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Paramagnetic Materials are those materials that get weakly magnetized when exposed to the external magnetic field. The spin of the paramagnetic materials are randomly oriented and they get arranged in the direction of the external magnetic field. They lose their magnetic properties when the external magnetic field is removed. Paramagnetic Materials are important in the field of material science as they are used for various applications
In this article, we will learn about Paramagnetic Materials, their properties, examples, applications, and how they are different from Diamagnetic Materials and Ferromagnetic Materials.
Table of Content
Paramagnetic Materials are materials that get weakly magnetized in the direction of the external magnetic field when placed in a magnetic field. They have a permanent Dipole moment. They have some unpaired electrons, and due to this, the net magnetic moment of all electrons is not added up to zero.
Learn,
Paramagnetic Materials are defined as the materials which get weakly magnetized in the direction of external magnetic field and lose their magnetic property when removed from external magnetic field
Examples of Paramagnetic Materials are,
The properties of Paramagnetic Materials are mentioned below:
The curie temperature for different paramagnetic material is tabulated below:
Substance | Curie Temperature |
|---|---|
Aluminum (Al) | 660.32°C or 1220.58°F |
Platinum (Pt) | 1772°C or 3222°F |
Copper (Cu) | 1358°C or 2476°F |
Oxygen (O2) | -183°C or -297°F |
The spin patterns of paramagnetic materials are different from those of ferromagnetic or antiferromagnetic materials. In paramagnetic materials, the magnetic moments of individual atoms or ions are randomly oriented, resulting in the absence of all magnetism. Unlike ferromagnets (in which adjacent magnetic fields are parallel) or antiferromagnets (in which adjacent magnetic fields are antiparallel), paramagnetic materials do not choose the best of their magnetic times.
Random orientation: In paramagnetic materials, the magnetic moment associated with individual atoms or ions is randomly oriented due to thermal motion. Thermal energy above the Curie temperature, or magnetic order temperature of the material, is sufficient to overcome any affinity.
No magnetic properties: Unlike ferromagnetic materials, which have positive magnetic properties and magnetic moments, paramagnetic materials do not have these properties. Lack of coordination results in a weak, transient response to the external magnetic field.
Magnetic susceptibility: Paramagnetic materials show magnetic susceptibility, which means that they can be weakly magnetized in the presence of an external magnetic field. However, when the external magnetic field is removed, the magnetic moment returns to its random direction.
There are two types of Paramagnetic Materials
The paramagnetic properties of intrinsic paramagnetic materials result from the presence of unpaired electrons in their atomic or molecular orbitals. Examples of intrinsic paramagnets include some transition metal ions, such as Fe3+ and Cr3+, and free radicals.
Examples of Intrinsic Paramagnetic Materials are Iron(III) Ion, Chromium(III) Ion, Oxygen Molecule.
Extrinsic Paramagnetic Materials acquire paramagnetic properties due to impurities or defects in non-magnetic materials. Impurities introduce unpaired electrons into the material, causing paramagnetic behavior.
Examples include Ruby (Aluminum Oxide with Chromium Impurities), Copper Sulfate (CuSO4) with Unpaired Electrons, Doped Silicon with Phosphorus Impurities.
Various properties of Paramagnetic materials are,
There are three kinds of magnetic material namely Paramagnetic, Diamagnetic and Ferromagnetic Material. A detailed comparison between them is tabulated below:
Difference Between Paramagnetic, Diamagnetic and Ferromagnetic Material | |||
|---|---|---|---|
Property | Paramagnetic Materials | Ferromagnetic Materials | Diamagnetic Materials |
Behavior | Weakly attracted to external magnetic fields. | Strongly attracted to external magnetic fields, and can retain magnetization. | Weakly repelled by external magnetic fields. |
Magnetic Moment | Alignment of magnetic moments with the applied field is temporary. | Spontaneous alignment of magnetic moments, leading to strong and persistent magnetization. | Alignment of magnetic moments opposite to the applied field is weak and temporary. |
Origin of Magnetism | Due to unpaired electrons in the presence of an external magnetic field. | Arises from the alignment of atomic magnetic moments, which can persist even in the absence of an external field. | Induced by an external magnetic field; all electrons are paired. |
Materials Examples | Iron, Aluminum, Platinum, Gadolinium. | Iron, Cobalt, Nickel. | Copper, Bismuth, Zinc. |
Magnetic Susceptibility | Positive | High positive magnetic susceptibility. | Negative |
Curie Temperature | Typically, there is no Curie temperature | Above the Curie temperature, ferromagnetic materials lose their magnetic properties. | Below the Curie temperature, diamagnetic materials exhibit weak repulsion. |
Applications | MRI contrast agents, electromagnetic devices, research probes. | Permanent magnets, transformer cores, magnetic storage media. | Magnetic levitation, superconductors, screening of magnetic fields. |
Interaction Range | Interaction is short-range and weak. | Interaction can extend over longer distances. | Interaction is weak and short-range. |
There are two formulas related to properties of Paramagnetic Material which are mentioned below:
Let's discuss these two formulas in detail
Magnetic susceptibility of an object, expressed as χ, measures its response to an external magnetic field. For paramagnetic materials, the magnetic susceptibility is positive and small. The formula is:
χ = M/H
where,
- χ is Magnetic Susceptibility
- M is Magnetization
- H is applied Magnetic Field
Example: Suppose you have a paramagnetic material that has a Magnetization of (M) of 2.5 A/m when exposed to a magnetic field (H) of 500 A/m. Calculate the magnetic susceptibility.
χ = M/H
χ = 2.5/500
χ = 0.005
Curie's law describes the magnetic susceptibility of paramagnetic materials as a function of temperature. The formula is given by:
χ = C/T
where
- χ is Magnetization
- C is the Curie constant
- T is the absolute temperature.
χ = C/T
χ = 2.0/300
χ = 0.0067
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