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IB 5.2 Electric Field

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IB 5.2 Electric Field & Potential Electric Field Just like mass create gravitational fields, charges create electric fields With gravity the field strength is measure ... – PowerPoint PPT presentation

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Title: IB 5.2 Electric Field


1
IB 5.2 Electric Field Potential
2
Electric Field
  • Just like mass create gravitational fields,
    charges create electric fields
  • With gravity the field strength is measure as
    Newton per kilogram
  • What do you think Electric fields are measured
    in?
  • Newton's per Coulomb

3
Measuring the Electric Field
  • If the unit is Newton's per Coulomb, what is the
    equation?
  • E F / qo
  • Simple enough, right.
  • E Electric Field
  • F Force
  • qo charge in the field

4
Summing electric Fields
  • Alternative Equation
  • It is the surrounding charges that creates an
    electric field at a given point in space.
  • Look at Example 8

5
Picturing the Electric Field
Click on the picture to open an applet
6
Electric Field Rules
  • Fields start at positive and end at negative, or
    start and end at infinity.
  • This is by convention. The field is said to
    predict the movement of a positive charge.
  • The density of lines should represent the
    strength of the field.
  • A positive charge will have a velocity tangent to
    a field line.
  • Field lines do not actually exist since the are
    an infinite number of paths a test charge can
    take.

7
Parallel Plate Capacitors
  • Used to store charge.
  • The most common type is a parallel plate
    capacitor.
  • Charge is spread uniformly, not really,
    throughout the plate
  • The electric field between two parallel plates is
    100 N C-1.
  • What acceleration would a 2.0 mC charge with a
    mass of 10-3 kg experience if placed in the field?

8
Electric Potential
  • Consider a positive charge Q and a test charge q.
  • Work must be done to move q closer to Q since
    like charges repel.
  • V Voltage (Potential measured in Volts)

9
Work and Route
  • Regardless of the path taken to move the charge
    the work is always the same.
  • Electric Potential Energy is U qV
  • Potential Difference is DU

10
Electric Fields Inside Conductors
  • Excess electric charge moves to the surface of a
    conductor
  • At equilibrium the electric field inside a
    conductor is zero
  • This comes from the fact that free electrons will
    always be on the outside of the conductor.
  • So the electric field lines dont penetrate the
    conductor
  • The electric field outside a conductor is
    perpendicular to the surface

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