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The magnetism of magnet is due to (a) The spin motion of electron (b) Earth (c) Pressure inside the earth core region (d) Cosmic rays

Short Answer

Expert verified
The magnetism of a magnet is primarily due to the alignment and movement of electrons within the atoms of the material, particularly their spin motion. Therefore, the correct answer is (a) The spin motion of electron.

Step by step solution

01

Recall the basics of magnetism

Magnetism is a force that can attract or repel other magnetic materials. It is due to the movement and alignment of electrons within the atoms of the material.
02

Analyze each option

(a) The spin motion of electron: The magnetism in a material is due to the alignment and movement of electrons within the atoms of the material. In particular, the spin motion of electrons contributes to the magnetic properties of materials. (b) Earth: Earth itself acts as a giant magnet due to the motion of molten iron in its core, creating a magnetic field. However, the magnetism in magnets is not directly due to the Earth. (c) Pressure inside the earth core region: This option is not directly related to the magnetism of magnets. The pressure inside the Earth's core can influence the magnetic properties of Earth, but it does not cause magnetism in individual magnets. (d) Cosmic rays: Cosmic rays are high-energy particles from outer space, which interact with Earth's atmosphere and can have various effects on Earth and its magnetic field. However, they are not responsible for the magnetism in magnets.
03

Identify the correct option

Based on the analysis of each option, the correct answer is (a) The spin motion of electron. The magnetism of a magnet is primarily due to the alignment and movement of electrons within the atoms of the material, particularly their spin motion.

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Key Concepts

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

Electron Spin
Electron spin is a fundamental concept in magnetism. Spin is a property of electrons that can be thought of as something similar to spinning on an axis, like a tiny top. Although we cannot directly see this spin, it plays a crucial role in an atom's behavior.

Electrons are like tiny magnets because of their spin. Each electron has a magnetic moment or a small magnetic field of its own. This is a result of the electron spinning, creating what scientists refer to as magnetic dipoles. These dipoles can align in certain conditions to cause larger magnetic effects.
  • Think of electron spins like tiny bar magnets.
  • They can either pair up, canceling their magnetic fields, or align in the same direction to enhance the magnetic effect.
The reason magnets are effective is that many electron spins in a material align in the same direction, causing the material to become magnetized. Electron spins are fundamental to why magnets attract or repel one another.
Without electron spin, much of what we consider magnetism would not exist.
Magnetic Properties
Magnetic properties are characteristics that define how materials respond to magnetic fields. These properties depend heavily on the structure and behavior of electrons within the material.

The key magnetic properties include:
  • Ferromagnetism: Materials that can form permanent magnets or are attracted to magnets, like iron.
  • Paramagnetism: Materials that are weakly attracted to magnetic fields and do not retain magnetic properties once the external field is removed.
  • Diamagnetism: Materials that create an opposing magnetic field in response to an external magnetic field and are weakly repelled.
These properties arise mainly because of how electrons are organized and behave in materials. In ferromagnetic materials, electron spins are aligned over large regions called domains. When these domains are aligned, the material exhibits strong magnetic properties.

In a nutshell, understanding magnetic properties help us know why some materials become magnets and how they interact with magnetic fields. Their behavior is crucial for applications in technology, such as in hard disks and MRI machines.
Alignment of Electrons
The alignment of electrons is what makes materials magnetic. In any given material, electrons can have different alignments which directly impact its magnetic behavior.

Imagine having a group of tiny bumper cars, each with a small directional arrow. If these arrows all point in random directions, the overall impact is none. But, if most arrows point the same way, the group moves seamlessly in that direction, demonstrating collective behavior.
  • In magnets, electron spins are predominantly aligned in the same direction.
  • This uniform alignment strengthens the material's overall magnetic field and effect.
Materials capable of maintaining aligned electron spins create what we know as permanent magnets. This is due to the unique arrangement of electrons and the interactions within their atomic structure.

For students, grasping electron alignment is key to understanding how magnetic fields form and why some materials have stronger magnetic properties than others.

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Most popular questions from this chapter

A long wire carr1es a steady current. It is bent into a circle of one turn and the magnetic field at the centre of the coil is \(\mathrm{B}\). It is then bent into a circular Loop of n turns. The magnetic field at the centre of the coil for same current will be. (a) \(\mathrm{nB}\) (b) \(\mathrm{n}^{2} \mathrm{~B}\) (c) \(2 \mathrm{nB}\) (d) \(2 \mathrm{n}^{2} \mathrm{~B}\)

A magnet of magnetic moment \(50 \uparrow \mathrm{A} \mathrm{m}^{2}\) is placed along the \(\mathrm{X}\) -axis in a mag. field \(\mathrm{B}^{-}=(0.5 \uparrow+3.0 \mathrm{~J} \wedge\) ) Tesla. The torque acting on the magnet is N.m. (c) \(75 \mathrm{k} \wedge\) (d) \(25 \sqrt{5} \mathrm{k} \wedge\) (a) \(175 \mathrm{k}\) (b) \(150 \mathrm{k}\)

A Galvanometer has a resistance \(\mathrm{G}\) and \(\mathrm{Q}\) current \(\mathrm{I}_{\mathrm{G}}\) flowing in it produces full scale deflection. \(\mathrm{S}_{1}\) is the value of the shunt which converts it into an ammeter of range 0 to \(\mathrm{I}\) and \(\mathrm{S}_{2}\) is the value of the shunt for the range 0 to \(2 \mathrm{I}\). The ratio \(\left(\mathrm{S}_{1} / \mathrm{S}_{2}\right) \mathrm{is}\) (a) \(\left[\left(2 \mathrm{I}-\mathrm{I}_{\mathrm{G}}\right) /\left(\mathrm{I}-\mathrm{I}_{\mathrm{G}}\right)\right]\) (b) \((1 / 2)\left[\left(\mathrm{I}-\mathrm{I}_{\mathrm{G}}\right) /\left(2 \mathrm{I}-\mathrm{I}_{\mathrm{G}}\right)\right]\) (c) 2 (d) 1

A current of a \(1 \mathrm{Amp}\) is passed through a straight wire of length 2 meter. The magnetic field at a point in air at a distance of 3 meters from either end of wire and lying on the axis of wire will be (a) \(\left(\mu_{0} / 2 \pi\right)\) (b) \(\left(\mu_{0} / 4 \pi\right)\) (c) \(\left(\mu_{0} / 8 \pi\right)\) (d) zero

A dip needle lies initially in the magnetic meridian when it shows an angle of dip at a place. The dip circle is rotted through an angle \(\mathrm{x}\) in the horizontal plane and then it shows an angle of dip \(\theta^{\prime}\). Then \(\left[\left(\tan \theta^{\prime}\right) /(\tan \theta)\right]\) is (a) \([1 /(\cos x)]\) (b) \([1 /(\sin x)]\) (c) \([1 /(\tan \mathrm{x})]\) (d) \(\cos \mathrm{x}\)

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