Chapter 20: Problem 7
Compute (a) the saturation magnetization and (b) the saturation flux density for iron, which has a net magnetic moment per atom of 2.2 Bohr magnetons and a density of \(7.87 \mathrm{g} / \mathrm{cm}^{3}\).
Chapter 20: Problem 7
Compute (a) the saturation magnetization and (b) the saturation flux density for iron, which has a net magnetic moment per atom of 2.2 Bohr magnetons and a density of \(7.87 \mathrm{g} / \mathrm{cm}^{3}\).
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Get started for freeAn iron bar magnet having a coercivity of \(7000 \mathrm{A} / \mathrm{m}\) is to be demagnetized. If the bar is inserted within a cylindrical wire coil \(0.25 \mathrm{m}\) long and having 150 turns, what electric current is required to generate the necessary magnetic field?
It is possible to express the magnetic susceptibility \(\chi_{m}\) in several different units. For the discussion of this chapter, \(\chi_{m}\) was used to designate the volume susceptibility in SI units, that is, the quantity that gives the magnetization per unit volume \(\left(\mathrm{m}^{3}\right)\) of material when multiplied by \(H\). The mass susceptibility \(\chi_{m}(\mathrm{kg})\) yields the magnetic moment (or magnetization) per kilogram of material when multiplied by \(H ;\) and, similarly, the atomic susceptibility \(\chi_{m}(\text { a })\) gives the magnetization per kilogram- mole. The latter two quantities are related to \(\chi_{m}\) through the relationships $$\begin{aligned}\chi_{m} &=\chi_{m}(\mathrm{kg}) \times \text { mass density }\left(\mathrm{in} \mathrm{kg} / \mathrm{m}^{3}\right) \\\\\chi_{m}(\mathrm{a}) &=\chi_{m}(\mathrm{kg}) \times \text { atomic weight }(\mathrm{in} \mathrm{kg})\end{aligned}$$ When using the cgs-emu system, comparable parameters exist, which may be designated by \(\chi_{m}^{\prime}, \chi_{m}^{\prime}(\mathrm{g}),\) and \(\chi_{m}^{\prime}(\mathrm{a})\); the \(\chi_{m}\) and \(\chi_{m}^{\prime}\) are related in accordance with Table 20.1 From Table \(20.2, \quad \chi_{m}\) for copper is \(-0.96 \times 10^{-5} ;\) convert this value into the other five susceptibilities.
There is associated with each atom in paramagnetic and ferromagnetic materials a net magnetic moment. Explain why ferromagnetic materials can be permanently magnetized whereas paramagnetic ones cannot.
Cite the primary limitation of the new superconducting materials that have relatively high critical temperatures.
Assume there exists some hypothetical metal that exhibits ferromagnetic behavior and that has (1) a simple cubic crystal structure (Figure 3.23 ), (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.
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