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`-=[]โŸจโŸฉ\;',./~!@#$%^&*()_+{}|:"<>? ๐‘Ž๐‘๐‘๐‘‘๐‘’๐‘“๐‘”โ„Ž๐‘–๐‘—๐‘˜๐‘™๐‘š๐‘›๐‘œ๐‘๐‘ž๐‘Ÿ๐‘ ๐‘ก๐‘ข๐‘ฃ๐‘ค๐‘ฅ๐‘ฆ๐‘ง ร…โ€‰โˆ’โ€‚ร—โ€ƒโ‹…โˆ“ยฑโˆ˜๊žŠ๏นฆโˆ—โˆ™ โ„ฏ ๐”ธ๐”นโ„‚๐”ป๐”ผ๐”ฝ๐”พโ„๐•€๐•๐•‚๐•ƒ๐•„โ„•๐•†โ„™โ„šโ„๐•Š๐•‹๐•Œ๐•๐•Ž๐•๐•โ„ค๐ด๐ต๐ถ๐ท๐ธ๐น๐บ๐ป๐ผ๐ฝ๐พ๐ฟ๐‘€๐‘๐‘‚๐‘ƒ๐‘„๐‘…๐‘†๐‘‡๐‘ˆ๐‘‰๐‘Š๐‘‹๐‘Œ๐‘ โˆผโˆฝโˆพโ‰โ‰‚โ‰ƒโ‰„โ‰…โ‰†โ‰‡โ‰ˆโ‰‰โ‰Œโ‰โ‰ โ‰ก โ‰คโ‰ฅโ‰ฆโ‰งโ‰จโ‰ฉโ‰ชโ‰ซ โˆˆโˆ‰โˆŠโˆ‹โˆŒโˆ โŠ‚โŠƒโŠ„โŠ…โІโЇ ๐›ผ๐›ฝ๐›พ๐›ฟ๐œ€๐œ๐œ‚๐œƒ๐œ„๐œ…๐œ†๐œ‡๐œˆ๐œ‰๐œŠ๐œ‹๐œŒ๐œŽ๐œ๐œ๐œ‘๐œ’๐œ“๐œ” โˆ€โˆ‚โˆƒโˆ…โฆฐโˆ†โˆ‡โˆŽโˆžโˆโˆดโˆต โˆโˆโˆ‘โ‹€โ‹โ‹‚โ‹ƒ โˆงโˆจโˆฉโˆช โˆซโˆฌโˆญโˆฎโˆฏโˆฐโˆฑโˆฒโˆณ โˆฅโ‹ฎโ‹ฏโ‹ฐโ‹ฑ โ€– โ€ฒ โ€ณ โ€ด โ„ โ— สน สบ โ€ต โ€ถ โ€ท ๏น ๏น‚ ๏นƒ ๏น„ ๏ธน ๏ธบ ๏ธป ๏ธผ ๏ธ— ๏ธ˜ ๏ธฟ ๏น€ ๏ธฝ ๏ธพ ๏น‡ ๏นˆ ๏ธท ๏ธธ โœ   โ   โŽด  โŽต  โž   โŸ   โ    โก โ†โ†‘โ†’โ†“โ†คโ†ฆโ†ฅโ†งโ†”โ†•โ†–โ†—โ†˜โ†™โ–ฒโ–ผโ—€โ–ถโ†บโ†ปโŸฒโŸณ โ†ผโ†ฝโ†พโ†ฟโ‡€โ‡โ‡‚โ‡ƒโ‡„โ‡…โ‡†โ‡‡ โ‡โ‡‘โ‡’โ‡“โ‡”โ‡Œโ‡โ‡โ‡•โ‡–โ‡—โ‡˜โ‡™โ‡™โ‡ณโฅขโฅฃโฅคโฅฅโฅฆโฅงโฅจโฅฉโฅชโฅซโฅฌโฅญโฅฎโฅฏ
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Content

Electric flux
โ€ƒGauss's Law
โ€ƒGauss's Law for Point Charge
โ€ƒGauss's Law for Plane
โ€ƒGauss's Law for Magnetism
โ€ƒSource and Reference

Electric flux

image The source of electric field is charge. When there is electric field flowing radially, there is a source inside. Electric flux is defined as the effect of electric field over the area of the surface projected in a plane perpendicular to the field, that is (๐ธโ‹…๐‘›)๐‘‘๐ด. In order words, the electric flux of a surface which is parallel to the electric field, is equal to zero. image The electric flux over a surface is โˆ‘(๐ธโ‹…๐‘›)๐‘‘๐ด.

Gauss's Law

The total electric flux out of a closed surface is equal to the charge enclosed divided by the permittivity. โˆฎ ๐ธโ‹…๐‘›๐‘‘๐ด=1๐œ€0โˆ‘๐‘žinside

Gauss's Law for Point Charge

image For a point charge, the electric flus of concentric spherical surface shell of radius ๐‘Ÿ is โˆฎ ๐ธโ‹…๐‘›๐‘‘๐ด=14๐œ‹๐œ€0๐‘ž๐‘Ÿ2(4๐œ‹๐‘Ÿ2)=๐‘ž๐œ€0. The electric flux does not depend on the radius of the concentric spherical surface shell because field ๐ธโˆ1๐‘Ÿ2 and surface area ๐ดโˆ๐‘Ÿ2. image In any segment, the contribution from any shell is the same. image Since electric flux through any outer shell surface is always the same. The electric flux of any closed surface formed by any outer shell surfaces is always the same. image Similarly, by limit the segment to infinite small segment, the enclosed surface can be refined to surround the charge with any smooth shape by following different shperes in different places with the same electric flux.

Gauss's Law for Plane

image For an infinite plane with surface charge density, ๐œŽ=[๐‘„/๐ด]. Due to geometry of plane, the electric filed is perpendicular to plane and has same magnitude everywhere. image Define a Gaussian box, ๐ธ is constant and perpendicular to the two plane surfaces of the Gaussian box. โˆฎ ๐ธโ‹…๐‘›๐‘‘๐ด=1๐œ€0๐‘žinside=[๐‘„/๐ด]๐ด ๐ธ(2๐ด)=1๐œ€0๐œŽ๐ด ๐ธ=๐œŽ๐ด2๐œ€0

Gauss's Law for Magnetism

So far, no experiment has found a magnetic charge, i.e. a magnetic monopole. Therefore ๐‘žmagnet=0 and Gauss's law for magnetism is โˆฎ ๐ตโ‹…๐‘›๐‘‘๐ด=0

Source and Reference

https://www.youtube.com/watch?v=ULWIQvF-muo&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=22

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ID: 200102202 Last Updated: 1/22/2020 Revision: 0


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