Title: CLASS 6 January 31 Gauss law
1CLASS 6 (January 31) Gauss law Law of
conservation of charge. Maxwells equations in
integral form.
2Faradays and Amperes Laws in integral form
Faradays Law
The electromotive force around a closed path C
Is equal to the negative of the time rate of
the magnetic flux enclosed by that path.
Amperes Law
The magnetomotive force around a closed path C
is equal to the algebraic sum of the current due
to flow of charges and the displacement current
bounded by that path C.
Whirl or Eddy
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4Gauss laws
For electric field
For magnetic field
There are origins and/or endpoints of D field
lines inside the volume surrounded by S.
5Maxwells equations in integral form
Faradays Law
Amperes Law
Gauss law for electrical field
Gauss law for magnetic field
In vacuum (Free space)
6Gausss Law for the magnetic field is not
independent of Faradays Law
Gausss Law for the electric field is not
independent of Amperes Law
(Conservation of charge)
7Maxwells equations for static fields
General form Always true!
True only for statics (False in general)
for all C
(No whirl (eddy) in static electric fields)
Conservation of charge
Coulombs Law
Lorentz force
Electric and Magnetic fields are INDEPENDENT!
8Application of
enable us to find the static electric field
for certain charge distributions IF THE
resulting E field possess SYMMETRY, to be able to
replace the integrals by expressions of E.
Electric field due to an infinitely long line
charge
Cylindrical symmetry Cylindrical coordinate system
9Electric field due to a spherical volume charge
uniform charge density In region
Spherical symmetry Spherical coordinates
10enable us to find the static magnetic field
Application of
for certain current distributions IF THE
resulting H field possess SYMMETRY, to be able to
replace the integrals by expressions of H.
Magnetic field due to a cylindrical wire of
current
Axis along z axis
Wire radius a
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