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Charge \(Q\) is distributed uniformly throughout the volume of an insulating sphere of radius \(R =\) 4.00 cm. At a distance of \(r =\) 8.00 cm from the center of the sphere, the electric field due to the charge distribution has magnitude \(E =\) 940 N/C. What are (a) the volume charge density for the sphere and (b) the electric field at a distance of 2.00 cm from the sphere's center?

Short Answer

Expert verified
(a) \(\rho \approx 6.26 \times 10^{-4}\, \text{C/m}^3\); (b) \(E \approx 187.19\,\text{N/C}\) at 2 cm.

Step by step solution

01

Understanding the given information

We are given:- Total charge on the sphere, \(Q\) (not directly provided, we need to find it).- Radius of the sphere, \(R = 4.00\) cm.- The electric field at a distance \(r = 8.00\) cm outside the sphere, \(E = 940\) N/C.- We need to find the volume charge density \(\rho\) and the electric field at a distance \(r = 2.00\) cm.
02

Using Gauss's Law for points outside the sphere

For a point outside a uniformly charged sphere, the sphere can be treated as a point charge. The electric field \(E\) at a distance \(r = 8.00\) cm is given by:\[E = \frac{kQ}{r^2},\]where \(k = 8.99 \times 10^9\, \text{N} \cdot \text{m}^2/\text{C}^2\) is the Coulomb's constant.Solving for \(Q\), we have:\[Q = \frac{Er^2}{k} = \frac{940 \times (0.08)^2}{8.99 \times 10^9}.\]
03

Calculate the Charge Q

Substitute the values into the equation:\[Q = \frac{940 \times 0.0064}{8.99 \times 10^9} = \frac{6.016}{8.99 \times 10^7}.\]Calculate \(Q\) to find:\[Q \approx 6.69 \times 10^{-8}\, \text{C}.\]
04

Finding the volume charge density \(\rho\)

The volume charge density \(\rho\) is uniform throughout the sphere and is given by:\[\rho = \frac{Q}{\text{Volume of sphere}}.\]The volume \(V\) of the sphere is \(\frac{4}{3}\pi R^3\), where \(R = 0.04\) m.\[\rho = \frac{6.69 \times 10^{-8}}{\frac{4}{3}\pi (0.04)^3}.\]
05

Calculate \(\rho\) and find its value

Substituting in:\[\rho = \frac{6.69 \times 10^{-8}}{\frac{4}{3} \pi \times (0.064 \times 10^{-3})} \approx \frac{6.69 \times 10^{-8}}{1.07 \times 10^{-4}}.\]This gives:\[\rho \approx 6.26 \times 10^{-4}\, \text{C/m}^3.\]
06

Calculate the electric field inside the sphere at r = 2.00 cm

Using Gauss's law inside the sphere, the electric field \(E\) at distance \(r\) is given by:\[E = \frac{kQr}{R^3}.\]Substitute \(Q\) and calculate:\[E = \frac{8.99 \times 10^9 \times 6.69 \times 10^{-8} \times 0.02}{(0.04)^3}.\]
07

Find the electric field at r = 2.00 cm

Compute the value:\[E = \frac{8.99 \times 10^9 \times 6.69 \times 10^{-8} \times 0.02}{6.4 \times 10^{-5}} = \frac{1.198 \times 10^{-2}}{6.4 \times 10^{-5}}.\]Calculate:\[E \approx 187.19\,\text{N/C}.\]

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Key Concepts

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

Volume Charge Density
Volume charge density, denoted as \( \rho \), is a measure of how much electric charge is contained within a given volume of space, such as inside a sphere. It is expressed in units of coulombs per cubic meter (C/m\(^3\)).
For a uniformly charged body, like the insulating sphere in this problem, volume charge density can be determined using the formula: - \( \rho = \frac{Q}{V} \) - where \( Q \) is the total charge and \( V \) is the volume of the sphere.The volume of a sphere is calculated using the formula: - \( V = \frac{4}{3} \pi R^3 \)- where \( R \) is the radius.In this exercise, we found that the sphere's total charge was approximately \( 6.69 \times 10^{-8} \) C. After calculating the volume using the sphere's radius, you can use it to find \( \rho \). Understanding how \( \rho \) is derived helps you comprehend how electric fields arise from distributed charges.
Gauss's Law
Gauss's Law is a key principle for understanding electric fields, particularly in symmetric situations like spheres or cylinders. It states that the electric flux through a closed surface is proportional to the charge enclosed within that surface. In mathematical form, Gauss's Law is written as:- \( \Phi_E = \frac{Q_{enclosed}}{\varepsilon_0} \)- where \( \Phi_E \) is the electric flux and \( \varepsilon_0 \) is the vacuum permittivity.For a spherical charge distribution, if a point lies outside the sphere, the sphere can be treated as if all its charge were concentrated at its center. This allows for simplifications when calculating the electric field.In this problem:- At 8 cm, the electric field was calculated using the formula \( E = \frac{kQ}{r^2} \) since the point is outside the sphere.- At 2 cm, the point is inside, and the formula \( E = \frac{kQr}{R^3} \) is used, exploiting the symmetry and linear relationship of radius inside the sphere. Gauss's Law simplifies the process of calculating electric fields, especially when dealing with symmetrical charge distributions.
Coulomb's Constant
Coulomb's constant, denoted as \( k \), plays a crucial role in the equations governing electric forces and fields. Its value is \( 8.99 \times 10^9 \) N·m\(^2\)/C\(^2\), and it appears in Coulomb's Law, which describes the force between two point charges:- \( F = k \frac{|q_1q_2|}{r^2} \)- where \( F \) is the force, \( q_1 \) and \( q_2 \) are the charges, and \( r \) is the distance between them.In this exercise, Coulomb's constant is used to express the electric field due to a charge:- \( E = \frac{kQ}{r^2} \) for a distance outside the sphere.This constant is essential for converting the relationship between electric field (E) and the charge causing it. It ensures the units work out correctly and provides a standard way of calculating electric forces and fields across various problems. By understanding how \( k \) fits into these calculations, you gain deeper insight into the nature of electric interactions and force.

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Most popular questions from this chapter

A hollow, conducting sphere with an outer radius of 0.250 m and an inner radius of 0.200 m has a uniform surface charge density of +6.37 \(\times\) 10\(^{-6}\) C/m\(^2\). A charge of -0.500 \(\mu\)C is now introduced at the center of the cavity inside the sphere. (a) What is the new charge density on the outside of the sphere? (b) Calculate the strength of the electric field just outside the sphere. (c) What is the electric flux through a spherical surface just inside the inner surface of the sphere?

A solid conducting sphere with radius \(R\) carries a positive total charge \(Q\). The sphere is surrounded by an insulating shell with inner radius \(R\) and outer radius 2\(R\). The insulating shell has a uniform charge density \(\rho\). (a) Find the value of \(\rho\) so that the net charge of the entire system is zero. (b) If \(\rho\) has the value found in part (a), find the electric field \(\overrightarrow{E}\) (magnitude and direction) in each of the regions 0 \(< r < R, R < r < 2R\), and \(r > 2R\). Graph the radial component of \(\overrightarrow{E}\) as a function of r. (c) As a general rule, the electric field is discontinuous only at locations where there is a thin sheet of charge. Explain how your results in part (b) agree with this rule.

A very large, horizontal, nonconducting sheet of charge has uniform charge per unit area \(\sigma =\) 5.00 \(\times\) 10\(^{-6}\) C/m\(^2\). (a) A small sphere of mass \(m =\) 8.00 \(\times\) 10\(^{-6}\) kg and charge \(q\) is placed 3.00 cm above the sheet of charge and then released from rest. (a) If the sphere is to remain motionless when it is released, what must be the value of \(q\)? (b) What is \(q\) if the sphere is released 1.50 cm above the sheet?

A solid conducting sphere with radius \(R\) that carries positive charge \(Q\) is concentric with a very thin insulating shell of radius \(2R\) that also carries charge \(Q\). The charge \(Q\) is distributed uniformly over the insulating shell. (a) Find the electric field (magnitude and direction) in each of the regions \(0 < r < R, R < r < 2R\), and \(r > 2R\). (b) Graph the electric-field magnitude as a function of \(r\).

An electron is released from rest at a distance of 0.300 m from a large insulating sheet of charge that has uniform surface charge density +2.90 \(\times\) 10\(^{-12}\) C/m2. (a) How much work is done on the electron by the electric field of the sheet as the electron moves from its initial position to a point 0.050 m from the sheet? (b) What is the speed of the electron when it is 0.050 m from the sheet?

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