/*! 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 22 An electron is released \(9.0 \m... [FREE SOLUTION] | 91Ó°ÊÓ

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An electron is released \(9.0 \mathrm{~cm}\) from a very long nonconducting rod with a uniform \(6.0 \mu \mathrm{C} / \mathrm{m} .\) What is the magnitude of the electron's initial acceleration?

Short Answer

Expert verified
The electron's initial acceleration is approximately \(2.10 \times 10^{17} \, \text{m/s}^2\).

Step by step solution

01

Identify Given Values

We have the following values: The linear charge density \( \lambda = 6.0 \, \mu\text{C/m} \) or \( 6.0 \times 10^{-6} \, \text{C/m} \), the distance from the rod \( r = 9.0 \, \text{cm} \) or \( 0.09 \, \text{m} \), and the electron's charge \( e = -1.6 \times 10^{-19} \, \text{C} \). The electron's mass \( m = 9.11 \times 10^{-31} \, \text{kg} \).
02

Determine Electric Field from Rod

The electric field \( E \) produced by an infinitely long charged rod at a distance \( r \) is given by \( E = \frac{\lambda}{2 \pi \varepsilon_0 r} \). Using \( \varepsilon_0 = 8.85 \times 10^{-12} \, \text{C}^2/(\text{N} \cdot \text{m}^2) \), the electric field at \( r = 0.09 \, \text{m} \) is: \[ E = \frac{6.0 \times 10^{-6}}{2 \pi \times 8.85 \times 10^{-12} \times 0.09} \].
03

Calculate the Electric Field Value

Substitute the known values into the equation from Step 2: \[ E = \frac{6.0 \times 10^{-6}}{2 \pi \times 8.85 \times 10^{-12} \times 0.09} \approx 1.196 \times 10^{6} \, \text{N/C} \].
04

Determine Force on the Electron

The force \( F \) on an electron in an electric field \( E \) is given by \( F = eE \). Using the electric field from Step 3: \[ F = 1.6 \times 10^{-19} \cdot 1.196 \times 10^{6} \approx 1.914 \times 10^{-13} \, \text{N} \].
05

Calculate the Electron's Acceleration

The acceleration \( a \) can be found using Newton's second law: \( F = ma \). Hence, \( a = \frac{F}{m} \). Substitute \( F \) from Step 4 and \( m = 9.11 \times 10^{-31} \, \text{kg} \): \[ a = \frac{1.914 \times 10^{-13}}{9.11 \times 10^{-31}} \approx 2.10 \times 10^{17} \, \text{m/s}^2 \].

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Key Concepts

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

Linear Charge Density
Linear charge density, denoted by the symbol \( \lambda \), is a crucial concept when dealing with electrically charged rods. It represents the amount of electric charge per unit length along a rod or wire. In our problem, we've been given a linear charge density of \( 6.0 \, \mu \text{C/m} \), which means that for every meter of the rod's length, there is a charge of \( 6.0 \, \mu \text{C} \).

Understanding linear charge density helps us calculate the electric field generated by the charged rod. An electric field is a field around a charged object where a force would be exerted on other charges entering the field. The linear charge density is essential because it affects the strength and distribution of this electric field around the rod.
  • High linear charge density means a stronger electric field.
  • Low linear charge density means a weaker electric field.
This relationship is important because it ultimately influences how other charges, such as electrons, will move in the vicinity of the charged rod.
Electron Acceleration
Acceleration occurs when a force acts on an object and changes its velocity. In our problem, we are concerned with an electron's initial acceleration when subjected to an electric field generated by a long charged rod.

Acceleration can be calculated using Newton's Second Law, where the force applied to an object divides by the object's mass. For an electron, acceleration is crucial because it defines how quickly its velocity changes. In this scenario, the force is exerted by the electric field, calculated previously, acting on the negative charge of the electron.
  • Mass of electron: \( 9.11 \times 10^{-31} \, \text{kg} \)
  • Charge of electron: \( -1.6 \times 10^{-19} \, \text{C} \)
The magnitude of an electron's acceleration is ultimately determined by the force exerted upon it divided by its mass, resulting in a substantial acceleration due to its minimal mass.
Newton's Second Law
Newton's Second Law of Motion is a fundamental principle describing how a force applied to an object leads to an acceleration based on the formula \( F = ma \). This formula illustrates how the force \( F \) and mass \( m \) determine the acceleration \( a \) an object experiences.

This law is pivotal in our problem as it helps calculate the electron's acceleration. We know:
  • Force \( F \) involved is the electric force acting on the electron.
  • Mass \( m \) of the electron is \( 9.11 \times 10^{-31} \, \text{kg} \).
By rearranging Newton's Second Law to solve for acceleration: \( a = \frac{F}{m} \), we use the calculated electric force acting on the electron to find its acceleration. This approach defines how forces affect motion and is crucial for understanding physical dynamics.
Electric Force
The electric force is an essential concept in electromagnetism describing the force exerted by an electric field on a charged particle. In this exercise, the electric force acts on an electron released near a charged rod.

The magnitude of this force is calculated using the formula \( F = eE \), where:
  • \( F \) represents the force.
  • \( e \) is the charge of the electron \(-1.6 \times 10^{-19} \, \text{C} \).
  • \( E \) is the electric field strength at the given point.
The electric force is directly proportional to the electric field and the amount of charge. This relationship is what moves the electron and causes it to accelerate. Recognizing the influence of electric forces explains how charged particles interact within electric fields, fundamental to the principles of physics and electromagnetism.

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Most popular questions from this chapter

co A long, straight wire has fixed negative charge with a linear charge density of magnitude \(3.6 \mathrm{nC} / \mathrm{m} .\) The wire is to be enclosed by a coaxial, thin-walled nonconducting cylindrical shell of radius \(1.5 \mathrm{~cm} .\) The shell is to have positive charge on its outside surface with a surface charge density \(\sigma\) that makes the net external electric field zero. Calculate \(\sigma .\)

SSM The electric field in a certain region of Earth's atmosphere is directed vertically down. At an altitude of \(300 \mathrm{~m}\) the field has magnitude \(60.0 \mathrm{~N} / \mathrm{C} ;\) at an altitude of \(200 \mathrm{~m}\), the magnitude is \(100 \mathrm{~N} / \mathrm{C}\). Find the net amount of charge contained in a cube \(100 \mathrm{~m}\) on edge, with horizontal faces at altitudes of 200 and \(300 \mathrm{~m}\).

Charge of uniform volume density \(\rho=1.2 \mathrm{nC} / \mathrm{m}^{3}\) fills an infinite slab between \(x=-5.0 \mathrm{~cm}\) and \(x=+5.0 \mathrm{~cm}\). What is the magnitude of the electric field at any point with the coordinate (a) \(x=\) \(4.0 \mathrm{~cm}\) and (b) \(x=6.0 \mathrm{~cm} ?\)

Equation 23-11 \(\left(E=\sigma / \varepsilon_{0}\right)\) gives the electric field at points near a charged conducting surface. Apply this equation to a conducting sphere of radius \(r\) and charge \(q\), and show that the electric field outside the sphere is the same as the field of a charged particle located at the center of the sphere.

A uniform surface charge of density \(8.0 \mathrm{nC} / \mathrm{m}^{2}\) is distributed over the entire \(x y\) plane. What is the electric flux through a spherical Gaussian surface centered on the origin and having a radius of \(5.0 \mathrm{~cm}\) ?

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