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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

Magnetic Field of a Straight Wire
โ€ƒMagnetic Field along Axis of Circular Loop of Wire
โ€ƒPermanent Magnet
โ€ƒSource and Reference

Magnetic Field of a Straight Wire

image The magnetic field of a long straight wire is ๐‘Ÿ=<๐‘ฅ,0,โˆ’๐‘ง>โ‡’{|๐‘Ÿ|2=๐‘ฅ2+๐‘ง2๐‘Ÿ=๐‘Ÿ|๐‘Ÿ|=<๐‘ฅ,0,โˆ’๐‘ง>๐‘ฅ2+๐‘ง2
โˆ†๐‘™=โˆ†๐‘ง=<0,0,โˆ†๐‘ง>โ‡’โˆ†๐‘งร—๐‘Ÿ=1|๐‘Ÿ|(โˆ†๐‘งร—๐‘Ÿ)=1|๐‘Ÿ|๐‘ฅโ€‚๐‘ฆโ€‚๐‘ง0โ€‚0โ€‚โˆ†๐‘ง๐‘ฅโ€‚0โ€‚โˆ’๐‘ง=0๐‘ฅ+๐‘ฅโˆ†๐‘ง๐‘ฆ+0๐‘ง|๐‘Ÿ|=๐‘ฅโˆ†๐‘ง๐‘ฅ2+๐‘ง2๐‘ฆ
โˆ†๐ต=๐œ‡04๐œ‹๐ผโˆ†๐‘™ร—๐‘Ÿ|๐‘Ÿ|2=๐œ‡04๐œ‹๐ผโˆ†๐‘งร—๐‘Ÿ๐‘ฅ2+๐‘ง2=๐œ‡0๐ผ4๐œ‹๐‘ฆ๐‘ฅโˆ†๐‘ง(๐‘ฅ2+๐‘ง2)3/2
๐ต=โˆซโˆ†๐ต=๐œ‡0๐ผ4๐œ‹๐‘ฆ๐ฟ/2โˆซโˆ’๐ฟ/2๐‘ฅ(๐‘ฅ2+๐‘ง2)3/2๐‘‘๐‘ง
|๐ต๐‘ฆ|=๐œ‡04๐œ‹๐ผ๐ฟ๐‘ฅ๐‘ฅ2+(๐ฟ/2)2
By symmetry, the magnetic field of a long straight wire can be expressed in cylindrical coordinates with ๐‘ฅ=๐‘… as following ๐ต=๐œ‡04๐œ‹๐ผ๐ฟ๐‘…๐‘…2+(๐ฟ/2)2๐œƒ When the length of wire tend to infinite long the measured point is very close to the wire, ๐‘…โ‰ช๐ฟ ๐‘…โ‰ช๐ฟโ‡’๐‘…2+(๐ฟ/2)2โ‰ˆ๐ฟ/2
๐ต=๐œ‡04๐œ‹๐ผ๐ฟ๐‘…(๐ฟ/2)๐œƒ=๐œ‡04๐œ‹2๐ผ๐‘…๐œƒ

Magnetic Field along Axis of Circular Loop of Wire

image By symmetry, the magnetic field is reduced to ๐‘ง-component. and the magnetic field of one element is โˆ†๐ต๐‘ง=๐œ‡04๐œ‹๐ผ๐‘…2โˆ†๐œƒ(๐‘…2+๐‘ง2)3/2
๐ต๐‘ง=โˆซโˆ†๐ต๐‘ง=2๐œ‹โˆซ0๐œ‡04๐œ‹๐ผ๐‘…2โˆ†๐œƒ(๐‘…2+๐‘ง2)3/2=๐œ‡04๐œ‹๐ผ๐‘…22๐œ‹(๐‘…2+๐‘ง2)3/2=๐‘‡โˆ™๐‘š๐ด(๐‘š2โˆ™๐ด)(๐‘š2)3/2=[๐‘‡]
For ๐‘ง far from the loop, ๐‘งโ‰ซ๐‘… (๐‘ง2+๐‘…2)3/2=(๐‘ง2)3/2=๐‘ง3 Therefore the magnetic field along axis far from loop ๐ตaxisโ‰ˆ๐œ‡04๐œ‹2๐œ‹๐‘…2๐ผ๐‘ง3
Let Magnetic dipole moment ๐œ‡=๐ผ๐ด; ๐ด=๐œ‹๐‘…2โ‡’๐ตaxisโ‰ˆ๐œ‡04๐œ‹2๐œ‡๐‘Ÿ3
Similar to electric field Let electric dipole moment ๐‘=๐‘ž๐‘ โ‡’๐ธaxisโ‰ˆ14๐œ‹๐œ€02๐‘๐‘Ÿ3

Permanent Magnet

Current loop induces electromagnet, while electrons orbit atoms are atomic scale electomagnet. Electron orbiting atom in a p-orbital. When all the atomic magnet align, the material is a ferromagnet. The temperature at which atomic magnets align is called the curie temperature and is arel phase transition of the electrons inside a material, e.g. about 1000K. Electron orbits atom and electron also spins. Both act like electromagnets and both contribut to permanent magnet.
Some common ferromagnetic materials: iron, cobalt, nickel. The alignment of atomic dipole moments in ferromagnetic materials is along one direction to produce a strong magnetic as permanent magnet. The magnetic domains of ferromagnetic materials can also aligned by induced core. However, the magnetic field can also be demagnetized by hitting or heating.

Source and Reference

https://www.youtube.com/watch?v=JnhxIY0mHuw&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=13


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ID: 191201902 Last Updated: 12/19/2019 Revision: 0


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