, so the field lines are sometimes called.
III.A 3, Gauss’ Law.
22 Electric Field II Covering sections 1-5 (omit section 6)
1 Lecture 3 Gauss’s Law Ch. 23 Physlet ch9_2_gauss/default.html Topics –Electric Flux –Gauss’
Application of Gauss’ Law to calculate Electric field:
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.
Physics 2102 Gauss’ law Physics 2102 Gabriela González Carl Friedrich Gauss
Physics 2113 Lecture: 09 MON 14 SEP
Physics 212 Lecture 4, Slide 1 Physics 212 Lecture 4 Today's Concepts: Conductors + Using Gauss’ Law Applied to Determine E field in cases of high symmetry.
Gauss’s Law (II) Examples: charged spherical shell, infinite plane, long straight wire Review: For a closed surface S: Net outward flux through S.
Fig 24-CO, p.737 Chapter 24: Gauss’s Law قانون جاوس 1- Electric Flux 2- Gauss’s Law 3-Application of Gauss’s law 4- Conductors in Electrostatic Equilibrium.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
+q r A A) |E| = kq/r2, to left B) kq/r2 > |E| > 0, to left
24.2 Gauss’s Law.
Electric Forces and Electric Fields
Ch 24 – Gauss’s Law Karl Friedrich Gauss
Electric Forces and Electric Fields
Physics 2102 Lecture: 04 THU 28 JAN
Cultural enlightenment time. Conductors in electrostatic equilibrium.
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
Day 5: Objectives Electric Field Lines
Problem-Solving Guide for Gauss’s Law
Gauss’s Law ENROLL NO Basic Concepts Electric Flux
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”
Gauss’s Law Electric Flux
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)
E. not enough information given to decide Gaussian surface #1
C. less, but not zero. D. zero.
Gauss’s Law Electric Flux
Symmetry Some charge distributions have translational, rotational, or reflective symmetry. If this is the case, we can determine something about the field.
Physics 2113 Lecture: 11 MON 09 FEB
Chapter 23 Gauss’s Law.
Electricity and Magnetism
Question for the day Can the magnitude of the electric charge be calculated from the strength of the electric field it creates?
Gauss’s Law (II) Examples: charged spherical shell, infinite plane,
The Electric Flux The electric flux measures the amount of electric field passing through a surface of area A whose normal to the surface is tilted at.
From last time… Motion of charged particles
Last Lecture This lecture Gauss’s law Using Gauss’s law for:
Physics 2102 Lecture 05: TUE 02 FEB
Norah Ali Al-moneef King Saud university
Chapter 23 Gauss’ Law Key contents Electric flux
Phys102 Lecture 3 Gauss’s Law
Chapter 23 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”
Conductors A conductor is a material in which charges can move relatively freely. Usually these are metals (Au, Cu, Ag, Al). Excess charges (of the same.
Gauss’s law This lecture was given mostly on the board so these slides are only a guide to what was done.
Using Gauss’ Law From flux to charge.
Gauss’s Law: applications
Electricity and Magnetism
Chapter 23 Gauss’s Law.
Presentation transcript:

Last Lectures This lecture Gauss’s law Using Gauss’s law for: spherical symmetry line symmetry plane symmetry This lecture Conductors in electric fields

21.6 Charges on Conductors electrostatic equilibrium

A Gaussian surface completely within the conductor. Since E must be zero inside conductor, the net flux through this surface must be zero.

EXAMPLE: (a) shows a cross section of a spherical metal shell of inner radius R. A point charge of –5.0 C is located at a distance R/2 from the centre of the shell. If the shell is electrically neutral, what are the (induced) charges on its inner and outer surfaces? Are those charges uniformly distributed? What is the field pattern inside and outside the shell? Key Idea: Electric field is zero inside metal and thus on Gaussian surface. Key Idea: Shell is electrically neutral. Electrons move from inner surface to outer surface and spread out uniformly

Assess: What does this charge distribution look like from far away? Example 21.7 There is a hollow cavity inside a conductor. The conductor itself has a charge of 1 μC, and there is a 2 μC charge inside the cavity. Find the net charge on the outer surface of the conductor, assuming electrostatic equilibrium. Assess: What does this charge distribution look like from far away?

NB E is always perpendicular to the surface Field at the surface of a conductor NB E is always perpendicular to the surface WHY? More on this with potential

Now use Gauss’s law to find E just outside a conductor surface Field at the surface of a conductor Now use Gauss’s law to find E just outside a conductor surface (field at conductor surface)

Field at the surface of a conductor

Two oppositely charged conducting plates Field at the surface of a conductor Two oppositely charged conducting plates

Try these again! True A True or False? If the net electric flux out of a closed surface is zero, the electric field must be zero everywhere on the surface. If the net electric flux out of a closed surface is zero, the charge density must be zero everywhere inside the surface. The electric field is zero everywhere within the material of a conductor in electrostatic equilibrium. The tangential component of the electric field is zero at all points just outside the surface of a conductor in electrostatic equilibrium. The normal component of the electric field is the same at all points just outside the surface of a conductor in electrostatic equilibrium. False F False False True True False Try these again!