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A charge of \(6.00 \mathrm{pC}\) is spread uniformly throughout the volume of a sphere of radius \(r=4.00 \mathrm{~cm}\). What is the magnitude of the electric field at a radial distance of (a) \(6.00 \mathrm{~cm}\) and (b) \(3.00 \mathrm{~cm}\) ?

Short Answer

Expert verified
At 6.00 cm, the electric field is 1499 N/C; at 3.00 cm, it is 1011 N/C.

Step by step solution

01

Understand the Problem

There is a uniformly charged sphere with a total charge of \(6.00 \mathrm{pC}\) and radius \(4.00 \mathrm{cm}\). We need to find the electric field magnitude at two points: (a) outside the sphere at \(6.00 \mathrm{cm}\) and (b) inside the sphere at \(3.00 \mathrm{cm}\). We will apply Gauss's law to solve this.
02

Calculate Electric Field outside the Sphere

According to Gauss's law, the electric field at a distance \(r\) from a point charge is \(E = \frac{kQ}{r^2}\), where \(k = 8.99 \times 10^9 \mathrm{~N~m^2/C^2}\) is the Coulomb's constant, \(Q\) is the charge, and \(r\) is the radial distance. At \(r = 6.00 \mathrm{~cm}\), we use the entire charge in the sphere:\[E_{6~cm} = \frac{8.99 \times 10^9 \mathrm{~N~m^2/C^2} \times 6.00 \times 10^{-12} \mathrm{C}}{(0.06 \mathrm{~m})^2} = 1499 \mathrm{~N/C}\]
03

Use Gauss's Law Inside the Sphere

Inside a uniformly charged sphere, the electric field is given by the formula \(E = \frac{kQr}{R^3}\), where \(Q\) is the total charge, \(r\) is the radial distance from the center within the sphere, and \(R\) is the sphere’s radius. At \(r = 3.00 \mathrm{~cm}\),\[E_{3~cm} = \frac{8.99 \times 10^9 \mathrm{~N~m^2/C^2} \times 6.00 \times 10^{-12} \mathrm{C} \times 0.03 \mathrm{~m}}{(0.04 \mathrm{~m})^3} = 1011 \mathrm{~N/C}\]

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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 powerful tool in electrostatics that relates electric flux to charge. It states that the total electric flux through a closed surface is equal to the charge enclosed divided by the permittivity of free space. This law is expressed mathematically as \[\Phi_E = \oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{enc}}{\varepsilon_0}\]where \(\Phi_E\) is the electric flux, \(\mathbf{E}\) is the electric field vector, \(d\mathbf{A}\) is a differential area on the closed surface, \(Q_{enc}\) is the enclosed charge, and \(\varepsilon_0\) is the permittivity of free space.
  • This law simplifies the calculation of electric fields, especially for symmetric charge distributions.
  • It becomes extremely useful for objects like spheres, cylinders, and planes where the symmetrical setup makes the flux calculation straightforward.
Understanding Gauss's Law helps to analyze the electric field both inside and outside charged bodies.
Coulomb's Law
Coulomb's Law describes the interaction between two point charges. It tells us that the electric force \(F\) between two charges \(Q_1\) and \(Q_2\) is directly proportional to the product of the charges and inversely proportional to the square of the distance \(r\) between them:\[F = k \frac{|Q_1Q_2|}{r^2}\]where \(k\) is Coulomb's constant, valued at approximately \(8.99 \times 10^9 \, \text{N m}^2/\text{C}^2\).
  • This law forms the foundation of electrostatics, similar to how Newton's law of gravitation governs gravitational interactions.
  • It helps explain how charge distributions such as a sphere impact the surrounding space, impacting the electric field.
Coulomb's Law, in conjunction with Gauss's Law, allows us to compute and understand electric fields due to various charge configurations.
Uniform Charge Distribution
Uniform charge distribution indicates that charge is spread evenly over a certain volume, surface, or length. For a sphere, this means each small segment of the sphere’s volume contains the same amount of charge per cubic centimeter.
  • In a uniform distribution, the charge density \(\rho\) is constant across the region of the sphere.
  • It is calculated as \(\rho = \frac{Q}{V}\), where \(Q\) is the total charge and \(V\) is the total volume of the sphere.
A uniformly charged sphere simplifies electric field calculations using Gauss’s Law, because irrespective of where you calculate inside the sphere, the impact of charge distribution remains consistent.
Sphere
A sphere, in the context of electric fields and charges, is often considered due to its symmetry, which simplifies many calculations. The symmetry means any radial line from the center to the surface is identical in terms of electrical properties.
  • The radius defines the size of the sphere and influences the volume \(V\) given by \(V = \frac{4}{3}\pi R^3\).
  • The spherical symmetry allows assumption of consistent charge density for uniform charge distribution.
Spheres are significant in physics because their geometry allows the use of Gauss's Law to determine internal and external electric fields with ease.
Radial Distance
Radial distance refers to the straight-line distance from the center of a sphere to any point either inside or outside the sphere. It plays a crucial role in calculating electric fields using both Coulomb's and Gauss's Laws.
  • Outside a uniformly charged sphere, the radial distance \(r\) is considered from the center to the point where the field is measured.
  • For points inside, the radial distance becomes crucial in defining part of the volume that influences the electric field, as only the charge within that specific radial distance affects the result.
Comprehending radial distance helps in setting up problems and understanding how enclosed charge impacts the electric field at various points.
Electric Field Inside and Outside Sphere
The electric field behaves differently inside and outside a sphere with uniform charge distribution.
  • Outside the sphere, at radial distance \(r > R\), the electric field is as if all the charge were concentrated at the center, governed by \(E = \frac{kQ}{r^2}\).
  • Inside the sphere at radial distance \(r < R\), the field increases linearly with distance from the center, described by \(E = \frac{kQr}{R^3}\).
Understanding these differences aids in applying Gauss's Law appropriately, and reveals intriguing features of electrostatic fields around symmetric charge distributions.

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Most popular questions from this chapter

A uniform charge density of \(500 \mathrm{nC} / \mathrm{m}^{3}\) is distributed throughout a spherical volume of radius \(6.00 \mathrm{~cm} .\) Consider a cubical Gaussian surface with its center at the center of the sphere. What is the electric flux through this cubical surface if its edge length is (a) \(4.00 \mathrm{~cm}\) and (b) \(14.0 \mathrm{~cm} ?\)

A point charge of \(1.8 \mu \mathrm{C}\) is at the center of a Gaussian cube 55 \(\mathrm{cm}\) on edge. What is the net electric flux through the surface?

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 point charge located at the center of the sphere.

Space vehicles traveling through Earth's radiation belts can intercept a significant number of electrons. The resulting charge buildup can damage electronic components and disrupt operations. Suppose a spherical metal satellite \(1.3 \mathrm{~m}\) in diameter accumulates \(2.4\) \(\mu \mathrm{C}\) of charge in one orbital revolution. (a) Find the resulting surface charge density. (b) Calculate the magnitude of the electric field just outside the surface of the satellite, due to the surface charge.

A charge of uniform linear density \(2.0 \mathrm{nC} / \mathrm{m}\) is distributed along a long, thin, nonconducting rod. The rod is coaxial with a long conducting cylindrical shell (inner radius \(=5.0 \mathrm{~cm}\), outer radius \(=10 \mathrm{~cm})\). The net charge on the shell is zero. (a) What is the magnitude of the electric field \(15 \mathrm{~cm}\) from the axis of the shell? What is the surface charge density on the (b) inner and (c) outer surface of the shell?

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