/*! 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 6 Inside a hollow charged spherica... [FREE SOLUTION] | 91Ó°ÊÓ

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Inside a hollow charged spherical conductor, the potential a. is constant b. varies directly as the distance from the center c. varies inversely as the distance from the center d. varies inversely as the square of the distance from the center

Short Answer

Expert verified
The potential inside a hollow charged spherical conductor is constant.

Step by step solution

01

Understanding the Concept of Electric Potential in a Conductor

In a conductive sphere, charges reside on the surface due to the repulsion between like charges. This surface charge distribution leads to a uniform electric field inside the conductor itself, resulting in a constant electric potential in the hollow region.
02

Applying Gauss's Law for a Spherical Conductor

According to Gauss's Law, the electric field inside a conductor is zero when in electrostatic equilibrium. Since the electric field \( E = -abla V \) is zero, the potential \( V \) must be uniform and not vary with distance.
03

Conclusion on the Variation of Potential

Since the electric field inside the hollow conductor is zero, the electric potential remains constant throughout the hollow region of the sphere. Thus option \( a \) is the correct answer.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Gauss's Law
Gauss's Law is a fundamental principle that helps us understand electric fields and their relation to electric charges. This law says that the electric flux through a closed surface is proportional to the charge enclosed by that surface. Mathematically, it is expressed as \( \Phi = \frac{Q_{enclosed}}{\varepsilon_0} \), where \( \Phi \) is the electric flux, \( Q_{enclosed} \) is the total charge inside the surface, and \( \varepsilon_0 \) is the permittivity of free space.
Gauss's Law is particularly useful for symmetric charge distributions, like spherical conductors. For a spherical conductor in electrostatic equilibrium, Gauss's Law tells us that the electric field inside is zero. This is because the charges reside on the surface of the conductor, creating an area of zero electric field inside.
In essence, within a spherical conductor, the lack of interior electric field results in a uniform electric potential. The concept is powerful as it simplifies calculations and helps us predict how electric fields behave based on the symmetry of charge distributions.
Spherical Conductor
A spherical conductor, as the name suggests, is a conductor shaped like a sphere. One key characteristic of such conductors is that charges on the sphere reside on the outer surface. This is due to the nature of electrostatic repulsion, which pushes like charges as far apart as possible.
This surface charge distribution means that inside the spherical conductor, the electric field is zero when in electrostatic equilibrium. This occurs because the electric fields from the surface charges cancel each other out within the hollow part of the sphere.
  • Since there is no electric field inside, the electric potential remains constant throughout the hollow space.
  • This holds true for any point within the inner region of the spherical conductor, emphasizing that the potential is not influenced by the distance from the center.
These attributes make spherical conductors very significant in understanding electric potential and field behavior.
Electrostatic Equilibrium
Electrostatic equilibrium occurs when the charges within a conductor are at rest and evenly distributed across the surface. This means there is no relative motion between charges, and the electric field within the conductor is zero.
In this state, the interior of the conductor experiences constant electric potential, as there are no variations in the electric field to cause changes.
  • Since the electric field inside the conductor is zero, the potential difference across any two points is zero, leading to a uniform potential situation.
  • The surface, however, may have a non-zero electric field just outside, influencing the surrounding environment.
Understanding electrostatic equilibrium helps with predicting the behavior of electric fields and potentials, particularly in spherical conductors, where it leads to a constant electric potential inside.

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Most popular questions from this chapter

When the separation between two charges is increased, the electric potential energy of the charges a. increases b. decreases c. remains the same d. may increase or decrease

A solid conducting sphere having a charge \(Q\) is surrounded by an uncharged concentric conducting hollow spherical shell. The potential difference between the surface of the solid sphere and that of the outer surface of the hollow shell is \(V\). If the shell is now given a charge of \(-3 Q\), the new potential difference between the same two surfaces is (IIT-JEE, 1989) a. \(V\) b. \(2 V\) c. \(4 \mathrm{~V}\) d. \(-2 V\)

Four identical charges are placed at the points \((1,0,0)\), \((0,1,0),(-1,0,0)\) and \((0,-1,0)\). Then, a. the potential at the origin is zero b. the electric field at the origin is not zero c. the potential at all points on the \(z\) -axis, other than the origin, is zero d. the field at all points on the \(z\) -axis, other than the origin, acts along the \(z\) -axis

A hollow metal sphere of radius \(5 \mathrm{~cm}\) is charged such that the potential on its surface is \(10 \mathrm{~V}\). The potential at the center of the sphere is a. \(0 \mathrm{~V}\) b. \(10 \mathrm{~V}\) c. same as at point \(5 \mathrm{~cm}\) away from the surface d. same as at a point \(20 \mathrm{~cm}\) away from the surface

We bave three identical metallic spheres \(A, B\), and \(C, A\) is given a charge \(Q\) and \(B\) and \(C\) are uncharged. The following processes of touching of two spheres is camied out in succession. Each process is carried out with sufficient time: i. \(A\) and \(B\) ii. \(B\) and \(C\) iii. \(C\) and \(A\) iv. \(A\) and \(B\) v. \(B\) and \(C\) The final charges on the spheres are a. \(\frac{11 Q}{32}, \frac{5 Q}{16}, \frac{11 Q}{32}\) b. \(\frac{11 Q}{32}, \frac{11 Q}{32}, \frac{5 Q}{16}\) C. \(\frac{8 Q}{8}, \frac{5 Q}{16}, \frac{5 Q}{16}\) d. \(\frac{5 Q}{16}, \frac{11 Q}{32}, \frac{11 Q}{32}\)

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