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Lecture 20 Today Conductors Resistance Dielectrics

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Presentation on theme: "Lecture 20 Today Conductors Resistance Dielectrics"— Presentation transcript:

1 16.360 Lecture 20 Today Conductors Resistance Dielectrics
Electric boundary conditions Capacitance Electrostatic potential energy Image method

2 16.360 Lecture 20 Conductors Electron drift velocity
Hole drift velocity Conducting current Point form of Ohm’s law

3 Lecture 20 Resistance General form

4 Lecture 20 Joule’s law General form

5 Lecture 20 Dielectrics Electrical field induced polarization

6 16.360 Lecture 20 Dielectrics P: electric polarization field
For homogeneous material: Electric susceptibility Relative permittivity: Dielectric breakdown

7 16.360 Lecture 20 Electric boundary condition
the tangential component is continuous across the boundary of two media.

8 16.360 Lecture 20 Electric boundary condition
the normal component of D changes, the amount of change is equal to the surface Charge density.

9 Lecture 20 Dielectric-Conductor boundary

10 Lecture 20 Conductor-Conductor boundary

11 Lecture 20 Capacitance

12 16.360 Lecture 20 Electrostatic Potential Energy Image Method
Any given charge above an infinite, perfect conducting plane is electrically equivalent to the combination of the give charge and it’s image with conducting plane removed.


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