Lecture 6 E interactions matter Insulator Conductor Ionized Solution Metal Mobile Electrons Initial...
5
Lecture 6 E interactions matter Insulator Conductor Ionized Solution Metal obile Electrons Initial Drift Velocity: Collision: Δt electron mobility Intermediate: Eventually
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Transcript of Lecture 6 E interactions matter Insulator Conductor Ionized Solution Metal Mobile Electrons Initial...
Lecture 6
E interactions matterInsulator
ConductorIonized SolutionMetal
Mobile Electrons
Initial Drift Velocity:
Collision: Δt
electron mobility
Intermediate: Eventually
A. E at B due to positive surface charge
B. E at B due to all chargesResultant field at B = 0
C. E at B due to all surface charges
At B:
D. EA due to all charges, due to all surface charges
Verify Following Answer:
Both lead to: + =
Example HW problemExample: let Q < 0For a conducting sphere with charge Q on it...
Place positive q1 at P, get F1
Place positive q2 at P get F2
If shows that thenReasoning:
q1 leads to E0q1 p1
Example Polarizability
Find q, α
At midpoint of the pipe: