Charged Sphere sliced, force required to keep them as they were

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AGNuke
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A metallic sphere of radius R is cut in two parts along a plane whose minimum distance from the sphere's centre is h and the sphere is uniformly charged by a total electric charge Q. What minimum force is necessary to hold the two parts of the sphere together?

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The solution which we were "encouraged" to come up was using a term called "electric pressure", defined as the electrostatic force per unit area. By multiplying it with the base area of the cross-section obtained after slicing the sphere, I got the answer.

[tex]P_{el}=\frac{\sigma ^{2}}{2\varepsilon _{0}}; \; \sigma =\frac{Q}{4\pi R^2}[/tex]
[tex]F_{el}=P_{el}\times S; \; S=\pi(R^2-h^2)[/tex]
[tex]F_{el}=\frac{\frac{Q^2}{16\pi^2R^4}}{2\varepsilon_{0}}\times \pi(R^2-h^2)=\frac{Q^2(R^2-h^2)}{32\pi\varepsilon_{0}R^4}[/tex]

Now I actually didn't get the concept here, what was that supposed to mean. Isn't there a conventional way to solve this problem?
 
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Hi AGNuke. I'm not too clear on what specific question you are asking. Are you asking why the pressure is given by σ2/2εo or are you asking why the force is given by F = P*[itex]\pi[/itex](R2-h2)? Or are you asking something else?

The expression for the pressure can be obtained in a fairly conventional way by considering the force on a small patch of area of the surface of a charged conductor.
 
TSny, I am sorry if I was unable to convey my question properly, but I am asking that can I solve this question using coulomb's law and some other textbook stuff like properties of conductors, etc.?

I mean, if I don't know the concept of electric field (which I am still trying to justify, even if for a sphere), can I solve it? If so, then what should I do? (Coulomb's Law?)
 
A direct integration using Coulomb's law is a bit messy. Using the following concepts involving electric field makes it a lot easier:

(1) The relation between force and electric field: F = qE

(2) The relation between electric field at the surface of a conductor and the charge density: E = σ/εo

(3) The electric field produced by a large flat sheet of uniform charge density: E = σ/2εo

The latter 2 properties are easily derived from Gauss' law.