Harmonic functions: Mean value theorem

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  • Опубликовано: 13 дек 2024

Комментарии • 19

  • @npr386
    @npr386 9 лет назад +7

    Learned more than the class I paid $1200 to attend... Thanks

  • @porkypine1888
    @porkypine1888 11 лет назад +2

    Exciting... I'm seeing all of these ideas I know about and heaps I have no idea about and understanding how all this fits together is a boggle. Can't wait till the holidays :D

  • @gustavobagu7156
    @gustavobagu7156 6 лет назад +1

    Minute 10:28 ... an R should come out in front of the partial d/dr ... Right?

  • @АртемПоляков-ж6ю
    @АртемПоляков-ж6ю 7 лет назад +3

    9:40 if you use "chain rule" R disapear, you will have ux cost+uy sint , doesn't it?

    • @infinity-and-regards
      @infinity-and-regards 5 лет назад

      Same here? Anyone have an answer for this or is this just a little mistake?

    • @infinity-and-regards
      @infinity-and-regards 5 лет назад +1

      Did some thinking, and you are right; this is wrong. However, the rest of the proof is still correct with one additional observation:
      R*u_R = u_x Rcos(t) + u_y Rsin(t)
      One can take the constant R out of the integral and divide both sides (0 on the LHS and the integral on the RHS) by R. From there the proof can continue as in the video. That is why Dr. C gets the same result, he just missed a little calculational step.

  • @gustavobagu7156
    @gustavobagu7156 6 лет назад +1

    My question to you, Chris, is why did you change "r" (radius of the ball), for "R", in the proof.

  • @zeinabashtab1456
    @zeinabashtab1456 4 года назад

    thanks, can You please explain why the solutions of Laplace's equations are continuous?

  • @fsr7860
    @fsr7860 9 лет назад +2

    Great Video, Thank you!

  • @minhokim8263
    @minhokim8263 4 года назад

    I think it would be easier to introduce the directional derivative of direction of radial vector instead of parameterising.

  • @flaminhotzerg
    @flaminhotzerg 9 лет назад +1

    Great video, ty!

  • @finweman
    @finweman 6 лет назад

    Something isn't quite right. at 9:40 you claim that d/dR by the chain rule would give you the integrand but it doesn't. You have an extra R in the integrand. I think the reason is that you didn't divide by |r'(t)| = R which is necessary to give you the unit normal since you are not parameterizing by arc length. Or, I could be wrong.

    • @haraldtasti372
      @haraldtasti372 5 лет назад +1

      It seems he includes a R to much when he takes the chain rule derivative of Rcos(t).
      When he does the subsequent inverse derivation on R, he does it as if the above R does not exist. Thus, the derivation is OK, it seems despite a "typgraphic" error. These Videos are extremly valueable, they make an almost forbidding area of mathematics approachable wirhout the fuss of complex incomprihensible formalities of greek letters etc.

    • @haraldtasti372
      @haraldtasti372 5 лет назад

      On furher reflexion, he explicitly declares R as a constant. Thus, he can divide og multiply both sides by R without changing the equation. However, he treats R in one contest as a constant, in the other as a variable. I suppose this is OK

  • @matthiasstahli239
    @matthiasstahli239 8 лет назад +3

    why is it Ux*dy -Uy*dx and not Ux*dx + Uy*dy ??
    good video!

    • @gustavobagu7156
      @gustavobagu7156 6 лет назад

      Because (Ux, Uy) is projected against the normal to the curve, and not against the tangent, as you usually would do to compute the circulation... He is interested in the outward flux in this case

    • @mohammedal-haddad2652
      @mohammedal-haddad2652 4 года назад +1

      @@gustavobagu7156 I think it is the opposite, (dx,dy) is normal to the curve and (dy,-dx) is tangential to the curve.

    • @davidkwon1872
      @davidkwon1872 4 года назад

      Thank you, but still I don’t understand it. ㅜㅜ;;;

  • @ernestooropeza6150
    @ernestooropeza6150 9 лет назад +1

    OMEGA!!!