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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

Electrical Force
โ€ƒCharged Particles
โ€ƒElectric Field of Spherical shell
โ€ƒElectric Dipole
โ€ƒโ€ƒDipole Electric Field
โ€ƒSource and Reference

Electrical Force

The electrical forces of magnets and electricity are either induced of generated. These forces work very differently from general mechanic forces, e.g. gravitational forces. In fact, the attractive electrostatic force between two charged particles is far stronger than the gravitation forces being exerted between two solid particles.

Charged Particles

The tiny particles prsent in atoms are called protons and electrons. Protons are positively charged, while electrons are negatively charged. Both protons and electrons are the smallest existing charged particles. Protons are very tightly packed within a nucleus of an atom. However, electrons can move freely around the nucleus since these electrons are not perpetually attracted to the nucleus. For example a hydrogen atom. image The gravity of two masses is equal to ๐นgrav=๐บ๐‘š1๐‘š2๐‘Ÿ2๐‘Ÿ
๐‘šproton=1.7ร—10โˆ’27๐‘˜๐‘” ; ๐‘šelectron=9ร—10โˆ’31๐‘˜๐‘”
๐‘Ÿ=5.3ร—10โˆ’11๐‘š ; ๐บ=6.7ร—10โˆ’11๐‘๐‘š2๐‘˜๐‘”2
๐นgrav=6.7ร—10โˆ’11(1.7ร—10โˆ’27)(9ร—10โˆ’31)5.3ร—10โˆ’11โ‰ˆ๐‘‚(10โˆ’46)๐‘
Fhe electricity of two charged particles is ๐นelec=14๐œ‹๐œ€0๐‘„1๐‘„2๐‘Ÿ2๐‘Ÿ
๐‘’=1.6ร—10โˆ’19๐ถ
๐‘Ÿ=5.3ร—10โˆ’11๐‘š ; 14๐œ‹๐œ€0=8.99ร—109๐‘๐‘š2๐ถ2
๐นelec=8.99ร—109(1.6ร—10โˆ’19)25.3ร—10โˆ’11โ‰ˆ๐‘‚(10โˆ’7)๐‘
Therefore with reference to an hydrogen atom, the electricity is much stronger than gravity. The ratio of two forces is ๐นelec๐นgravโ‰ˆ2.27ร—1039

Electric Field of Spherical shell

For a point particle, when the radius ๐‘Ÿ of electric field approaches 0, ๐ธ is undefined at the origin, since ๐‘Ÿ is self-contradictory. Therefore the particle cannot exert a force on itself.
For a uniformly charged spherical shell as below image The charged spherical cell acts like a point particle for ๐‘Ÿโ‰ซ๐‘…, i.e. ๐ธ๐‘ ๐‘โ„Ž๐‘’๐‘Ÿ๐‘’=14๐œ‹๐œ€0๐‘„๐‘Ÿ2๐‘Ÿ; for ๐‘Ÿ>๐‘… i.e. outside the spherical shell Due to spherical symmetry, the field is in the ๐‘Ÿ direction even close up to the sphere. The total electric field ๐ธ๐‘ ๐‘โ„Ž๐‘’๐‘Ÿ๐‘’ can be calculated using the principle of superposition where ๐ธ๐‘ก๐‘œ๐‘ก๐‘Ž๐‘™ is the vector sum of the electric field from all charges.
However, the electric field inside the shell is always equal to zero. i.e. ๐ธ๐‘ ๐‘โ„Ž๐‘’๐‘Ÿ๐‘’=0; for ๐‘Ÿ<๐‘… i.e. inside the spherical shell

Electric Dipole

A electric dipole is a pair of two equal but opposite point charges at a distance apart. image The dipole moment is ๐‘=๐‘ž๐‘ 

Dipole Electric Field

By choicing the midpoint of the dipole as the origin, the dipole electric field can be determined as below image The dipole electric field is equal to ๐ธ0,๐‘ฅ=๐ธ+,๐‘ฅ+๐ธโˆ’,๐‘ฅ=14๐œ‹๐œ€0๐‘ž๐‘Ÿ2+,๐‘ฅ๐‘Ÿ+14๐œ‹๐œ€0โˆ’๐‘ž๐‘Ÿ2โˆ’,๐‘ฅ๐‘Ÿ ๐ธ0,๐‘ฅ=14๐œ‹๐œ€0๐‘ž(๐‘Ÿโˆ’๐‘ /2)2+14๐œ‹๐œ€0โˆ’๐‘ž(๐‘Ÿ+๐‘ /2) along ๐‘ฅ-axis ๐ธ0,๐‘ฅ=14๐œ‹๐œ€0๐‘ž๐‘Ÿ2+๐‘ž๐‘Ÿ๐‘ +๐‘ž๐‘ 2/4โˆ’๐‘ž๐‘Ÿ2+๐‘ž๐‘Ÿ๐‘ โˆ’๐‘ž๐‘ 2/4(๐‘Ÿโˆ’๐‘ /2)2(๐‘Ÿ+๐‘ /2)2 ๐ธ0,๐‘ฅ=14๐œ‹๐œ€02๐‘ž๐‘Ÿ๐‘ (๐‘Ÿโˆ’๐‘ /2)2(๐‘Ÿ+๐‘ /2)2 For electric field far away from the electric dipole, i.e ๐‘Ÿโ‰ซ๐‘ , then the dipole electric field along ๐‘ฅ-axis is ๐‘Ÿโˆ’๐‘ 22โ‰ˆ๐‘Ÿ+๐‘ 22โ‰ˆ๐‘Ÿ2
๐ธ0,๐‘ฅ=14๐œ‹๐œ€02๐‘ž๐‘ ๐‘Ÿ3
๐ธ0,๐‘ฅ=14๐œ‹๐œ€02๐‘ž๐‘ ๐‘Ÿ3,0,0
For the electric field of point particle is approximately equal to ~1/๐‘Ÿ2 and the electric field of dipole is approximately equal to ~1/๐‘Ÿ3.

Source and Reference

https://www.youtube.com/watch?v=v57B_1ZBAho&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=1


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ID: 191100302 Last Updated: 11/3/2019 Revision: 0


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