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Which type of magnetic material cannot be used to make permanent magnets, a ferromagnetic substance, an anti-ferromagnetic substance, or a ferrimagnetic substance?

Short Answer

Expert verified
An anti-ferromagnetic substance cannot be used to make permanent magnets because its magnetic domains have opposite directions resulting in a net magnetization of zero.

Step by step solution

01

Ferromagnetic Substance

Ferromagnetic substances are materials that have a strong magnetism and can be easily magnetized. They exhibit strong magnetic properties due to the alignment of their magnetic domains in the presence of an external magnetic field. Some examples of ferromagnetic substances are iron, cobalt, and nickel. These materials can be used to make permanent magnets.
02

Anti-ferromagnetic Substance

Anti-ferromagnetic substances are materials that have magnetic domains, but the direction of the magnetization in each domain is opposite to that of the neighboring domains, resulting in the overall magnetization being zero. This cancellation of magnetic properties occurs due to the opposing alignment of magnetic moments. Some examples of anti-ferromagnetic substances are manganese oxide and chromium. These materials cannot be used to make permanent magnets as the net magnetization is zero.
03

Ferrimagnetic Substance

Ferrimagnetic substances are materials that exhibit magnetic properties similar to ferromagnetic substances but have a partial cancellation of their magnetic moments. The magnetization in the magnetic domains is not completely canceled out due to unequal magnetic moments, resulting in a net magnetic moment. Some examples of ferrimagnetic substances are magnetite and ferrites. These materials can also be used to make permanent magnets.
04

Conclusion

Based on the properties of the magnetic materials discussed above, an anti-ferromagnetic substance cannot be used to make permanent magnets because of the cancellation of magnetic properties, resulting in a net magnetization of zero.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Ferromagnetic Substance
Understanding ferromagnetic substances is critical for those looking to grasp the foundational principles of magnetism. These materials, such as iron, cobalt, and nickel, are renowned for their strong magnetic properties. What makes them special? It's all about the alignment of magnetic domains. Imagine each domain as a tiny magnet with a north and south pole. In ferromagnetic materials, most of these tiny 'magnets' naturally align in the same direction when exposed to a magnetic field, creating a powerful collective magnetic effect.

This alignment is not just temporary. Even when the external magnetic field is removed, these substances retain a significant amount of magnetization, a property called hysteresis. This is what makes them ideal for creating permanent magnets, commonly found in everyday devices like speakers, hard drives, and motors. Learning about ferromagnetic materials helps students visualize how magnetic force fields arise from the orderly patterns of countless tiny domains working in unison.
Anti-ferromagnetic Substance
Anti-ferromagnetic substances might seem similar to their ferromagnetic cousins at first glance because they too have magnetic domains. However, there's a twist in the tale for these materials—the neighboring magnetic moments are oriented in opposite directions. These opposing forces cancel each other out, making the overall magnetization of the substance effectively zero.

Consider this simple analogy: it's like having an equal number of people pushing on either side of a box, resulting in no movement at all. Examples such as manganese oxide and chromium illustrate this delicate balance of forces. Consequently, anti-ferromagnetic substances are not suitable for creating permanent magnets, a concept that can be somewhat counterintuitive but is crucial to understand the diverse behaviors of magnetic materials in different applications, including memory storage devices and sensors.
Ferrimagnetic Substance
Ferrimagnetic substances are intriguing because they're in between ferromagnetic and anti-ferromagnetic substances in terms of magnetic behavior. These materials, including popular examples like magnetite and ferrites, also possess domains with magnetic moments. The key difference is that the magnetic moments are not equally opposed, leading to an incomplete cancellation. This results in a net magnetic moment, although usually weaker than that of a ferromagnetic material.

To visualize, imagine a rowing team where one side is slightly stronger than the other—the boat still moves forward due to the imbalance. This is why some ferrimagnetic materials can function as permanent magnets—though less powerful—and are essential to technologies like transformers and inductors. Highlighting the properties of ferrimagnetic substances helps students appreciate the variety and complexity of magnetic interactions that serve as a backbone for modern electronic devices.
Permanent Magnets
Permanent magnets are the superheroes of the magnetic world. They provide a continuous source of magnetic field without the need for an external power source. These materials, crafted from ferromagnetic or certain ferrimagnetic substances, are 'trained' to maintain their magnetism over time. Their internal structure holds the key, locking the magnetic domains in position after magnetization. The result? A dependable magnetic field that doesn't falter.

Students finding familiarity with permanent magnets will see them at the heart of daily tools and machines: from the simple refrigerator magnet to advanced medical MRI equipment. Understanding permanent magnets not only serves to clarify the concept of magnetic memory but also ignites curiosity on how these materials impact a myriad of technological advancements. It's the exploration of permanent magnets that bridges the gap between theoretical magnetic principles and real-world practical applications.

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Most popular questions from this chapter

The square-planar complex \(\left[\mathrm{Pt}(\mathrm{en}) \mathrm{Cl}_{2}\right]\) only forms in one of two possible geometric isomers. Which isomer is not observed: cis or trans?

Indicate the coordination number and the oxidation number of the metal for each of the following complexes: (a) \(\mathrm{K}_{3}\left[\mathrm{Co}(\mathrm{CN})_{6}\right]\) (b) \(\mathrm{Na}_{2}\left[\mathrm{CdBr}_{4}\right]\) (c) \(\left[\mathrm{Pt}(\mathrm{en})_{3}\right]\left(\mathrm{ClO}_{4}\right)_{4}\) (d) \(\left[\mathrm{Co}(\mathrm{en})_{2}\left(\mathrm{C}_{2} \mathrm{O}_{4}\right)\right]^{+}\) (e) \(\mathrm{NH}_{4}\left[\mathrm{Cr}\left(\mathrm{NH}_{3}\right)_{2}(\mathrm{NCS})_{4}\right]\) (f) \(\left[\mathrm{Cu}(\mathrm{bipy})_{2} \mathrm{I}\right] \mathrm{I}\)

A palladium complex formed from a solution containing bromide ion and pyridine, \(\mathrm{C}_{5} \mathrm{H}_{5} \mathrm{N}\) (a good electron-pair donor), is found on elemental analysis to contain 37.6\(\%\) bromine, 28.3\(\%\) carbon, 6.60\(\%\) nitrogen, and 2.37\(\%\) hydrogen by mass. The compound is slightly soluble in several organic solvents; its solutions in water or alcohol do not conduct electricity. It is found experimentally to have a zero dipole moment. Write the chemical formula, and indicate its probable structure.

In 2001 , chemists at SUNY-Stony Brook succeeded in synthesizing the complex trans-\(\left[\mathrm{Fe}(\mathrm{CN})_{4}(\mathrm{CO})_{2}\right]^{2-}\), which could be a model of complexes that may have played a role in the origin of life. (a) Sketch the structure of the complex. (b) The complex is isolated as a sodium salt. Write the complete name of this salt. (c) What is the oxidation state of Fein this complex? How many d electrons are associated with the Fe in this complex? (d) Would you expect this complex to be high spin or low spin? Explain.

Identify each of the following coordination complexes as either diamagnetic or paramagnetic: (a) \(\left[\mathrm{Ag}\left(\mathrm{NH}_{3}\right)_{2}\right]^{+}\) (b) square planar \(\left[\mathrm{Cu}\left(\mathrm{NH}_{3}\right)_{4}\right]^{2+}\) (c) \(\left[\mathrm{Ru}(\mathrm{bipy})_{3}\right]^{2+}\) (d) \(\left[\mathrm{CoCl}_{4}\right]^{2-}\)

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