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Which of the following characteristie is not associated with a ferromagnetic material? [Kerala CET 2008] (a) It is strongly attracted by a magnet (b) It tends to move from a region of strong magnetic ficld to a region of weak magnetic ficld (c) Its origin is the spin of clectrons (d) Above the curie temperature, it exhibits paramagnetic properties

Short Answer

Expert verified
Option (b) is not associated with ferromagnetic materials.

Step by step solution

01

Understand Ferromagnetic Properties

Ferromagnetic materials are substances that exhibit strong magnetic properties. They are characterized by their ability to be strongly attracted by magnets and can be magnetized to become permanent magnets. This is due to the alignment of magnetic domains within the material.
02

Review Each Option

Assess each option's relationship with ferromagnetic properties: - (a) Ferromagnetic materials are indeed strongly attracted by magnets. This is a defining characteristic. - (b) Ferromagnetic materials do not typically move from strong to weak magnetic fields; they are drawn to strong magnetic fields, not the opposite. - (c) The origin of ferromagnetic properties is linked to electron spin, which aligns to form domains that exhibit strong magnetism. - (d) Above the Curie temperature, ferromagnetic materials lose their ferromagnetic properties and behave as paramagnetic materials.
03

Identify the Incorrect Characteristic

Based on typical behaviors: Ferromagnetic materials do not exhibit a tendency to move from regions of strong magnetic fields to weaker ones (Option b). Instead, they are attracted to areas of higher magnetic field strength to enhance domain alignment.

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Key Concepts

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

Magnetic Properties
Magnetic properties refer to how a material responds to a magnetic field. For ferromagnetic materials, this involves a very strong attraction to magnets. These materials have the unique capability to become permanent magnets themselves when exposed to a magnetic field. This occurs because the internal magnetic domains within the material can be aligned. The intense magnetic attraction is primarily due to the alignment of these domains in the same direction. Once aligned, the domains act collectively, enhancing the overall magnetic field of the material. Ferromagnetism is a fascinating phenomenon and is different from paramagnetism or diamagnetism. While paramagnetic materials are weakly attracted to magnets and diamagnetic materials are weakly repelled, ferromagnetic materials show a very strong attraction, making them distinct in the realm of magnetism.
Curie Temperature
Curie temperature is a critical point for ferromagnetic materials. It is the temperature above which these materials lose their permanent magnetic properties and become paramagnetic. At the Curie temperature, the thermal energy is sufficient to disrupt the alignment of the magnetic domains that had been formed. In a ferromagnetic material, at temperatures below the Curie point, the domains are aligned. This allows the material to retain magnetism even in the absence of an external magnetic field. However, as the temperature increases to the Curie point, the thermal agitation overcomes the forces aligning the domains. Consequently, the material can no longer maintain its magnetization. Understanding the Curie temperature is crucial for using ferromagnetic materials effectively, especially in applications that involve varying temperatures.
Electron Spin
Electron spin is a fundamental property linked to ferromagnetism. It is one of the intrinsic forms of angular momentum carried by electrons. Each electron has a spin, which can be thought of as either "up" or "down." In ferromagnetic materials, the majority of electron spins align in the same direction, contributing to a strong overall magnetic effect. This alignment happens because electrons tend to pair up in such a way that their spins produce the maximum possible magnetic moment. The aligned spins create a strong cumulative magnetic field in specific regions called domains. The concept of electron spin is central to the understanding of both how these domains form and why ferromagnetic materials display such strong magnetic properties. Thus, the manipulation of electron spins underlies the operation of many devices, from traditional magnets to modern advanced technologies like spintronics.
Magnetic Domains
Magnetic domains are small, localized areas within a ferromagnetic material where the magnetic moments of atoms are aligned in the same direction. These domains are like tiny magnets within the material and can align or misalign based on external magnetic fields or temperatures. In the unmagnetized state, these domains are randomly oriented, creating no net magnetic field outside the material. However, when exposed to a magnetic field, the domains can grow and reorient in the direction of the applied field, strengthening the material's magnetism. Understanding the behavior of magnetic domains is essential for explaining ferromagnetism. It helps us grasp why ferromagnetic materials can be permanently magnetized. Moreover, the concept of domains is crucial in the development of magnetic storage technologies and other magnetic-based applications.

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Most popular questions from this chapter

In a vibration magnetometer, the time period of a bar magnet oscillating in horizontal component of earth's magnetic field is \(2 \mathrm{~s}\). When a magnet is brought near and parallel to it, the time period reduces to 18 . The ratio \(F / H\) of the fields, \(F\) due to magnet and \(H\), the horizontal component will be (a) \(\sqrt{3}\) (b) \(\frac{1}{\sqrt{3}}\) (c) \(\frac{1}{3}\) (d) 3

In a permanent magnet at room temperature [NCERT Exemplar] (a) magnetic moment of each molecule is zero (b) the individual molecules have non-zero magnetic moment which are all perfectly aligned (c) domains are partially aligned (d) domains are all perfectly aligned

A tangent galvanometer is used for detection and measurement of low electric currents. It is based on tangent law in magnetism, according to which \(F=G \tan \theta\), where \(\theta\) is angle with \(H\) made by a magnet suspended freely under the combined effect of \(H\) and \((F \perp H) .\) Now, \(F=\frac{\mu_{0}}{4 \pi} \frac{2 \pi n I}{r}\), where \(n\) is number of turns in the coil of radius, \(r\) earrying current \(I\). From, \(F=H \tan \theta\), we get $$ I=\frac{2 r H}{\mu_{0} n} \tan \theta=K \tan \theta $$ where \(K\) is called reduction factor of tangent galvanometer. In the use of tangent galvanometer, \(H\) is (a) earth's magnetic ficld (b) horizontal component of earth's magnetic field (c) vertical component of earth's magnetic ficld (d) None of the above

At a certain place, a magnet makes 30 oscillations per min. At another place where the magnetic field is double, its time period will be [a) \(4 \mathrm{~s}\) (b) \(2 s\) (c) \(1 / 2 s\) (d) \(\sqrt{2} \mathrm{~s}\)

A vibration magnetometer consists of two identical bar magnets placed one over the other such that they are perpendicular and bisect each other. The time period of oscillation in a horizontal magnetic field is \(2^{5 / 4}\) s. One of the magnets is removed and if the other magnet oscillates in the same field, then the time period in second is (a) \(2^{1 / 4}\) (b) \(2^{10}\) (c) 2 (d) 4

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