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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

Conservation of Charge
โ€ƒCharges of an Atom
โ€ƒPolarization of Atoms
โ€ƒForce of a Point Charge on an Atom
โ€ƒSource and Reference

Conservation of Charge

The net charge of a system and its surroundings cannot change. But charge can move from the systtem to surroundings or from surroundings to the system. However, charges can be created or destroyed in (+,โˆ’) pairs. For examples, electron-positron annihilation.

Charges of an Atom

image Charge of electron cloud equals that of nucleus implies neutral atom. If the electron cloud is centered on the nucleus implies electric field produced by electrons exactly cancels the field produced by nucleus.

Polarization of Atoms

image By placing a point charge close to an atom, point charge exerts electric field on the atom. Atom becomes polarized by electric field. An induced dipole can be represented as follow image A more easily polarized atom has a larger induced dipole moment, which produces a larger electric field. And a more easily polarized atom experiences a greater attraction to a point charge. Polarization is defined as ๐‘=๐›ผ๐ธ where ๐›ผ is polarizability of a material
|๐‘|=๐‘=๐‘ž๐‘ 
In an induced dipole, the distance between the charges is proportional to the strength of the applied field.

Force of a Point Charge on an Atom

image A point charge first creates electric field ๐ธ0 at atom, ๐ธ0=14๐œ‹๐œ€0๐‘ž0๐‘Ÿ2๐‘Ÿ Then the electric field ๐ธ0 polarizes atom image and the polarization is ๐‘=๐›ผ๐ธ0=14๐œ‹๐œ€0๐›ผ๐‘ž0๐‘Ÿ2๐‘Ÿ The induced dipole in turn creates field ๐ธ๐‘Ž at point image The electric field is ๐ธ๐‘Ž=14๐œ‹๐œ€02๐‘๐‘Ÿ3=14๐œ‹๐œ€02๐›ผ๐ธ0๐‘Ÿ3=14๐œ‹๐œ€02๐›ผ๐‘Ÿ314๐œ‹๐œ€0๐‘ž0๐‘Ÿ2๐‘Ÿ=14๐œ‹๐œ€022๐›ผ๐‘ž0๐‘Ÿ5๐‘Ÿ ~1/๐‘Ÿ5 The electric field ๐ธ๐‘Ž due to the induced dipole exerts force on point charge image The force is ๐น0=๐‘ž0๐ธ๐‘Ž=14๐œ‹๐œ€022๐›ผ๐‘ž20๐‘Ÿ5๐‘Ÿ By reciprocity, the force ๐น๐‘Ž that the point charge exerts on atom will be equal and opposite to the force ๐น0 image The force is ๐น๐‘Ž=โˆ’๐น0=โˆ’๐‘ž0๐ธ๐‘Ž=14๐œ‹๐œ€022๐›ผ๐‘ž20๐‘Ÿ5๐‘Ÿ Neutral atoms are attracted by charges with interaction strength ~1/๐‘Ÿ5

Source and Reference

https://www.youtube.com/watch?v=rb_ybczb7Ig&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=3


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ID: 191101002 Last Updated: 11/10/2019 Revision: 0


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