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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 Potential at a Single Point
โ€ƒPotential inside a Metal
โ€ƒPotential Difference in an Insulator
โ€ƒโ€ƒDielectric Constant
โ€ƒSource and Reference

Electric Potential at a Single Point

Potential of finite systems of charges at a single point ๐ด is the potential relative to infinite separation. ๐‘‰๐ดโ‰ก๐‘‰๐ด-๐‘‰โˆž By convention, the potential at infinity is equal to zero.
The potential of a point charge ๐‘‰๐‘Ÿโ‰ก๐‘‰๐‘Ÿ-๐‘‰โˆž=โˆ’๐‘Ÿโˆซโˆž๐ธโˆ™๐‘‘๐‘™=โˆ’๐‘Ÿโˆซโˆž14๐œ‹๐œ€0๐‘ž๐‘ฅ2๐‘‘๐‘ฅ=14๐œ‹๐œ€0๐‘ž๐‘ฅ๐‘Ÿ๏ฝœโˆž=14๐œ‹๐œ€0๐‘ž๐‘Ÿ (volts) While the electric potential energy of two particles is ๐‘ˆele=14๐œ‹๐œ€0๐‘ž1๐‘ž2๐‘Ÿ12๐‘‘๐‘ฅ (joules) The relationship of potential difference and electric field can be expressed as ๐ธ=โˆ’๐‘‘๐‘‰๐‘‘๐‘ฅ=โˆ’โˆ‡๐‘‰; โˆ†๐‘‰=โˆ’๐‘“โˆซ๐‘–๐ธโˆ™๐‘‘๐‘™ Therefore, knowing ๐ธ at only one point does not tell ๐‘‰ at that point. And knowing ๐‘‰ at that point does not tell ๐ธ.

Potential inside a Metal

For a metal in equilibrium, the eletric field inside is ๐ธ=0, and the potential is constant. image when a metal is in equilibrium, electron sea inside the metal is in equilibrium also, that is the velocity ๐‘ฃnet=0. When a metal is out of equilibrium, /for examples, applied current, ie hooked up in a circuit. or immediately after aplying a field i.e. electrons move to screen it.

Potential Difference in an Insulator

image The electric field in capacitor filled with insulator is equal to ๐ธnet=๐ธplates+๐ธdipoles
where ๐ธplates=const in capacitor; ๐ธdipoles=๐‘“(๐‘ฅ,๐‘ฆ,๐‘ง)
โˆ†๐‘‰=โˆ’๐‘โˆซ๐‘Ž๐ธโˆ™๐‘‘๐‘ฅ
The electric field in insulator composes of two components. Field from the charges on plates and field from the induced dipoles. The average field from induced dipoles is opposite to the field from the plates. When a charged particle moving from ๐ด to ๐ต, ๐ธdipoles is sometimes parallel to ๐‘‘๐‘ฅ and sometimes is antiparallel to ๐‘‘๐‘ฅ.
Considering the path due to polarized insulator outside the insulator. ๐ธโˆ™๐‘‘๐‘™โ‰ฅ0
โˆ†๐‘‰=๐‘‰๐ตโˆ’๐‘‰๐ด=โˆ’๐‘โˆซ๐‘Ž๐ธโˆ™๐‘‘๐‘™

Dielectric Constant

Dielectric medium has a constant ๐พ. Inside the insulating medium ๐ธnet=๐ธapplied๐พ. The bigger ๐พ is the more it dampens the electric field. In other words, a bigger ๐พ means greater polarization. Dielectric constant for various insulators: vacuum1 by definition air1.0006 typical plastic5 NaCl6.1 water80 strontium titanate310

Source and Reference

https://www.youtube.com/watch?v=FZIGV-AppFo&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=10


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ID: 191200702 Last Updated: 12/7/2019 Revision: 0


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