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astro2cosmos
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suppose there is a uncharged thin spherical ball (thickness tends to 0) then Does if have any capacitance if a +q charge is placed near it?
iitjee10 said:yes there will be an induced charge on the shell due to which there will be some capacitance
saunderson said:Yes, you need a reference point to specify the capacitance of the spherical ball, due to
[tex]C = \frac{Q}{\phi(A) - \phi(B)}[/tex]
with [tex]\phi(A)[/tex]: potential on the surface of the ball; [tex]\phi(B)[/tex]: potential on the surface, the reference point is on
If the reference point is in infinity, we know that the potential in infinity must vanish, cause only in this case the energy is finite. So we can take [tex]B=\infty[/tex] (imagine a giant spherical capacitor which outer shell is in infinity with the potential [tex]\phi(\infty)=0[/tex]). In this term we can derive the capacitance of the spherical ball!
astro2cosmos said:i didn't get the phi(B)}[/tex]. which surface do you mention here??
Capacitance is a measure of an object's ability to store an electric charge. It is defined as the ratio of the electric charge on an object to the potential difference across the object.
The capacitance of a thin spherical ball can be calculated using the following formula: C = 4πεr, where C is the capacitance, ε is the permittivity of the material between the two conductors, and r is the radius of the sphere.
The capacitance of a thin spherical ball is affected by the radius of the sphere, the distance between the two conductors, and the permittivity of the material between the conductors. It is also affected by the presence of any other nearby conductors or insulators.
The material of the thin spherical ball affects its capacitance through its permittivity, which is a measure of how easily electric fields can pass through the material. Materials with higher permittivity have a higher capacitance, while materials with lower permittivity have a lower capacitance.
The unit of measurement for capacitance is the farad (F). It is named after the scientist Michael Faraday and is defined as one coulomb of charge per volt of potential difference.