Consider two spherical infinitely thin conducting surfaces (= ∞o) with the same center. The cross section of this configuration is shown below. The inner sphere (radius a) has a total negative charge of -Q. The outer sphere (radius b) has a positive charge with unknown amount. Assume the electric potential at the center is Vo (Vo > 0) and at infinity is zero. Also, assume free-space permittivity in all regions. (a) Find the electric potential V(R) at the distance R from the center for 0 < R < b. (b) Find the amount of positive charge on the outer sphere. Hint: The integral form of Gauss' Law is your best friend! Also you may pay close attention to the net charge.
Consider two spherical infinitely thin conducting surfaces (= ∞o) with the same center. The cross section of this configuration is shown below. The inner sphere (radius a) has a total negative charge of -Q. The outer sphere (radius b) has a positive charge with unknown amount. Assume the electric potential at the center is Vo (Vo > 0) and at infinity is zero. Also, assume free-space permittivity in all regions. (a) Find the electric potential V(R) at the distance R from the center for 0 < R < b. (b) Find the amount of positive charge on the outer sphere. Hint: The integral form of Gauss' Law is your best friend! Also you may pay close attention to the net charge.
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Transcribed Image Text:Consider two spherical infinitely thin conducting surfaces (= ∞o) with the same center. The cross section
of this configuration is shown below. The inner sphere (radius a) has a total negative charge of -Q. The
outer sphere (radius b) has a positive charge with unknown amount.
Assume the electric potential at the center is Vo (Vo > 0) and at infinity is zero. Also, assume free-space
permittivity in all regions.
(a) Find the electric potential V(R) at the distance R from the center for 0 < R < b.
(b) Find the amount of positive charge on the outer sphere.
Hint: The integral form of Gauss' Law is your best friend! Also you may pay close attention to the
net charge.
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