/*! 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 31 Charge Is Distributed Uniformly ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Charge Is Distributed Uniformly Charge is distributed uniformly throughout the volume of an infinitely long cylinder of radius \(R\). (a) Show that, at a distance \(r\) from the cylinder axis (for \(rR\)

Short Answer

Expert verified
Inside ( r < R): \(|\vec{E}| \frac{|\rho| r}{2 \varepsilon_{0}}\). Outside ( r > R): \(|\vec{E}| \frac{|\rho| R^2}{2 \varepsilon_{0} r}\).

Step by step solution

01

Understanding the problem

Charge is distributed uniformly throughout the volume of an infinitely long cylinder of radius R. Need to find the electric field at a distance r from the axis for both r < R and r > R.
02

Using Gauss's Law Inside the Cylinder (r

Gauss's Law states \(\oint\vec{E} \cdot d\vec{A} = \frac{Q_{enc}}{\varepsilon_{0}}\). For an infinitely long cylinder, choose a cylindrical Gaussian surface of radius r<R and length L. The enclosed charge is given by \(Q_{enc} = \rho \pi r^2 L\), where \(\rho\) is the volume charge density. Since the electric field \(\vec{E}\) is radially symmetrical, \(\vec{E} \) is constant over the surface area which is \(2 \pi r L\).
03

Calculating the Enclosed Charge Inside the Cylinder

Integrate Gauss’s Law: \(E (2 \pi r L) = \frac{\rho \pi r^2 L}{\varepsilon_{0}}\). Divide both sides by \(2 \pi r L\) to solve for \(E\): \(E = \frac{\rho r}{2 \varepsilon_{0}}\). Thus, \(|\vec{E}| = \frac{|\rho| r}{2 \varepsilon_{0}}\).
04

Using Gauss's Law Outside the Cylinder (r>R)

For the case r>R, choose a cylindrical Gaussian surface of radius r>R and length L. The enclosed charge remains constant and is given by the total charge of the cylinder of radius R and length L, \(Q_{enc} = \rho \pi R^2 L\).
05

Calculating the Electric Field Outside the Cylinder

Using Gauss’s Law: \(E (2 \pi r L) = \frac{\rho \pi R^2 L}{\varepsilon_{0}}\). Divide both sides by \(2 \pi r L\) to solve for \(E\): \(E = \frac{\rho R^2}{2 \varepsilon_{0} r}\). Thus, \(|\vec{E}| = \frac{|\rho| R^2}{2 \varepsilon_{0} r}\).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Electric Field
The electric field, denoted as \(\text{E}\), is a vector field that represents the force per unit charge exerted on a positive test charge at any point in space. In simpler terms, it shows how a charge would 'feel' the force at a particular location. The electric field due to a distribution of charges can be found using Gauss's Law, making calculations more manageable, especially in systems with symmetrical charge distributions.
The electric field inside and outside a charged cylinder depends on the distance from the cylinder's axis. The field inside the cylinder increases linearly with distance from the center, while outside, it decreases with distance.
Uniform Charge Distribution
A uniform charge distribution means that charge is spread evenly throughout a given volume. In the context of this exercise, the charge is distributed uniformly along the volume of an infinitely long cylinder. This means the volume charge density, called \(\rho\), remains constant throughout the cylinder. This simplifies calculations as \(\rho\) doesn't change at different points within the cylinder.
For uniform charge distribution:
  • The charge per unit volume is constant.
  • The total charge can be calculated by multiplying the volume charge density \(\rho\) by the volume.
Cylindrical Symmetry
Cylindrical symmetry means that a system looks the same when rotated around a particular axis. In our exercise, the cylinder's charge distribution remains unchanged irrespective of how we rotate around its central axis. This symmetry simplifies the use of Gauss's Law to find the electric field because:
  • The electric field depends only on the radial distance \(\text{r}\) from the axis, not the angle or height.
  • A cylindrical Gaussian surface matches the symmetry, making the calculations straightforward.
The symmetry helps in reducing a 3D problem to a simpler 1D radial dependency.
Volume Charge Density
Volume charge density, denoted as \(\rho\), is a measure of the amount of electric charge per unit volume at a given location. For our problem, the volume charge density is constant throughout the cylinder, indicating a uniform charge distribution. Volume charge density is crucial because:
  • It helps in calculating the enclosed charge for Gauss's Law.
  • The relationship between \(\rho\) and the electric field is direct, simplifying the determination of the field.
In mathematical terms, the enclosed charge \(Q_{enc}\) inside a Gaussian surface is given by \(Q_{enc} = \rho \times \text{Volume enclosed by the surface}\).
Gaussian Surface
A Gaussian surface is an imaginary closed surface used in Gauss's Law to simplify the calculation of electric fields due to symmetrical charged objects. In this exercise, we use cylindrical Gaussian surfaces to leverage the cylindrical symmetry of the problem. When choosing a Gaussian surface:
  • It should match the symmetry of the charge distribution.
  • For points inside the cylinder \(r
  • For points outside the cylinder \(r>R\), the Gaussian surface is a larger coaxial cylinder enclosing the entire charge.
The electric flux through the Gaussian surface is connected to the enclosed charge, making it easier to find the electric field through \(\oint \vec{E} \cdot d\vec{A} = \frac{Q_{enc}}{\varepsilon_0}\).

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Conducting Sphere A conducting sphere of radius \(10 \mathrm{~cm}\) has an unknown charge. If the electric field \(15 \mathrm{~cm}\) from the center of the sphere has the magnitude \(3.0 \times 10^{3} \mathrm{~N} / \mathrm{C}\) and is directed radially inward, what is the net charge on the sphere?

Uniform Volume Charge Density Figure 24-29a shows a spherical shell of charge with uniform volume charge density \(\rho .\) Plot \(E\) due to the shell for distances \(r\) from the center of the shell ranging from zero to \(30 \mathrm{~cm}\). Assume that \(\rho=1.0 \times 10^{-6} \mathrm{C} / \mathrm{m}^{3}, a=10 \mathrm{~cm}\), and \(b=20 \mathrm{~cm}\).

Charged Sphere A uniformly charged conducting sphere of \(1.2 \mathrm{~m}\) diameter has a surface charge density of \(8.1 \mu \mathrm{C} / \mathrm{m}^{2} .\) (a) Find the net charge on the sphere. (b) What is the total electric flux leaving the surface of the sphere?

Arbitrary Shape Conductor An isolated conductor of arbitrary shape has a net charge of \(+10 \times 10^{-6} \mathrm{C}\). Inside the conductor is a cavity within which is a point charge \(q=+3.0 \times 10^{-6} \mathrm{C}\). What is the charge (a) on the cavity wall and (b) on the outer surface of the conductor?

Large Metal Plates Two large metal plates of area \(1.0 \mathrm{~m}^{2}\) face each other. They are \(5.0 \mathrm{~cm}\) apart and have equal but opposite charges on their inner surfaces. If the magnitude \(|\vec{E}|\) of the electric field between the plates is \(55 \mathrm{~N} / \mathrm{C}\), what is the amount of charge on each plate? Neglect edge effects.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.