Chapter 20: Problem 4
(a) Explain the two sources of magnetic moments for electrons. (b) Do all electrons have a net magnetic moment? Why or why not? (c) Do all atoms have a net magnetic moment? Why or why not?
Chapter 20: Problem 4
(a) Explain the two sources of magnetic moments for electrons. (b) Do all electrons have a net magnetic moment? Why or why not? (c) Do all atoms have a net magnetic moment? Why or why not?
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Get started for freeBriefly describe the phenomenon of magnetic hysteresis and why it occurs for ferro- and ferrimagnetic materials.
The following data are for a plain carbon steel alloy: \begin{tabular}{cccc} \hline \(\boldsymbol{H}(\boldsymbol{A} / \mathrm{m})\) & \(\boldsymbol{B}(\) tesla \()\) & \(\boldsymbol{H} \mathbf{( A / m )}\) & \(\boldsymbol{B}\) (tesla) \\ \hline 0 & 0 & 80 & \(0.90\) \\ \hline 15 & \(0.007\) & 100 & \(1.14\) \\ \hline 30 & \(0.033\) & 150 & \(1.34\) \\ \hline 50 & \(0.10\) & 200 & \(1.41\) \\ \hline 60 & \(0.30\) & 300 & \(1.48\) \\ \hline 70 & \(0.63\) & & \\ \hline \end{tabular} (a) Construct a graph of \(B\) versus \(H\). (b) What are the values of the initial permeability and initial relative permeability? (c) What is the value of the maximum permeability? (d) At about what \(H\) field does this maximum permeability occur? (e) To what magnetic susceptibility does this maximum permeability correspond?
The magnetic flux density within a bar of some material is \(0.630\) tesla at an \(H\) field of \(5 \times 10^{5} \mathrm{~A} / \mathrm{m}\). Compute the following for this material: (a) the magnetic permeability and (b) the magnetic susceptibility. (c) What type(s) of magnetism would you suggest is (are) being displayed by this material? Why?
Assume there exists some hypothetical metal that exhibits ferromagnetic behavior and that has (1) a simple cubic crystal structure (Figure 3.3), (2) an atomic radius of \(0.125 \mathrm{~nm}\), and (3) a saturation flux density of \(0.85\) tesla. Determine the number of Bohr magnetons per atom for this material
Cite the primary limitation of the new superconducting materials that have relatively high critical temperatures.
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