PHYS 212 Chapter 26: 26.4-26.7
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26. 4: the e-fields of rings, disks, planes, and spheres. R is the radius of the ring. Z is the distance from the center of the ring perpendicular to. (cid:4666)(cid:3045) (cid:3047)(cid:4667)= (cid:2869)4 0 (cid:3018) (cid:4666)(cid:3118)+(cid:3019)(cid:3118)(cid:4667)(cid:3119)/(cid:3118)works for both positive and negative z. Divide disk into infinitely many rings with radius ri and charge (cid:1843) On axis electric field of a charged disk is increases out to about |z| = r, then decreases again. Disks factor z^2 out of the square root to get (cid:4666)(cid:3031)(cid:3046)(cid:3038)(cid:4667)= (cid:884)(cid:2868)[(cid:883) (cid:4666)(cid:3031)(cid:3046)(cid:3038)(cid:4667)= (cid:884)(cid:2868)[(cid:883) . Electrodes can often be modeled as infinite planes. Electric field of a plane of charge is found from a disk of infinite radius. Positively charged planes have electric fields pointing away on both sides. So, if z is less than zero, the field must be inverted. 26. 5: the parallel plate capacitor two electrodes equally oppositely charged find between plates (inside) and outside the capacitor.