Difference Between Thin and Conductive charge configurations

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The discussion explores the computational differences between thin spherical insulating and conductive shells, particularly in the context of capacitors. It emphasizes that while textbooks state capacitors must be conductors, insulating shells can theoretically have capacitance, although they are impractical for actual capacitor functionality. The conversation highlights that charge distribution on insulating surfaces remains static, limiting their effectiveness compared to conductive materials that allow charge movement. Additionally, it notes that capacitive sensors can exhibit capacitance without functioning as traditional capacitors due to the necessary voltage/current relationship. Ultimately, the practicality of charging and the nature of charge movement are critical in defining effective capacitors.
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Difference Between "Thin" and "Conductive" charge configurations

Is there any difference computationally between say a thin spherical insulating shell and a thin conductive shell ?

Can you create a capacitor with two thin insulating shells, one smaller than the other ?

I see most textbooks explicitly say that capacitors must be conductors. Is this so ?
 
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The charge enters the capacitor from outside - with an insulator the incoming charge is stuck in one spot, so it would make a lousy capacitor. With conducting surfaces source charges can flow so that the entire surface is charged (both plates/spheres).

The region between the conductors is the insulator; the charges on the plates induce small movements in the molecules of the conductor - they "polarize" the material, but no charge moves more than a few nanometers.
 
Say a charge is already uniformly distributed on the thin spheres. Can you talk about capacitance then ? I realize that it is the practicality of charging that is the problem, but textbooks talk about uniform charge on insulators all the time.
 
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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