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Ch 23: Electric Potential
Chapter 23, Problem 23

A thin spherical shell with radius R_1 = 3.00 cm is concentric with a larger thin spherical shell with radius R_2 = 5.00 cm. Both shells are made of insulating material. The smaller shell has charge q_1 = +6.00 nC distributed uniformly over its surface, and the larger shell has charge q_2 = -9.00 nC distributed uniformly over its surface. Take the electric potential to be zero at an infinite distance from both shells. (a) What is the electric potential due to the two shells at the following distance from their common center: (i) r=0; (ii) r=4.00 cm; (iii) r=6.00 cm?

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Identify the regions of interest based on the given radii and distances: (i) Inside the inner shell (r < R_1), (ii) Between the shells (R_1 < r < R_2), (iii) Outside the outer shell (r > R_2).
Use the formula for the electric potential V due to a spherical shell of charge Q at a distance r from the center, which is V = kQ/r for r >= R (outside the shell) and V = kQ/R for r < R (inside the shell), where k is Coulomb's constant.
Calculate the electric potential at r = 0 by considering the contributions from both shells. Since the point is inside both shells, use the potential formula for inside the shell.
Calculate the electric potential at r = 4.00 cm. This point is outside the smaller shell but inside the larger shell. Use the appropriate potential formulas for each region and sum the contributions from both shells.
Calculate the electric potential at r = 6.00 cm. This point is outside both shells. Use the potential formula for points outside the shell for each shell and sum their contributions.

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Electric Potential

Electric potential is the amount of electric potential energy per unit charge at a point in an electric field. It is a scalar quantity measured in volts (V) and indicates the work done to move a unit positive charge from infinity to that point. The potential due to a point charge decreases with distance, and for spherical charge distributions, it can be treated as if all charge were concentrated at the center for points outside the shell.
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Electric Potential

Gauss's Law

Gauss's Law relates the electric flux through a closed surface to the charge enclosed by that surface. For spherical charge distributions, it simplifies the calculation of electric fields and potentials. Inside a uniformly charged spherical shell, the electric field is zero, while outside, the shell behaves like a point charge located at its center, allowing for straightforward potential calculations.
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Superposition Principle

The superposition principle states that the total electric potential at a point due to multiple charges is the algebraic sum of the potentials due to each charge individually. This principle is crucial when dealing with multiple charge distributions, as it allows for the calculation of the net potential by considering the contributions from each shell separately, regardless of their interactions.
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Related Practice
Textbook Question
Two large, parallel conducting plates carrying op­posite charges of equal magnitude are separated by 2.20 cm. The surface charge density for each plate has magnitude 47.0 nC/m^2. (c) If the separation between the plates is doubled while the surface charge density is kept constant at the given value, what happens to the magnitude of the electric field and to the po­tential difference?
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Textbook Question
(a) How much excess charge must be placed on a copper sphere 25.0 cm in diameter so that the potential of its center, rela­tive to infinity, is 3.75 kV? (b) What is the potential of the sphere's surface relative to infinity?
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Textbook Question
Two stationary point charges +3.00 nC and +2.00 nC are separated by a distance of 50.0 cm. An electron is released from rest at a point midway between the two charges and moves along the line connecting the two charges. What is the speed of the electron when it is 10.0 cm from the +3.00-nC charge?
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Textbook Question
(a) How much work would it take to push two protons very slowly from a separation of 2.00x10^-10 m (a typical atomic distance) to 3.00x10^-15 m (a typical nuclear distance)? (b) If the protons are both released from rest at the closer distance in part (a), how fast are they moving when they reach their original separation?
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Textbook Question
A small metal sphere, carrying a net charge of q_1 = -2.80 μC, is held in a stationary position by insulat­ing supports. A second small metal sphere, with a net charge of q_2 = -7.80 μC and mass 1.50 g, is projected toward q_1. When the two spheres are 0.800 m apart, q_2, is moving toward q_1 with speed 22.0 m/s (Fig. E23.5). Assume that the two spheres can be treated as point charges. You can ignore the force of gravity. (a) What is the speed of q_2 when the spheres are 0.400 m apart?
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Textbook Question
CALC. A metal sphere with radius r_a is supported on an insulating stand at the center of a hollow, metal, spherical shell with radius r_b. There is charge +q on the inner sphere and charge -q on the outer spherical shell. (a) Calculate the potential V(r) for (i) r < r_a; (ii) r_a < r < r_b; (iii) r > r_b. (Hint: The net potential is the sum of the potentials due to the individual spheres.) Take V to be zero when r is infinite. (b) Show that the potential of the inner sphere with respect to the outer is V_ab=q/(4πϵ_0 ) (1/r_a -1/r_b). (c) Use E_r=-∂V/∂r=(-∂/∂r) (1/(4πϵ_0 ) q/r)=[1/(4πϵ_0 )](q/r^2) and the result from part (a) to show that the electric field at any point between the spheres has magnitude E(r)=[V_ab/(1/r_a -1/r_b )](1/r^2) (d) Use E_r = [1/(4πϵ_0 )](q/r^2) and the result from part (a) to find the electric field at a point outside the larger sphere at a distance r from the center, where r > r_b. (e) Suppose the charge on the outer sphere is not -q but a negative charge of different magnitude, say -Q. Show that the answers for parts (b) and (c) are the same as before but the answer for part (d) is different.
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