Chapter 7: Problem 3
Two semi-infinite filaments on the \(z\) axis lie in the regions \(-\infty
Short Answer
Step by step solution
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Chapter 7: Problem 3
Two semi-infinite filaments on the \(z\) axis lie in the regions \(-\infty
These are the key concepts you need to understand to accurately answer the question.
All the tools & learning materials you need for study success - in one app.
Get started for freeA current sheet \(\mathbf{K}=8 \mathbf{a}_{x} \mathrm{~A} / \mathrm{m}\) flows
in the region \(-2
Infinitely long filamentary conductors are located in the \(y=0\) plane at \(x=n\) meters where \(n=0, \pm 1, \pm 2, \ldots\) Each carries \(1 \mathrm{~A}\) in the \(\mathbf{a}_{z}\) direction. (a) Find \(\mathbf{H}\) on the \(y\) axis. As a help, $$\sum_{n=1}^{\infty} \frac{y}{y^{2}+n^{2}}=\frac{\pi}{2}-\frac{1}{2 y}+\frac{\pi}{e^{2 \pi y}-1}$$ (b) Compare your result of part \((a)\) to that obtained if the filaments are replaced by a current sheet in the \(y=0\) plane that carries surface current density \(\mathbf{K}=1 \mathbf{a}_{z} \mathrm{~A} / \mathrm{m}\).
A solid cylinder of radius \(a\) and length \(L\), where \(L \gg a\), contains volume charge of uniform density \(\rho_{0} \mathrm{C} / \mathrm{m}^{3}\). The cylinder rotates about its axis (the \(z\) axis) at angular velocity \(\Omega \mathrm{rad} / \mathrm{s}\). (a) Determine the current density \(\mathbf{J}\) as a function of position within the rotating cylinder. (b) Determine \(\mathbf{H}\) on-axis by applying the results of Problem 7.6. ( \(c\) ) Determine the magnetic field intensity \(\mathbf{H}\) inside and outside. \((d)\) Check your result of part ( \(c\) ) by taking the curl of \(\mathbf{H}\).
Consider a sphere of radius \(r=4\) centered at \((0,0,3)\). Let \(S_{1}\) be that portion of the spherical surface that lies above the \(x y\) plane. Find \(\int_{S_{1}}(\nabla \times \mathbf{H}) \cdot d \mathbf{S}\) if \(\mathbf{H}=3 \rho \mathbf{a}_{\phi}\) in cylindrical coordinates.
A long, straight, nonmagnetic conductor of \(0.2 \mathrm{~mm}\) radius carries a uniformly distributed current of 2 A dc. \((a)\) Find \(J\) within the conductor. (b) Use Ampère's circuital law to find \(\mathbf{H}\) and \(\mathbf{B}\) within the conductor. (c) Show that \(\nabla \times \mathbf{H}=\mathbf{J}\) within the conductor. \((d)\) Find \(\mathbf{H}\) and \(\mathbf{B}\) outside the conductor. \((e)\) Show that \(\nabla \times \mathbf{H}=\mathbf{J}\) outside the conductor.
What do you think about this solution?
We value your feedback to improve our textbook solutions.