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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
โ€ƒPotential Difference
โ€ƒโ€ƒNon-uniform Electric Field
โ€ƒPath of Potential Difference
โ€ƒSource and Reference

Electric Potential

For two fixed opposite charged plates, the electric field due to plates is as following image If a charged particle is placed in the capacitor, an induced force will drive the charged particle to move. image The eletric pontential energy acting on the charge particle ๐‘ž๐‘– is ๐‘ˆele=โ€‰โˆ‘๐‘—๐‘ˆ๐‘–๐‘—=โ€‰โˆ‘๐‘—14๐œ‹๐œ€0๐‘ž๐‘–๐‘ž๐‘—๐‘Ÿ๐‘–๐‘— The electric potential is defined as the potential or the ability to have potential energy if a test charge enters the system. In other words, the electric potential can be expressed as ๐‘‰โ‰ก๐‘ˆele๐‘ž=JoulesCoulomb=[Volts]

Potential Difference

When the charge particle is moved from ๐‘Ž to ๐‘ as following image the change in potential energy of the system is โˆ†๐‘ˆ=โˆ’๐‘Šinternal=โˆ’โˆซ๐‘ž๐ธโˆ™๐‘‘๐‘Ÿ=โˆ’๐‘žโˆซ๐ธ๐‘ฅ๐‘‘๐‘ฅ
โ‡’โˆ†๐‘ˆ=โˆ’๐‘ž๐ธโˆ†๐‘ฅ
In which the systems tends to lower their potential energy by moving the charge particle from a higher potential energy position to a lower potential energy position. In other words, the potential difference drive the charge particle to move from one position to another. โˆ†๐‘ˆ=โˆ’๐‘ž๐ธโˆ†๐‘ฅโ‰ก๐‘žโˆ†๐‘‰โ‡’โˆ†๐‘‰=โˆ†๐‘ˆ๐‘ž=โˆ’๐ธโˆ†๐‘ฅ
๐‘‰=[Volt]=JouleCoulomb
โˆ†๐‘ˆ/๐‘ž=โˆ’๐ธโˆ†๐‘ฅโ‰กโˆ†๐‘‰โ‡’๐ธ=โˆ’โˆ†๐‘ˆ/๐‘žโˆ†๐‘ฅ=โˆ’โˆ†๐‘‰/โˆ†๐‘ฅ
|๐ธ|=JouleCoulomb-meter=NewtonCoulomb=VoltMeter
An electron-Volt, ๐‘’๐‘‰ is the energy required to move a charge particle, ๐‘ž=1๐‘’=1.6ร—10โˆ’19๐ถ through 1๐‘‰. That is 1.6ร—10โˆ’19๐ฝ=1๐‘’๐‘‰

Non-uniform Electric Field

For a uniform electric field, i.e. ๐ธโˆฅ๐‘ฅ, โˆ†๐‘‰=โˆ’๐ธโˆ†๐‘ฅ. And for a uniform electric field pointing in any direction. โˆ†๐‘‰=โˆ’(๐ธ๐‘ฅโˆ†๐‘ฅ+๐ธ๐‘ฆโˆ†๐‘ฆ+๐ธ๐‘งโˆ†๐‘ง)โ‰กโˆ’๐ธโˆ™๐‘‘๐‘Ÿ If the electric field ๐ธ is not uniform, but varies in space. The potential difference can be determined by a line integral like stepping along a path. At each step, use component of electric field parallel to the step direction. โˆ†๐‘‰=โˆ’๐‘“โˆ‘๐‘–๐ธโˆ™๐‘‘๐‘™=โˆ’๐‘“โˆซ๐‘–๐ธโˆ™๐‘‘๐‘™ The electric field can therefore be expressed as ๐ธ=โˆ’๐‘‘๐‘‰๐‘‘๐‘ฅ=โˆ’โˆ‚โˆ‚๐‘ฅ๐‘‰๐‘ฅ+โˆ‚โˆ‚๐‘ฆ๐‘‰๐‘ฆ+โˆ‚โˆ‚๐‘ง๐‘‰๐‘ง=โˆ’โˆ‡๐‘‰

Path of Potential Difference

image Since electricity is a conservative force the potential difference โˆ†๐‘‰ is independent of the path taken. For example, in a simple uniform electric field โˆ†๐‘‰=โˆ’๐‘“โˆ‘๐‘–๐ธโˆ™๐‘‘๐‘™=โˆ’๐‘“โˆ‘๐‘–๐ธ๐‘ฅ๐‘‘๐‘™๐‘ฅ+๐‘“โˆ‘๐‘–๐ธ๐‘ฆ๐‘‘๐‘™๐‘ฆ+๐‘“โˆ‘๐‘–๐ธ๐‘ง๐‘‘๐‘™๐‘ง=๐‘‰๐‘“โˆ’๐‘‰๐‘–

Source and Reference

https://www.youtube.com/watch?v=8HSwBeHZoao&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=9


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ID: 191200302 Last Updated: 12/3/2019 Revision: 0


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