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Which of the following is true? (A) Diamagnetism is temperature dependent (B) Paramagnetism is temperature dependent (C) Paramagnetism is temperature independent (D) None of the above

Short Answer

Expert verified
(B) Paramagnetism is temperature dependent.

Step by step solution

01

Statement A: Diamagnetism is temperature dependent

Diamagnetism occurs in materials where there are no unpaired electrons, and all atomic magnetic moments are paired. It is a weak, negative response to an applied magnetic field. The induced magnetization is independent of temperature. In this case, Statement A is false.
02

Statement B: Paramagnetism is temperature dependent

Paramagnetism occurs in materials with unpaired electrons, and their atomic magnetic moments are aligned parallel to an applied magnetic field. The susceptibility of a paramagnetic material (the degree to which it responds to a magnetic field) is inversely proportional to its temperature (Curie's Law). Therefore, the paramagnetic response decreases as the temperature increases. In this case, Statement B is true.
03

Statement C: Paramagnetism is temperature independent

This statement directly contradicts Statement B, which we have already determined to be true. As the paramagnetic susceptibility is inversely proportional to temperature, the paramagnetic property is not temperature-independent. Thus, Statement C is false.
04

Statement D: None of the above

Since Statement B is true, Statement D indicating that none of the statements are true is false. Based on our analysis, the correct answer is: (B) Paramagnetism is temperature dependent.

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Key Concepts

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

Diamagnetism Temperature Dependence
In the realm of magnetism, diamagnetism is often misunderstood when it comes to its relationship with temperature. Unlike paramagnetic materials, diamagnetic materials exhibit a very weak form of magnetism. This occurs because electrons within the material's atoms are paired, and as a result, their magnetic moments cancel each other out.
An important point to understand is that the magnetization of diamagnetic materials is generally independent of temperature. The reason for this is that the electron pairing that causes their diamagnetic properties is not easily disrupted by thermal energy. When an external magnetic field is applied, these materials develop an induced magnetic moment that is very small and in the opposite direction to the applied field.

Implications on Material Properties

Due to their temperature-independence, diamagnetic materials maintain consistent magnetic behavior across a diverse range of temperatures. This characteristic makes them useful in applications where stability in the presence of magnetic fields is critical, such as in magnetic levitation and in the construction of magnetic shielding for sensitive electronic instruments.
Paramagnetic Susceptibility
Moving on to paramagnetic materials, we delve into the concept of paramagnetic susceptibility. Susceptibility is a measure of how much a material will become magnetized in an applied magnetic field. Paramagnetic materials are those that have atoms or ions with unpaired electrons. These unpaired electrons have intrinsic magnetic moments that tend to align with external magnetic fields, which makes these materials magnetically responsive.
Paramagnetic susceptibility is not constant and is highly influenced by a variety of factors, notably temperature.

Temperature's Role

As the temperature of a paramagnetic material increases, the thermal energy contributes to randomizing the orientation of the magnetic moments of the unpaired electrons. This thermal agitation reduces the efficacy of the external magnetic field to align these moments, thus decreasing the paramagnetic susceptibility. In essence, the magnetization of a paramagnetic material decreases as the temperature rises. It is this very dependence on temperature that gives rise to fascinating applications, especially in situations requiring temperature-based modulation of magnetic properties.
Curie's Law
Understanding paramagnetism leads us directly to a key principle known as Curie's Law. This law is fundamental in describing how the susceptibility (\b\(\bigchi\)\b)) of paramagnetic materials changes with temperature.

The Curie's Law Equation

Curie's Law is mathematically expressed as \(\bigchi = \frac{C}{T}\), where \(C\) is the Curie constant, which depends on the material, and \(T\) is the absolute temperature in Kelvin. This relationship indicates that susceptibility is inversely proportional to temperature.
In simpler terms, as you heat a paramagnetic material, the increasing disarray among its atomic magnetic moments leads to a decrease in its ability to align with a magnetic field, thus decreasing its overall magnetic susceptibility.

Significance in Physics

This law is critical in the study of magnets and has implications for various applications, including magnetic resonance imaging (MRI) and temperature sensors that rely on magnetic properties. Knowledge of Curie's Law also helps in understanding the behaviors of materials at the atomic level, which is vital for researchers and technologists working in the field of material science and its applications in modern technology.

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Most popular questions from this chapter

An electron accelerated by a potential difference \(V=3.6 \mathrm{~V}\) first enters into a uniform electric field of a parallel-plate capacitor whose plates extend over a length \(l=6 \mathrm{~cm}\) in the direction of initial velocity. The electric field is normal to the direction of initial velocity and its strength varies with time as \(E=a \times t\), where \(a=\) \(3200 \mathrm{Vm}^{-1} \mathrm{~s}^{-1}\). Then the electron enters into a uniform magnetic field of induction \(B=\pi \times 10^{-9} \mathrm{~T}\). Direction of magnetic field is same as that of the electric field. Calculate pitch (in \(\mathrm{mm}\) ) of helical path traced by the electron in the magnetic field (Mass of electron, \(m=9 \times\) \(10^{-31} \mathrm{~kg}\) ). [Neglect the effect of induced magnetic field.]

An equilateral triangular current loop \(P Q R\) carries a current \(I\) ampere. Length of each side is \(l\) metre. A uniform magnetic field of induction \(\vec{B}\) exists in a direction parallel to \(P Q\). Then the force on the side \(P Q\) is (A) \(I I B\) (B) \(\frac{I l B}{2}\) (C) \(\left(\frac{I l B}{2}\right) \sqrt{3}\) (D) Zero

A metal disc of radius \(R=6 \mathrm{~cm}\) is mounted on a frictionless axle. The current can flow through the axle out along the disc to a sliding contact of rim of the disc. A uniform magnetic field \(B=2 \mathrm{~T}\) is parallel to the axis of the disc. When the current is \(3 \mathrm{~A}\), the disc rotateswith constant angular velocity. The frictional force at the rim between the stationary electrical contact and the rotating rim is \(9 x \times 10^{-2} \mathrm{~N}\). Find the value of \(x\). W

Two short bar magnets of magnetic moments \(M\) each are arranged at the opposite corners of a square of side \(d\), such that their centers coincide with the corners and their axes are parallel. If the like poles are in the same direction, the magnetic induction at any of the other corners of the square is (A) \(\frac{\mu_{0}}{4 \pi} \cdot \frac{M}{d^{3}}\) (B) \(\frac{\mu_{0}}{4 \pi} \cdot \frac{2 M}{d^{3}}\) (C) \(\frac{\mu_{0}}{4 \pi} \cdot \frac{M \sqrt{5}}{d^{3}}\) (D) \(\frac{\mu_{0}}{4 \pi} \cdot \frac{3 M}{d^{3}}\)

A long wire having linear charge density \(\lambda\) moving with constant velocity \(v\) along its length. A point charge moving with same speed in opposite direction and at that instant, it is \(r\) distance from the wire. The net force acting on the charge is given by (A) \(\frac{\lambda q}{2 \pi r}\left[\frac{1}{\varepsilon_{0}}+v^{2} \mu_{0}\right]\) (B) \(\frac{\lambda q}{2 \pi r}\left[\frac{1}{\varepsilon_{0}}-\mu_{0} v^{2}\right]\) (C) \(\frac{\lambda q}{2 \pi r} \sqrt{\left(\frac{1}{\varepsilon_{0}}\right)^{2}+v^{4} \mu_{0}^{2}}\) (D) Zero

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