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HC Verma Solutions Class 12 Chapter 37 - Magnetic Properties of Matter

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Summary of HC Verma Solutions Part 2 Chapter 37: Magnetic Properties of Magnet

This chapter covers various magnetic properties. Concepts such as magnetization of materials and intensity of magnetization are discussed in detail. Furthermore, different kinds of magnetic materials such as ferromagnetism, paramagnetism, and diamagnetism are also covered. Lastly, Curie's Law, Dia-, Para-, and Ferromagnetic Substances, Hysteresis, Soft Iron, and Steel are discussed.


You can access the HC Verma Solutions for Chapter 37 - Magnetic Properties of Magnet in PDF format for free. This means that you have the flexibility to study anytime and from anywhere, ensuring that you have the necessary materials at your fingertips.


The Class 12 HC Verma Solutions Magnetic Properties of Magnet PDF provided by Vedantu is designed to support your learning journey. It is created by expert Physics teachers who possess a deep understanding of the concepts covered in the chapter. By offering solutions for all the exercises in the chapter, you have the opportunity to practice problem-solving in various contexts.


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Benefits of using Vedantu’s Class 12 HC Verma Solutions for Chapter 37 - Magnetic Properties of Magnet

  • Solutions provided by expert Physics teachers with a deep understanding of the concepts.

  • Covers all exercises in the chapter for comprehensive practice.

  • Available in a free PDF format for easy accessibility anytime, anywhere.

  • Clear and concise explanations of the solutions to the exercises.


About HC Verma Class 12 Solutions For Chapter 37 - Magnetic Properties of Matter

Magnetic forces mediate a subset of a physical phenomenon known as magnetism. The magnetism of matter is the force exerted by magnets when they attract or repulse each other. Magnetic moments and the electric currents of basic particles give rise to a magnetic field, which acts on other magnetic and currents moments. The magnetic state of a material based on pressure, temperature, and the applied magnetic field. As these variables shift, a substance can exhibit several forms of magnetism. Magnetic properties of matter can be found in various Earth materials that act as insulators and conductors of varying degrees and shapes.


Michael Faraday is the first statistician who was discovered classifying substances according to their magnetic properties in the 19th century. The strength of a magnetic field always decreases with distance, though the required mathematical relationship between strength and distance varies.


Magnetic dipoles have been recognized, although some theories predict the existence of magnetic monopoles.


Four Basic Facts About How Magnets Behave:

  • A magnet has two endpoints called poles, one is called a north pole or also called a north-seeking pole, and the other is called a south pole or also called a south-seeking pole.

  • The north pole of the first magnet attracts the south pole of a second magnet, while the north pole of the first magnet repels the second magnet's pole.

  • A magnet creates a magnetic field and is an intangible sphere of magnetism all over it.

  • The north pole of a magnet is roughly towards the Earth's north pole and vice-versa. That's because the Earth itself involves magnetic materials and behaves like a gigantic magnet.


Source of Magnetism

Magnetism is Derived from Two Sources:

  • Electric current.

  • Spin magnetic moments of elementary particles.

The magnetic properties of matter are mainly due to the magnetic moments of their atoms orbiting electrons. The magnetic moments of the nuclei of atoms are very small than the “electrons' magnetic moments, so they are negligible in the condition of the magnetization of materials.


In addition, even when the electron configuration is such that there are unpaired electrons and also non-filled subshells, it occurs frequently. In that case, the various electrons in the solid state will give the magnetic moments of that point in different, random directions so that the material will not be magnetic. Hence, the magnetic behavior of a material is based on its structure, particularly its electron configuration, and also on the temperature. Depending on whether there is an attraction or repulsion between the north pole and south pole of a magnet, the matter is classified as being either paramagnetic or diamagnetic, respectively.


Magnetic Properties of Matter

There are several magnetism properties of matters including Magnetization, Diamagnetism, Paramagnetism respectively.


Magnetization

In this section, we will learn about magnetization and the concept of magnetic intensity.

In electromagnetism, magnetization, also called magnetic polarization, is a vector field that contributes to the measure of the density of induced or permanent magnetic dipole moments in a given magnetic material. Magnetization is the magnetism of matter which was discovered by William Gilbert. The variation within this branch is described by direction and is either Axial or Diametric. As we know, magnetization results from magnetism, which results from the motion of electrons in the atoms or the spin of electrons in the atom or the nuclei.


The theory of magnetization helps us in classifying the materials based on their magnetic properties. Net magnetization is the result of the response material to an external magnetic field. The magnetization of a sample material M is called the net magnetic moment for that material per unit volume. The mathematical formula of magnetization field or M-field is,

M = mnetV


In a magnetic field, paramagnetic materials have a weak induced magnetism, which disappears when the magnetic field is eliminated and Ferromagnetic and ferrimagnetic materials have strong magnetization. That can be magnetized to retain its magnetism in the absence of an external field, resulting in the creation of a permanent magnet.


Diamagnetism

Michael Faraday discovered diamagnetism in September 1845. This is the weak form of magnetism that is arranged in the presence of an external magnetic field. This generates a magnetic moment that is very small and in a direction opposite to that of the applied field. Diamagnetic is a magnetism of matter in which materials are opposed by a magnetic field, an applied magnetic field creates an induced magnetic field in them that is usually in the opposite direction, causing a repulsive force. In addition, paramagnetic and ferromagnetic materials are attracted by a magnetic field.


When placed inside the strong diamagnetic and electromagnetic materials are attracted toward regions where the magnetic field is weak.  In ferromagnetic and paramagnetic material, the weak diamagnetic force is controlled by the attractive force of magnetic dipoles in the material.


Diamagnetism was first discovered by Michael Faraday in the year of 1845. In addition, when Anton Brugmans observed in 1778 that bismuth was opposed by magnetic fields. A simple rule of thumb is used in chemistry to determine whether a particle or atom or iron is paramagnetic or diamagnetic. In diamagnetic material, all electrons in the atom are paired, and the substance made from this atom. A paramagnetic material has an unpaired electron.


Paramagnetism

Paramagnetism has an unpaired electron in the material, so most atoms are incompletely filled with atomic orbitals. Hence this atom is called paramagnetism. Paramagnetism is a form of magnetism whereby several materials are weakly attracted by a strong magnetic field. In addition, paramagnetism creates a magnetic field in the direction of the applied magnetic field. Paramagnetism was discovered by the British scientist Michael Faraday in 1845. The materials that are arranged in paramagnetism are called paramagnetic. Therefore, true paramagnets are arranged in magnetic susceptibility conforming to the Curie-Weiss laws and exhibit paramagnetism over a wide temperature range.


This type of magnetization depends on Curie’s law. According to Curie’s law, paramagnetic materials, magnetic susceptibility χ are inversely proportional to their temperature. It is represented as;

M = χH = C/T x H

Where,

M = magnetization,

χ = magnetic susceptibility,

C = material-specific Curie constant,

T = absolute (Kelvin) temperature,

H = auxiliary magnetic field.

Here are some examples of paramagnetic materials, aluminum, oxygen, titanium, and iron oxide (FeO). In addition, a simple rule of thumb is used in chemistry to determine whether a particle or atom or molecule is paramagnetic or diamagnetic. This rule depends on the paired or unpaired electron.


HC Verma Volume 2 Solutions Other Chapters:


To make the most of the HC Verma Chapter 37 - Magnetic Properties of Magnet Solutions, Vedantu suggests the following tips:

Begin by thoroughly reading the chapter: It is important to have a solid understanding of the fundamental concepts and terminology before delving into the solutions.

Approach the examples step-by-step: Instead of simply memorizing the solutions, focus on understanding the logic and reasoning behind each step. This will enhance your comprehension and enable you to tackle similar problems.

Attempt the illustrative exercises independently: Challenge yourself to solve the exercises on your own before referring to the solutions. In case you encounter difficulties, the solutions can provide guidance, but attempting the problems independently first will improve your problem-solving skills.

Practice diligently: Engage in regular and consistent practice to enhance your proficiency in solving physics problems. The more you practice, the more proficient you will become.

In summary, Vedantu's Class 12 HC Verma Solutions for Chapter 37 - Magnetic Properties of Magnet offer expertly crafted solutions provided in a convenient and accessible PDF format. Utilizing these solutions, along with the suggested study tips, will empower you to excel in your physics studies.


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FAQs on HC Verma Solutions Class 12 Chapter 37 - Magnetic Properties of Matter

1. Where can I find clear, step-by-step solutions for all questions in HC Verma's Class 12 Physics Chapter 37, 'Magnetic Properties of Matter'?

Vedantu provides comprehensive, step-by-step solutions for all exercises in HC Verma's 'Magnetic Properties of Matter', Chapter 37. Each solution is prepared by subject matter experts to ensure accuracy and alignment with the problem-solving methods required for the CBSE 2025-26 board exams and competitive exams like JEE.

2. What is the correct method to solve problems related to magnetic susceptibility and permeability from HC Verma Chapter 37?

To correctly solve problems on magnetic susceptibility (χ) and permeability (μ) from this chapter, you should follow these steps:

  • First, carefully identify all the given parameters, such as magnetic intensity (H), magnetisation (M), or the magnetic field (B).
  • Recall the key relationships: B = μ₀(H + M) and M = χH.
  • Use these to find the connection between relative permeability (μᵣ) and susceptibility, which is μᵣ = 1 + χ.
  • Ensure you substitute all values using consistent SI units to arrive at the correct answer.

3. Why do diamagnetic materials have negative magnetic susceptibility, and how is this concept tested in HC Verma problems?

Diamagnetic materials have a negative magnetic susceptibility (χ) because when placed in an external magnetic field, the induced magnetic moment in them opposes the external field. This results in weak repulsion. In HC Verma problems, this concept is often tested by requiring you to:

  • Identify a material as diamagnetic based on a given negative value of χ.
  • Calculate the net magnetic field inside the material, which will be slightly weaker than the external field.
  • Differentiate the behaviour of diamagnetic, paramagnetic, and ferromagnetic materials in a uniform magnetic field.

4. How do the concepts of retentivity and coercivity, as explained in Chapter 37, help determine if a material is suitable for a permanent magnet or an electromagnet?

The suitability of a material is determined by its properties on the hysteresis loop:

  • Permanent Magnets: These require materials with high retentivity to remain strongly magnetised and high coercivity to resist demagnetisation from external fields. Steel is a classic example.
  • Electromagnets: These need materials with low retentivity and low coercivity. This allows them to be easily and quickly magnetised and demagnetised by controlling the electric current. Soft iron is the ideal choice for this application.

HC Verma solutions often feature problems where you must interpret a hysteresis curve to make these distinctions.

5. How do you calculate the intensity of magnetisation (M) for a solenoid with a magnetic core in HC Verma Chapter 37 exercises?

To calculate the intensity of magnetisation (M) for a magnetic core inside a solenoid, follow this procedure:

  • First, determine the magnetic intensity (H) generated by the solenoid current using the formula H = nI, where 'n' is the number of turns per unit length and 'I' is the current.
  • Next, use the magnetic susceptibility (χ) of the core material in the relationship M = χH.
  • If the total magnetic field (B) inside the core is provided instead, you can find M by first calculating H and then rearranging the formula B = μ₀(H + M).

6. What is a key difference in the approach to problems on magnetic properties in HC Verma compared to the NCERT textbook?

While both textbooks cover the same core topics for the Class 12 syllabus, HC Verma problems generally demand a deeper conceptual application and stronger analytical skills. NCERT focuses on establishing a solid foundation, whereas HC Verma exercises are structured to enhance problem-solving prowess for competitive exams like JEE and NEET. Consequently, HC Verma problems often feature more complex scenarios that require multi-step derivations and a nuanced understanding of how different magnetic properties interact.

7. Why is understanding the classification of magnetic materials (dia-, para-, ferro-) essential for solving problems in this chapter correctly?

Understanding the classification is critical because the material type dictates which physical laws and mathematical formulas to apply. Each class has distinct properties:

  • Diamagnetic: Susceptibility (χ) is small and negative.
  • Paramagnetic: Susceptibility (χ) is small and positive.
  • Ferromagnetic: Susceptibility (χ) is large and positive, and concepts like hysteresis and saturation are relevant.

Using the wrong assumptions for a material type, for example, ignoring hysteresis for a ferromagnetic material, will lead to an incorrect solution.

8. What is the best strategy to use Vedantu's HC Verma solutions for Chapter 37 to maximise learning?

For the most effective preparation, you should first attempt to solve the Chapter 37 exercises independently. Then, refer to Vedantu's solutions to:

  • Verify if your answer and method are correct.
  • Understand the most efficient, step-by-step approach for complex problems.
  • Clarify how to apply key formulas for magnetisation, susceptibility, and permeability in different contexts.
  • Resolve any conceptual doubts that arise during problem-solving, which is vital for both board exams and competitive tests.