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Electric fields.
Electrostatics.  ,[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object]
[object Object],[object Object]
[object Object],[object Object]
Q 1 Q 2 r Notice must be paid to the charges of the bodies, the charges may not be the same magnitude  or  have the same polarity (+ve or –ve)
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object]
Electric field strength  E ,[object Object],[object Object]
[object Object],[object Object],[object Object],1 r Point charge (+Q) E Test charge (+Q’)
[object Object],[object Object],2 Radial field
Radial fields  (draw in the radial field lines) Q+ Q-
Electric field strength in a uniform field. ,[object Object],[object Object],Separation  = d P.d.  = V A B
[object Object],[object Object],[object Object],Uniform field
Questions. ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Electric potential ,[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],Where:  V = Electric potential. (V)  0  = Permittivity of free space (F/m) r = separation (m) Q = Charge (C)
Field lines and Equipotential ,[object Object],[object Object],[object Object],+ - +Q -Q
Motion of charged particles in an electric field. ,[object Object],[object Object]
[object Object],[object Object]
[object Object],[object Object],and Where q is the minor or moving charge (Q 2)
[object Object],[object Object]
[object Object],Beam of +ve Particles + -
[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object]
Can be used to describe the field – direction is the direction of the force on a positive charge  Can be used to describe the field – direction is the direction of the force on a mass  Field lines  Infinite, decreases with distance but theoretically never reaches zero.   Infinite, decreases with distance but theoretically never reaches zero.  Range of field   Contact not needed, acts at distance  Contact not needed, acts at distance  For the force to act  Electrical  Gravitational
Can be used to describe work done in moving charges: (inverse law)  Can be used to describe work done in moving masses: (inverse law)  Potential  Given by Coulomb’s law:  Given by Newton’s law of universal gravitation:  Force between 2 objects.  Force on a unit charge:  Force on a unit mass:  Field strength
Kinetic energy  Field strength is (-ve of) potential gradient.   Field strength is (-ve of) potential gradient.   Relationship between potential and field strength.  Electrical PE:  GPE:  Potential energy
Differences Comparative sizes  Shielding Effect  Produced by and acts on charges  Produced by and acts on masses  Origin

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Electric Fields

  • 2.
  • 3.
  • 4.
  • 5.
  • 6. Q 1 Q 2 r Notice must be paid to the charges of the bodies, the charges may not be the same magnitude or have the same polarity (+ve or –ve)
  • 7.
  • 8.
  • 9.
  • 10.
  • 11.
  • 12.
  • 13. Radial fields (draw in the radial field lines) Q+ Q-
  • 14.
  • 15.
  • 16.
  • 17.
  • 18.
  • 19.
  • 20.
  • 21.
  • 22.
  • 23.
  • 24.
  • 25.
  • 26.
  • 27.
  • 28.
  • 29.
  • 30. Can be used to describe the field – direction is the direction of the force on a positive charge Can be used to describe the field – direction is the direction of the force on a mass Field lines Infinite, decreases with distance but theoretically never reaches zero. Infinite, decreases with distance but theoretically never reaches zero. Range of field Contact not needed, acts at distance Contact not needed, acts at distance For the force to act Electrical Gravitational
  • 31. Can be used to describe work done in moving charges: (inverse law) Can be used to describe work done in moving masses: (inverse law) Potential Given by Coulomb’s law: Given by Newton’s law of universal gravitation: Force between 2 objects. Force on a unit charge: Force on a unit mass: Field strength
  • 32. Kinetic energy Field strength is (-ve of) potential gradient. Field strength is (-ve of) potential gradient. Relationship between potential and field strength. Electrical PE: GPE: Potential energy
  • 33. Differences Comparative sizes Shielding Effect Produced by and acts on charges Produced by and acts on masses Origin