Cite the differences between hard and soft magnetic materials in terms of both hysteresis behavior and typical applications.

Short Answer

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Answer: The primary differences between hard and soft magnetic materials in terms of hysteresis behavior are the size of their hysteresis loops and their coercivity and remanence. Hard magnetic materials have large hysteresis loops, high coercivity, and high remanence, while soft materials have small hysteresis loops, low coercivity, and low remanence. In terms of applications, hard magnetic materials are used in situations requiring strong and stable magnetic fields like permanent magnets, magnetic data storage, and sensors and actuators. On the other hand, soft magnetic materials are commonly used in applications requiring rapid and efficient switching of magnetic fields or minimized energy losses, such as transformers, inductors, and electromagnetic shielding.

Step by step solution

01

Define Hard and Soft Magnetic Materials

Hard magnetic materials are materials that have high coercivity and high remanence, meaning that they require a substantial amount of magnetic field strength to change their magnetization, and they retain their magnetization well once the magnetic field is removed. Examples of hard magnetic materials include alnico and NdFeB (Neodymium-Iron-Boron) magnets. Soft magnetic materials have low coercivity and low remanence, meaning that they can be magnetized and demagnetized easily with relatively low magnetic field strength, but they do not retain their magnetization well once the magnetic field is removed. Examples of soft magnetic materials include iron, silicon steel, and permalloy.
02

Compare Hysteresis Behaviors

The primary difference between hard and soft magnetic materials, in terms of hysteresis behavior, is the size of their hysteresis loops. A hysteresis loop represents the relationship between a material's magnetization and the applied magnetic field strength. Hard magnetic materials have a large hysteresis loop, which means that they require a large amount of energy to change their magnetization and they retain their magnetization well once the magnetic field is removed. The large hysteresis loop indicates that hard magnetic materials have high coercivity and high remanence. Soft magnetic materials have a small hysteresis loop, meaning that they require little energy to change their magnetization and they do not retain their magnetization well once the magnetic field is removed. The small hysteresis loop shows that soft magnetic materials have low coercivity and low remanence.
03

Discuss Typical Applications for Hard and Soft Magnetic Materials

Hard magnetic materials are commonly used in applications that require strong and stable magnetic fields. Some examples of these applications include: 1. Permanent magnets: Hard magnetic materials are used in permanent magnets due to their high coercivity and high remanence, which allow them to maintain a strong magnetic field even in the absence of an applied external magnetic field. 2. Magnetic data storage: Hard magnetic materials, such as in hard disk drives, utilize their high coercivity to store data in the form of magnetized regions on the disk. 3. Sensors and actuators: The strong and stable magnetic fields produced by hard magnetic materials make them suitable for use in sensors and actuators, such as in automotive and industrial applications. Soft magnetic materials are typically used in applications that require rapid and efficient switching of magnetic fields, or where energy losses need to be minimized. Some examples of these applications include: 1. Transformers: Soft magnetic materials are used in the cores of transformers due to their ability to easily magnetize and demagnetize, minimizing energy losses during the transfer of energy between the primary and secondary coils. 2. Inductors: Soft magnetic materials are used as cores in inductors, where their low coercivity allows for efficient storage and release of energy in the form of a magnetic field. 3. Electromagnetic shielding: Soft magnetic materials can effectively shield electronic components from external magnetic fields due to their high magnetic permeability, which causes them to readily absorb and dissipate the energy of the incoming field.

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Most popular questions from this chapter

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 \(1.0 \mathrm{~A}\) ?

The formula for samarium iron garnet \(\left(\mathrm{Sm}_{3} \mathrm{Fe}_{5} \mathrm{O}_{12}\right)\) may be written in the form \(\mathrm{Sm}_{3}^{c} \mathrm{Fe}_{2}^{a} \mathrm{Fe}_{3}^{d} \mathrm{O}_{12}\), where the superscripts \(a, c\), and \(d\) represent different sites on which the \(\mathrm{Sm}^{3+}\) and \(\mathrm{Fe}^{3+}\) ions are located. The spin magnetic moments for the \(\mathrm{Sm}^{3+}\) and \(\mathrm{Fe}^{3+}\) ions positioned in the \(a\) and \(c\) sites are oriented parallel to one another and antiparallel to the \(\mathrm{Fe}^{3+}\) ions in \(d\) sites. Compute the number of Bohr magnetons associated with each \(\mathrm{Sm}^{3+}\) ion, given the following information: (1) each unit cell consists of eight formula \(\left(\mathrm{Sm}_{3} \mathrm{Fe}_{5} \mathrm{O}_{12}\right)\) units; (2) the unit cell is cubic with an edge length of \(1.2529 \mathrm{~nm} ;\) (3) the saturation magnetization for this material is \(1.35 \times 10^{5} \mathrm{~A} / \mathrm{m} ;\) and (4) there are 5 Bohr magnetons associated with each \(\mathrm{Fe}^{3+}\) ion.

The magnetization within a bar of some metal alloy is \(1.2 \times 10^{6} \mathrm{~A} / \mathrm{m}\) at an \(H\) field of \(200 \mathrm{~A} / \mathrm{m}\). Compute the following: (a) the magnetic susceptibility, (b) the permeability, and (c) the magnetic flux density within this material. (d) What type(s) of magnetism would you suggest is (are) being displayed by this material? Why?

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.

It is possible to express the magnetic susceptibility \(\chi_{m}\) in several different units. For the discussion in this chapter, \(\chi_{m}\) is 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 \(H\); similarly, the atomic susceptibility \(\chi_{m}\) (a) gives the magnetization per kilogram-mole. The last two quantities are related to \(\chi_{m}\) through the following relationships: $$ \begin{aligned} &\chi_{m}=\chi_{m}(\mathrm{~kg}) \times \text { mass density }\left(\text { in } \mathrm{kg} / \mathrm{m}^{3}\right) \\ &\chi_{m}(a)=\chi_{m}(\mathrm{~kg}) \times \text { atomic weight }(\text { in } \mathrm{kg}) \end{aligned} $$ When using the cgs-emu system, comparable parameters exist that may be designated by \(\chi_{m}^{\prime}\), \(\chi_{m}^{\prime}(\mathrm{g})\), and \(\chi_{m}^{\prime}(a) ;\) the \(\chi_{m}\) and \(\chi_{m}^{\prime}\) are related in accordance with Table 20.1. From Table 20.2, \(\chi_{m}\) for copper is \(-0.96 \times 10^{-5}\); convert this value into the other five susceptibilities.

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