ECE106 Lecture Notes - Lecture 55: Charge Density, Perfect Conductor, Dielectric

• School: University of Waterloo
• Department: Electrical and Computer Engineering
• Course: ECE106
• Professor: All

Document Summary

Where, qforce is the charge we put in the system, and qinduced is the charge get gets induced. In point form: q e = s. Q p q e = s s q (se + p ) = . Or, this charge is now the force charge. q d = . D = se (6. 52) (6. 53) (6. 54) (6. 55) (6. 56) (6. 57) Effects of material on e is accumulated for in s. We can calculated d without worrying about the material and then calculate as d s. What is sr for a perfect conductor? sr = . E = d = d = 0 s0sr. Parallel plate capacitors with a dielectric slab between two plates. (situation 1) d1 s0 d2 s1 d3 s0. Charge density (on the plates) = q .