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For more information, please see full course syllabus of AP Physics C/Electricity and Magnetism
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Lecture Comments (5)

1 answer

Last reply by: Richard Kennesson
Sun Mar 11, 2018 12:20 AM

Post by babu wanyeki on March 1, 2014

On the second extra example when he is finding the time he is assuming that the velocity is constant and doesn't consider the downward acceleration which would make the time bigger.

0 answers

Post by Werner Heisenberg on December 27, 2013

In extra example 1, did you forget to put the value of g (9.8) in the equation? or did I miss something out?

0 answers

Post by yannick Haberkorn on October 12, 2013

what if the permitivity of the vacuum = some number x for example 12 or three how would you apply the formula k*Q1*q2/r^2 ?

0 answers

Post by Troy Franckowiak on February 12, 2011

Great lectures :)

One question I have concerning electrostatic equilibrium: When you talk about making a cavity within a spherical conductor you say that no electric field exists within the cavity itself. However, could charge accumulate on the surface outlining the cavity of the sphere?

Related Articles:

Electric Field

  • Electric charges produce an electric field that fills the space. To find the value of the electric field E at a point, we place a very small point charge q at that point and measure the force F acting on the point charge; the electric field is then given by E = F / q. Note that the electric field is a vector, since F is a vector.
  • The electric field produced by a point charge Q at a distance r has a magnitude E = kQ/r^2. The field is directed radially outward if Q is positive and radially inward if Q is negative.
  • The electric field produced by a collection of point charges is equal to the vector sum of the fields produced by the individual point charges.
  • Between the plates of a charged parallel-plate capacitor, E = σ / ε0, where σ is the surface charge density on the plates and ε0 is the permittivity of free space.
  • Electric field lines are always tangent to the electric field at every point in space. The lines always begin at positive charge and end on negative charge, and their density is proportional to the field strength.
  • Under electrostatic conditions, any excess charge, added to a conductor, must reside on the conductor surface.

Electric Field

Lecture Slides are screen-captured images of important points in the lecture. Students can download and print out these lecture slide images to do practice problems as well as take notes while watching the lecture.

  • Intro 0:00
  • Definition of Electric Field 0:11
    • Q1 Produces Electric Field
    • Charges on a Conductor
  • Field of a Point Charge 13:10
    • Charge Point Between Two Fields
    • Electric Field E=kq/r2
    • Direction of the Charge Field
    • Positive Charge, Field is Radially Out
  • Field of a Collection of a Point Charge 19:40
    • Two Charges Q1,Q2
    • Q1 Positive, Electric Field is Radially Out
    • Q2 is Negative, Electric Field is Radially Inward
    • 4 Charges are Equal
  • Parallel Plate Capacitor 25:42
    • Two Plates ,Separated by a Distance
    • Fringe Effect
    • E=Constant Between the Parallel Plate Capacitor
  • Electric Field Lines 35:16
    • Pictorial Representation of Electric Field
    • Electric Lines are Tangent to the Vector
    • Lines Start at Positive Charge, End on Negative Charge
    • Parallel Line Proportional to Charge
    • Lines Never Cross
  • Conductors and Shielding 49:33
    • Static Equilibrium
    • No Net Moment of Charge
    • Electric Field is Perpendicular to the Surface of Conductor
  • Extra Example 1: Plastic Sphere Between Capacitor
  • Extra Example 2: Electron Between Capacitor
  • Extra Example 3: Zero Electric Field
  • Extra Example 4: Dimensional Analysis