For spherical symmetrical charge distribution, variation of electric potential with distance from centre is given in diagram. CAREER ENDEAVOUR r = Ro - for rs R, and V = - for r 2 R. 4x ɛ, r Given that : V = 47 E, R. Then which options(s) are correct : (a) Total charge within 2R, isq (b) ỹ.Ē = 0 everywhere (c) At r= R, electric field is discontinuous (d) There will be no charge anywhere except at r = R, %3D
For spherical symmetrical charge distribution, variation of electric potential with distance from centre is given in diagram. CAREER ENDEAVOUR r = Ro - for rs R, and V = - for r 2 R. 4x ɛ, r Given that : V = 47 E, R. Then which options(s) are correct : (a) Total charge within 2R, isq (b) ỹ.Ē = 0 everywhere (c) At r= R, electric field is discontinuous (d) There will be no charge anywhere except at r = R, %3D
College Physics
11th Edition
ISBN:9781305952300
Author:Raymond A. Serway, Chris Vuille
Publisher:Raymond A. Serway, Chris Vuille
Chapter1: Units, Trigonometry. And Vectors
Section: Chapter Questions
Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...
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![For spherical symmetrical charge distribution, variation of electric potential with distance from centre is given
in diagram.
CAREER ENDEAVOUR
r = Ro
- for r s R, and V =
for r2 R,
47 E, r
Given that : V = -
Απε, R
Then which options(s) are correct :
(a) Total charge within 2R, is q
(b) v.Ē = 0 everywhere
(c) At r= R, electric field is discontinuous
(d) There will be no charge anywhere except at r = R,](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Fbdecd06b-2880-48e4-b278-fd1d2c383e97%2F5bfe074c-6d6a-47fb-b3cc-a8deb30283ce%2F6w3bnwq_processed.png&w=3840&q=75)
Transcribed Image Text:For spherical symmetrical charge distribution, variation of electric potential with distance from centre is given
in diagram.
CAREER ENDEAVOUR
r = Ro
- for r s R, and V =
for r2 R,
47 E, r
Given that : V = -
Απε, R
Then which options(s) are correct :
(a) Total charge within 2R, is q
(b) v.Ē = 0 everywhere
(c) At r= R, electric field is discontinuous
(d) There will be no charge anywhere except at r = R,
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