5.4.1 Example 12

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  • čas přidán 28. 08. 2024
  • 5.4.1 of Griffith's Introduction to Electrodynamics 2nd Ed
    Find the A for an infinite solenoid.
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Komentáře • 9

  • @jasonyao3753
    @jasonyao3753 Před 2 lety +4

    "he calls that cute...if you're into anime" lmao

  • @michaeldejong6819
    @michaeldejong6819 Před měsícem

    how do we mathematically justify that the magnetic vector potential always points along the circumference of a given amperian loop with the same magnitude? I don't see how B being constant inside the solenoid implies this.

  • @user-qo2ck3bg9w
    @user-qo2ck3bg9w Před 3 měsíci

    Thanks

  • @panthopothik6338
    @panthopothik6338 Před 4 lety +1

    Excellent explanation! Thank you

  • @Math_Addicted111
    @Math_Addicted111 Před 6 měsíci

    How to prove if del×A=B

  • @kevinlification
    @kevinlification Před 6 lety

    thanks man

  • @hiranawaz7357
    @hiranawaz7357 Před 4 lety

    why u not upload 5.10 example......

  • @anereeee
    @anereeee Před 8 lety

    How did you decide the direction of A?

    • @mattbeaulieu2301
      @mattbeaulieu2301 Před 8 lety +2

      +Aneree Mehta
      A generally travels in the direction of the current, and the current of the solenoid travels through the wire, in the circular direction shown. The reasoning is written in the book as the paragraph after example 12.
      The paragraph in question, copied out of the 4th edition of the Griffiths book.
      "Typically, the direction of A mimics the direction of the current. For instance,
      both were azimuthal in Exs. 5.11 and 5.12. Indeed, if all the current flows in
      one direction, then Eq. 5.65 suggests that A must point that way too. Thus the
      potential of a finite segment of straight wire (Pro b. 5.23) is in the direction of the
      current. Of course, if the current extends to infinity you can't use Eq. 5.65 in the
      first place (see Probs. 5.26 and 5.27). Moreover, you can always add an arbitrary
      constant vector to A-this is analogous to changing the reference point for V, and
      it won't affect the divergence or curl of A, which is all that matters (in Eq. 5.65
      we have chosen the constant so that A goes to zero at infinity). In principle you
      could even use a vector potential that is not divergenceless, in which case all bets
      are off. Despite these caveats, the essential point remains: Ordinarily the direction
      of A will match the direction of the current."