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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

Charge Density
โ€ƒElectric Field of Charged Rod
โ€ƒโ€ƒElectric Field in the Bisecting Plane
โ€ƒProcedure for Calculating Electric Field of Distributed Charges
โ€ƒSource and Reference

Charge Density

For a simple 1d charged rod of length L in meter has total charge ๐‘„. Assuming there are 10 point charges in a row then image

Electric Field of Charged Rod

The electric field of charged rod can be calcuted as following โˆ†๐‘ฅ=๐ฟ/10โ‡’โˆ†๐‘ž=๐‘„/10=(๐‘„/๐ฟ)โˆ†๐‘ฅ
๐ฟ=โˆ‘โˆ†๐‘ฅ=โˆซ๐‘‘๐‘ฅ
๐‘„=โˆ‘โˆ†๐‘ž=๐‘„๐ฟโˆ‘โˆ†๐‘ฅ=๐‘„๐ฟโˆซ๐‘‘๐‘ฅ

Electric Field in the Bisecting Plane

image The electric field in the bisecting plance can be determined as following ๐‘Ÿ=(๐‘ฅ2+๐‘ฆ2)1/2 and sin ๐œƒ=๐‘ฅ๐‘Ÿ๐‘–
๐ธ๐‘ก๐‘œ๐‘ก=โˆ‘๐‘–โˆ†๐ธ๐‘–=โˆ‘๐‘–โˆ†๐ธ๐‘–,๐‘ฅ๐‘ฅ
โˆ†๐ธ๐‘–,๐‘ฅ=|โˆ†๐ธ๐‘–|cos(๐œƒ) โ€‚=14๐œ‹๐œ€0โˆ†๐‘ž๐‘Ÿ2๐‘–๐‘ฅ๐‘Ÿ๐‘– โ€‚=โˆ†๐‘ž4๐œ‹๐œ€0๐‘ฅ(๐‘ฅ2+๐‘ฆ2๐‘–)3/2
๐ธ๐‘ก๐‘œ๐‘ก=โˆ‘๐‘–โˆ†๐‘ž4๐œ‹๐œ€0๐‘ฅ(๐‘ฅ2+๐‘ฆ2๐‘–)3/2๐‘ฅ โ€‚=14๐œ‹๐œ€0๐‘„๐‘ฅ๐ฟ๐ฟ/2โˆซโˆ’๐ฟ/2๐‘‘๐‘ฆ(๐‘ฅ2+๐‘ฆ2๐‘–)3/2๐‘ฅ โ€‚=14๐œ‹๐œ€0๐‘„๐‘ฅ๐‘ฅ2+(๐ฟ/2)2๐‘ฅ
For an infinite rod ๐ฟโ†’โˆž; ๐‘„โ†’โˆž โ‡’๐‘„๐ฟโ†’๐œ† Where ๐œ† is defined as charge per unit length. ๐ธ๐‘ก๐‘œ๐‘ก=14๐œ‹๐œ€0๐‘„๐‘ฅ๐ฟโˆžโˆซโˆ’โˆž๐‘‘๐‘ฆ(๐‘ฅ2+๐‘ฆ2๐‘–)3/2๐‘ฅ=14๐œ‹๐œ€0๐‘„๐‘ฅ๐ฟ2๐‘ฅ2๐‘ฅ=14๐œ‹๐œ€02๐œ†๐‘ฅ๐‘ฅ Therefore, for a finite rod of length ๐ฟ only on the bisecting plane ๐ธ๐‘ก๐‘œ๐‘ก=14๐œ‹๐œ€0๐‘„๐‘ฅ๐‘ฅ2+(๐ฟ/2)2๐‘ฅ And for an infinite rod of length ๐ฟโ†’โˆž, and ๐‘„/๐ฟ is with linear charge density and is not equal to infinite or zero ๐ธ๐‘ก๐‘œ๐‘ก=14๐œ‹๐œ€02๐œ†๐‘ฅ๐‘ฅ

Procedure for Calculating Electric Field of Distributed Charges

  • Cut the charge distribution into pieces for which the field is known.
  • Write an expression for the electric field due to one piece
    • Choose origin
    • Write an expression for โˆ†๐ธ and its components
  • Add up the contributions of all the pieces
    • Try to integrate symbolically
    • If impossible-integrate numerically
  • Check the results
    • direction
    • Units
    • special cases

Source and Reference

https://www.youtube.com/watch?v=pJwg2Bk0BDE&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=5


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ID: 191101802 Last Updated: 11/18/2019 Revision: 0


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