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The electric field must be zero inside a conductor in electrostatic equilibrium, but not inside an insulator. It turns out that we can still apply Gauss's law to a Gaussian surface that is entirely within an insulator by replacing the right-hand side of Gauss's law, Qin/eo, with Qin/e, where ε is the permittivity of the material. (Technically, Eo is called the vacuum permittivity.) Suppose that a 70 nC point charge is surrounded by a thin, 32-cm-diameter spherical rubber shell and that the electric field strength inside the rubber shell is 2500 N/C.
What is the permittivity of rubber?

Respuesta :

Answer:

The permittivity of rubber is  [tex]\epsilon = 8.703 *10^{-11}[/tex]

Explanation:

From the question we are told that

     The  magnitude of the point charge is  [tex]q_1 = 70 \ nC = 70 *10^{-9} \ C[/tex]

      The diameter of the rubber shell is  [tex]d = 32 \ cm = 0.32 \ m[/tex]

       The Electric field inside the rubber shell is  [tex]E = 2500 \ N/ C[/tex]

The radius of the rubber is  mathematically evaluated as

              [tex]r = \frac{d}{2} = \frac{0.32}{2} = 0.16 \ m[/tex]

Generally the electric field for a point  is in an insulator(rubber) is mathematically represented as

         [tex]E = \frac{Q}{ \epsilon } * \frac{1}{4 * \pi r^2}[/tex]

Where [tex]\epsilon[/tex] is the permittivity of rubber

    =>     [tex]E * \epsilon * 4 * \pi * r^2 = Q[/tex]

   =>      [tex]\epsilon = \frac{Q}{E * 4 * \pi * r^2}[/tex]

substituting values

            [tex]\epsilon = \frac{70 *10^{-9}}{2500 * 4 * 3.142 * (0.16)^2}[/tex]

            [tex]\epsilon = 8.703 *10^{-11}[/tex]