A Question of Electrostatic Repulsion

It’s been a while since I posted a question in the Cute Physics Problems folder so I thought I’d offer this one. It’s not particularly hard, but I think it’s quite instructive.

A thin spherical shell of radius r carrying a charge Q spread uniformly with constant surface density is split into two equal halves by a narrow planar cut passing through the centre as shown in the detailed diagram below:

 

Calculate the force arising from electrostatic repulsion between the two hemispherical shells, expressing your answer in terms of Q and r in SI units.

Answers through the Comments Box please. First correct answer wins a tomato*

*subject to availability

9 Responses to “A Question of Electrostatic Repulsion”

  1. The electric field at the surface of the sphere is
    E = Q/r2,
    directed radially.
    Integrating F = ½ ∫Edq
    over the uniform charge distribution across
    the top half of the sphere gives a force
    F = ⅛
    Q/r2,
    directed upwards.
    Of the one eighth, one half is because the top has half the charge,
    one half is the half in the expression, from removing the self-field
    to obtain the externally applied field
    (averaging the inner and outer fields),
    and one half is from the geometric integral
    (average of the vertical component).
    The horizontal components sum to zero.
    Add the usual 1/4πε0 to get SI units.

    Or, maybe not, I haven’t been practicing lately.

  2. Jim Fry's avatar
    Jim Fry Says:

    Q2/r2, of course. And “up” is to the right.

    • telescoper's avatar
      telescoper Says:

      I’m afraid that’s not the right answer…even accounting for the lack of SI units!

      • Jim Fry's avatar
        Jim Fry Says:

        Somehow the original post didn’t make it, and what was to be
        a quick correction did.
        Here it is again, complete with the error:

        The electric field at the surface of the sphere is
        E = Q/r², directed radially.
        Integrating F = ½ ∫Edq
        over the uniform charge distribution across
        the top half of the sphere gives a force
        F = ⅛ Q/r&#178, directed upwards.
        Of the one eighth, one half is because the top has half the charge,
        one half is the half in the expression, from removing the self-field to
        obtain the externally applied field (averaging the inner and outer fields),
        and one half is from the geometric integral
        (average of the vertical component).
        The horizontal components sum to zero.
        Add the usual 1/4πε0 to get SI units.
        Or, maybe not, I haven’t been practicing lately.

        So, the SI issue was addressed.
        There is a YouTube video that does all integrals, but I couldn’t watch
        the whole thing and I never see it get to an answer.

  3. Andries's avatar
    Andries Says:

    8/9 k Q/r2
    with k the Coulomb constant

  4. Jim Fry's avatar
    Jim Fry Says:

    Somehow the original post didn’t make it, and what was to be
    a quick correction did.
    Here it is again, complete with the error:

    The electric field at the surface of the sphere is
    E = Q/r²,
    directed radially.
    Integrating F = ½ ∫Edq
    over the uniform charge distribution across
    the top half of the sphere gives a force
    F = ⅛ Q/r&#178,
    directed upwards.
    Of the one eighth, one half is because the top has half the charge,
    one half is the half in the expression, from removing the self-field
    to obtain the externally applied field
    (averaging the inner and outer fields),
    and one half is from the geometric integral
    (average of the vertical component).
    The horizontal components sum to zero.
    Add the usual 1/4πε0 to get SI units.
    Or, maybe not, I haven’t been practicing lately.

    So, the SI issue was addressed.
    There is a YouTube video that does all integrals, but I couldn’t watch
    the whole thing and I never say it get to an answer.

  5. Jim Fry's avatar
    Jim Fry Says:

    Somehow the original post didn’t make it, and what was to be a quick correction did.
    Here it is again, complete with the error:

    The electric field at the surface of the sphere is E = Q/r², directed radially.
    Integrating F = ½ ∫Edq
    over the uniform charge distribution across
    the top half of the sphere gives a force
    F = ⅛ Q/r&#178, directed upwards.
    Of the one eighth, one half is because the top has half the charge, one half is the half in the integral expression, from removing the self-field to obtain the externally applied field (averaging the inner and outer fields), and one half is from the geometric integral (average of the vertical component).
    The horizontal components sum to zero.
    Add the usual 1/4πε0 to get SI units.
    Or, maybe not, I haven’t been practicing lately.

    So, the SI issue was addressed.
    There is a YouTube video that does all integrals, but I couldn’t watch the whole thing and I never saw it get to an answer.

  6. John Peacock's avatar
    John Peacock Says:

    Q^2 / (32pi epsilon_0 r^2)

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