
ElectricElectric ForcePolarizationInsulator
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โยฑโ๊๏นฆโโ โฏ ๐ธ๐นโ๐ป๐ผ๐ฝ๐พโ๐๐๐๐๐โ๐โโโ๐๐๐๐๐๐๐โค๐ด๐ต๐ถ๐ท๐ธ๐น๐บ๐ป๐ผ๐ฝ๐พ๐ฟ๐๐๐๐๐๐
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โโ ๐ผ๐ฝ๐พ๐ฟ๐๐๐๐๐๐
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โโโโ
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โซโฌโญโฎโฏโฐโฑโฒโณ โฅโฎโฏโฐโฑ โ โฒ โณ โด โ โ สน สบ โต โถ โท
๏น ๏น ๏น ๏น ๏ธน ๏ธบ ๏ธป ๏ธผ ๏ธ ๏ธ ๏ธฟ ๏น ๏ธฝ ๏ธพ ๏น ๏น ๏ธท ๏ธธ โ โ โด โต โ โ โ โก
โโโโโคโฆโฅโงโโโโโโโฒโผโโถโบโปโฒโณ โผโฝโพโฟโโโโโโ
โโ โโโโโโโโโโโโโโโณโฅขโฅฃโฅคโฅฅโฅฆโฅงโฅจโฅฉโฅชโฅซโฅฌโฅญโฅฎโฅฏ
Draft for Information Only
ContentCharge Density
Charge DensityFor a simple 1d charged rod of length L in meter has total charge ๐. Assuming there are 10 point charges in a row then
Electric Field of Charged RodThe electric field of charged rod can be calcuted as followingโ๐ฅ=๐ฟ/10โโ๐=๐/10=(๐/๐ฟ)โ๐ฅ
Electric Field in the Bisecting Plane
The electric field in the bisecting plance can be determined as following
๐=(๐ฅ2+๐ฆ2)1/2 and
For an infinite rod
๐ฟโโ; ๐โโ โ
Where ๐ is defined as charge per unit length.
Therefore, for a finite rod of length ๐ฟ only on the bisecting plane
And for an infinite rod of length ๐ฟโโ, and ๐/๐ฟ is with linear charge density and is not equal to infinite or zero
Procedure for Calculating Electric Field of Distributed Charges
Source and Referencehttps://www.youtube.com/watch?v=pJwg2Bk0BDE&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=5 ยฉsideway ID: 191101802 Last Updated: 11/18/2019 Revision: 0 Latest Updated Links
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