Chapter 20: Problem 15
Briefly explain why the magnitude of the saturation magnetization decreases with increasing temperature for ferromagnetic materials, and why ferromagnetic behavior ceases above the Curie temperature.
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Chapter 20: Problem 15
Briefly explain why the magnitude of the saturation magnetization decreases with increasing temperature for ferromagnetic materials, and why ferromagnetic behavior ceases above the Curie temperature.
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Cite the primary limitation of the new superconducting materials that have relatively high critical temperatures.
Briefly describe the Meissner effect.
A coil of wire \(0.5 \mathrm{~m}\) long and having 20 turns carries a current of \(1.0 \mathrm{~A}\). (a) Compute the flux density if the coil is within a vacuum. (b) A bar of an iron-silicon alloy, the \(B-H\) behavior for which is shown in Figure \(20.29\), is positioned within the coil. What is the flux density within this bar? (c) Suppose that a bar of molybdenum is now situated within the coil. What current must be used to produce the same \(B\) field in the Mo as was produced in the iron-silicon alloy (part b) using \(1.0 \mathrm{~A}\) ?
A coil of wire \(0.25 \mathrm{~m}\) long and having 400 turns carries a current of \(15 \mathrm{~A}\). (a) What is the magnitude of the magnetic field strength \(H ?\) (b) Compute the flux density \(B\) if the coil is in a vacuum. (c) Compute the flux density inside a bar of chromium positioned within the coil. The susceptibility for chromium is given in Table \(20.2\). (d) Compute the magnitude of the magnetization \(M\)
A ferromagnetic material has a remanence of \(1.0\) tesla and a coercivity of \(15,000 \mathrm{~A} / \mathrm{m}\). Saturation is achieved at a magnetic field strength of \(25,000 \mathrm{~A} / \mathrm{m}\), at which the flux density is \(1.25\) teslas. Using these data, sketch the entire hysteresis curve in the range \(H=-25,000\) to \(+25,000 \mathrm{~A} / \mathrm{m}\). Be sure to scale and label both coordinate axes.
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