/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 11 Is the potential at the center o... [FREE SOLUTION] | 91Ó°ÊÓ

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Is the potential at the center of a hollow, uniformly charged spherical shell higher than, lower than, or the same as at the surface?

Short Answer

Expert verified
The potential at the center of a hollow, uniformly charged spherical shell is the same as at the surface of the shell.

Step by step solution

01

Case Evaluation

We have a hollow, uniformly charged shell. Due to the principle of superposition and the symmetrical arrangement of charges on the sphere, electric field inside the shell is zero.
02

Formula Evaluation

The electric potential \( V \) at a point due to a point charge \( q \) is given by \( V = k*q/r \), where \( k \) is Coulomb's constant and \( r \) is the distance from the point to the charge source. Since the electric field \( E \) inside the shell is zero, and since \( V = E*r \), the potential \( V \) is constant inside the shell.
03

Potential Comparison

Due to the uniform distribution of charge on the shell, potential is same at all points inside the shell. Hence the potential at the center of the shell is the same as that on the surface of the shell.

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Most popular questions from this chapter

A sphere of radius \(R\) carries a nonuniform but spherically symmetric volume charge density that results in an electric field in the sphere given by \(\vec{E}=E_{0}(r / R)^{2} \hat{r},\) where \(E_{0}\) is a constant. Find the potential difference from the sphere's surface to its center.

Measurements of the potential at points on the axis of a charged disk are given in the two tables below, one for measurements made close to the disk and the other for measurements made far away. In both tables \(x\) is the coordinate measured along the disk axis with the origin at the disk center, and the zero of potential is taken at infinity. (a) For each set of data, determine a quantity that, when you plot potential against it, should yield a straight line. Make your plots, establish a best-fit line, and determine its slope. Use your slopes to find (b) the total charge on the disk and (c) the disk radius. (Hint: Consult Example 22.7.) Table 1 $$\begin{array}{|l|l|l|l|l|l|} \hline x(\mathrm{mm}) & 2.0 & 4.0 & 6.0 & 8.0 & 10.0 \\ \hline V(\mathrm{V}) & 900 & 876 & 843 & 820 & 797 \\ \hline \end{array}$$ Table 2 $$\begin{array}{|l|l|l|l|l|l|} \hline x(\mathrm{cm}) & 20 & 30 & 40 & 60 & 100 \\ \hline V(\mathrm{V}) & 165 & 118 & 80 & 58 & 30 \\ \hline \end{array}$$

Points \(A\) and \(B\) lie \(32.0 \mathrm{cm}\) apart on a line extending radially from a point charge \(Q,\) and the potentials at these points are \(V_{A}=362 \mathrm{V}\) and \(V_{B}=146 \mathrm{V} .\) Find \(Q\) and the distance \(r\) between point \(A\) and the charge.

The potential difference between the two sides of an ordinary electric outlet is \(120 \mathrm{V}\). How much energy does an electron gain when it moves from one side to the other?

Two equal but opposite charges form a dipole. Describe the equipotential surface on which \(V=0\)

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