Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.
-
Upload
sheila-bradford -
Category
Documents
-
view
212 -
download
0
Transcript of Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.
![Page 1: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/1.jpg)
Coulomb’s Law
Section 36
![Page 2: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/2.jpg)
Electrostatic field
Poisson’s equation
![Page 3: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/3.jpg)
Vacuum: r = 0Laplace’s equation
![Page 4: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/4.jpg)
Theorem: Scalar potential cannot have an extremum in vacuum.
Proof: Suppose f has an extreme value somewhere
Then
AND
0 at that point
All have the same sign
But that violates
![Page 5: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/5.jpg)
Point charge. Field is spherically symmetricNo f or q dependence.E is oriented along a radius vector from the point charge.E = E(R) is a function only of the distance R from the charge.
Inversely proportional to the square of the distance from the charge.
Coulomb’s law
![Page 6: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/6.jpg)
Potential of a point charge
Since
![Page 7: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/7.jpg)
System of charges
Superposition principle:E-field at a field point is the vector sum of the fields form all charges
Potential at field point is sum of potentials from all charges
![Page 8: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/8.jpg)
Continuous charge distribution
r = charge density
Field point
![Page 9: Coulomb’s Law Section 36. Electrostatic field Poisson’s equation.](https://reader035.fdocuments.net/reader035/viewer/2022072010/56649dd15503460f94ac65ff/html5/thumbnails/9.jpg)
Point charge
Poisson’s equation