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3. Electric Flux Electric flux is the product of the magnitude of the electric field and the surface area, A, perpendicular to the field
FE = EA
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4. The electric flux is proportional to the number of electric field lines penetrating some surface
The field lines may make some angle ? with the perpendicular to the surface
Then FE = EA cos ?
The flux is a maximum
when the surface is
perpendicular to the field
The flux is a minimum
(zero) when the surface is (parallel) to the field
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5. Electric Flux If the field varies over the surface, F = EA cos ? is valid for only a small element of the area
In the more general case, look at a small area element
In general, this becomes 5 Norah Ali Al-moneef King Saud university
6. Electric Flux The surface integral means the integral must be evaluated over the surface in question
The value of the flux depends both on the field pattern and on the surface
SI units: N.m2/C 6 Norah Ali Al-moneef King Saud university
7. Electric Flux, Closed Surface For a closed surface, by convention, the A vectors are perpendicular to the surface at each point and point outward
(1) ? < 90o, F > 0
(2) ? = 90o, F = 0
(3) 180o > ? > 90o, F < 0
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10. Gaussian surfaces of various shapes can surround the charge (only S1 is spherical)
The electric flux is proportional to the number of electric field lines penetrating these surfaces, and this number is the same
Thus the net flux through any closed surface surrounding a point charge q is given by q/eo and is independent of the shape of the surface 10 Norah Ali Al-moneef King Saud university
11. Gauss Law If the charge is outside the closed surface of an arbitrary shape, then any field line entering the surface leaves at another point
Thus the electric flux through a closed surface that surrounds no charge is zero 11 Norah Ali Al-moneef King Saud university
12. Gauss Law Since the electric field due to many charges is the vector sum of the electric fields produced by the individual charges, the flux through any closed surface can be expressed as
Although Gausss law can, in theory, be solved to find for any charge configuration, in practice it is limited to symmetric situations
One should choose a Gaussian surface over which the surface integral can be simplified and the electric field determined 12 Norah Ali Al-moneef King Saud university
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16.
For r > a
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18. Field Due to a Spherically Symmetric Charge Distribution Inside the sphere, E varies linearly with r (E ? 0 as r ? 0)
The field outside the sphere is equivalent to that of a point charge located at the center of the sphere 18 Norah Ali Al-moneef King Saud university
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29. Charge Resides on the Surface Choose a Gaussian surface inside but close to the actual surface
The electric field inside is zero
There is no net flux through the gaussian surface
Because the gaussian surface can be as close to the actual surface as desired, there can be no charge inside the surface 29 Norah Ali Al-moneef King Saud university
30. E-Fields Magnitude and Direction Choose a cylinder as the Gaussian surface
The field must be perpendicular to the surface
If there were a parallel component to E, charges would experience a force and accelerate along the surface and it would not be in equilibrium 30 Norah Ali Al-moneef King Saud university
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41. 6/11/2012 41 Norah Ali Al-moneef king saud university
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