is a key concept in solid state physics, measuring how materials respond to magnetic fields. It helps classify materials as diamagnetic or paramagnetic, with being repelled and attracted to magnetic fields.
Diamagnetism and paramagnetism are two fundamental types of magnetism in materials. Diamagnetism opposes applied fields and occurs in all materials, while paramagnetism aligns with fields and requires unpaired electrons. Understanding these properties is crucial for many technological applications.
Magnetic susceptibility
Magnetic susceptibility is a measure of how strongly a material responds to an applied magnetic field
It is a fundamental property in the study of magnetic materials and their behavior in solid state physics
The sign and magnitude of magnetic susceptibility can be used to classify materials as diamagnetic, paramagnetic, or ferromagnetic
Diamagnetic vs paramagnetic materials
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Diamagnetic materials have a negative magnetic susceptibility, meaning they are slightly repelled by an applied magnetic field (bismuth, copper, water)
Paramagnetic materials have a positive magnetic susceptibility, meaning they are slightly attracted to an applied magnetic field (aluminum, platinum, oxygen)
The magnitude of the susceptibility is typically much larger for paramagnetic materials compared to diamagnetic materials
Magnetic susceptibility tensor
In anisotropic materials, the magnetic susceptibility is a tensor quantity, meaning it depends on the direction of the applied magnetic field
The susceptibility tensor is a 3x3 matrix that relates the induced magnetization to the applied magnetic field
The principal axes of the susceptibility tensor correspond to the directions of maximum and minimum susceptibility
Measuring magnetic susceptibility
Magnetic susceptibility can be measured using various techniques, such as the Faraday balance, vibrating sample magnetometer (VSM), and superconducting quantum interference device (SQUID)
These techniques involve applying a known magnetic field to the sample and measuring the resulting magnetization or force on the sample
Temperature-dependent susceptibility measurements can provide insights into the magnetic properties and phase transitions of materials
Diamagnetism
Diamagnetism is a weak form of magnetism that opposes an applied magnetic field
It arises from the induced magnetic moments of the electrons in an atom or molecule
Diamagnetic materials have no unpaired electrons and do not possess a permanent magnetic moment
Origin of diamagnetism
Diamagnetism originates from the change in the orbital motion of electrons in an atom or molecule when an external magnetic field is applied
According to , the induced current in the electron orbits creates a magnetic field that opposes the applied field
This results in a negative magnetic susceptibility and a repulsive force on the material
Diamagnetic susceptibility
The diamagnetic susceptibility is negative and typically on the order of -10^-5 to -10^-6 (SI units)
It is temperature-independent and does not vary with the strength of the applied magnetic field
The diamagnetic susceptibility can be calculated using Langevin's theory of diamagnetism, which considers the induced magnetic moments of the electrons
Diamagnetism in metals
In metals, the conduction electrons contribute to the diamagnetic susceptibility
The Landau diamagnetism arises from the quantization of the electron orbits in a magnetic field (Landau levels)
The Landau susceptibility is proportional to the density of states at the Fermi level and depends on the Fermi surface topology
Diamagnetism in insulators
In insulators, the diamagnetic susceptibility is determined by the bound electrons in the atoms or molecules
The susceptibility can be calculated using the Langevin-Larmor formula, which considers the induced magnetic moments of the electrons
The diamagnetic susceptibility of insulators is typically smaller than that of metals due to the absence of conduction electrons
Diamagnetic levitation
Diamagnetic materials can be levitated in strong magnetic fields due to their
Stable levitation occurs when the diamagnetic force balances the gravitational force on the object
Diamagnetic levitation has applications in materials processing, such as containerless processing of high-purity materials (graphite, bismuth, water droplets)
Paramagnetism
Paramagnetism is a form of magnetism where materials are attracted to an applied magnetic field
Paramagnetic materials have unpaired electrons in their atomic or molecular orbitals, which give rise to a net magnetic moment
The magnetic moments in paramagnetic materials are randomly oriented in the absence of an external field and align partially with the field when one is applied
Origin of paramagnetism
Paramagnetism arises from the presence of unpaired electrons in the atomic or molecular orbitals of a material
Each unpaired electron has a magnetic moment associated with its spin angular momentum
In the absence of an external magnetic field, these magnetic moments are randomly oriented due to thermal agitation
Paramagnetic susceptibility
The paramagnetic susceptibility is positive and typically on the order of 10^-3 to 10^-5 (SI units)
It is temperature-dependent, with the susceptibility decreasing as temperature increases
The paramagnetic susceptibility can be described by the or the Curie-Weiss law, depending on the presence of magnetic interactions between the moments
Curie's law
Curie's law states that the paramagnetic susceptibility is inversely proportional to the absolute temperature: χ=C/T
The Curie constant, C, depends on the effective magnetic moment of the paramagnetic ions and the density of the material
Curie's law assumes that the magnetic moments are non-interacting and that the thermal energy is much larger than the magnetic interaction energy
Curie-Weiss law
The Curie-Weiss law is a modification of Curie's law that accounts for the presence of magnetic interactions between the moments
It states that the paramagnetic susceptibility follows the relation: χ=C/(T−θ), where θ is the Weiss constant
A positive Weiss constant indicates ferromagnetic interactions, while a negative Weiss constant indicates antiferromagnetic interactions
Paramagnetic materials
Examples of paramagnetic materials include transition metal ions (Fe^3+, Mn^2+), rare earth ions (Gd^3+, Er^3+), and organic radicals (DPPH, TEMPO)
Paramagnetic salts, such as Mohr's salt (ammonium iron(II) sulfate), are commonly used in magnetic susceptibility measurements
Liquid oxygen is paramagnetic due to the presence of unpaired electrons in the oxygen molecules
Langevin theory of paramagnetism
The Langevin theory of paramagnetism is a classical approach to describing the behavior of paramagnetic materials in an applied magnetic field
It assumes that the magnetic moments are non-interacting and that their orientation is determined by the competition between the magnetic energy and the thermal energy
The theory provides a good approximation for the magnetization and susceptibility of paramagnetic materials at high temperatures
Classical approach
In the classical approach, the magnetic moments are treated as classical vectors that can orient in any direction
The orientation of the moments is determined by the balance between the magnetic energy, which tends to align the moments with the field, and the thermal energy, which tends to randomize their orientation
The distribution of the magnetic moments is described by the Boltzmann distribution, which gives the probability of a moment having a particular orientation
Langevin function
The Langevin function, L(α)=coth(α)−1/α, describes the average magnetization of a paramagnetic material as a function of the applied magnetic field
The parameter α is the ratio of the magnetic energy to the thermal energy: α=μB/kBT, where μ is the magnetic moment, B is the applied field, kB is the Boltzmann constant, and T is the absolute temperature
The Langevin function saturates to unity for large values of α, indicating a complete alignment of the magnetic moments with the field
Limitations of Langevin theory
The Langevin theory assumes that the magnetic moments are non-interacting, which is not always the case in real materials
It does not account for the quantum mechanical nature of the magnetic moments, which becomes important at low temperatures or for materials with strong spin-orbit coupling
The theory fails to describe the behavior of materials with localized magnetic moments, such as rare earth ions, where the crystal field effects play a significant role
Quantum theory of paramagnetism
The quantum theory of paramagnetism takes into account the quantum mechanical nature of the magnetic moments and their interactions with the crystal environment
It provides a more accurate description of the magnetic properties of paramagnetic materials, especially at low temperatures or for materials with strong spin-orbit coupling
The theory considers the contributions of both the spin and orbital angular momenta to the magnetic moment
Spin and orbital angular momentum
In atoms and ions, the magnetic moment arises from the spin and orbital angular momenta of the electrons
The spin angular momentum, S, is an intrinsic property of the electron and has a value of 1/2
The orbital angular momentum, L, is associated with the motion of the electron around the nucleus and can take integer values
The total angular momentum, J, is the vector sum of the spin and orbital angular momenta: J=L+S
Hund's rules
Hund's rules are a set of empirical rules that determine the ground state electronic configuration of an atom or ion
The first rule states that the electrons occupy orbitals to maximize the total spin, S
The second rule states that the electrons occupy orbitals to maximize the total orbital angular momentum, L, consistent with the first rule
The third rule states that the total angular momentum, J, is equal to ∣L−S∣ for a less than half-filled shell and L+S for a more than half-filled shell
Effective magnetic moment
The effective magnetic moment, μeff, is a measure of the strength of the paramagnetic response of an atom or ion
It is related to the total angular momentum, J, by the equation: μeff=gJJ(J+1)μB, where gJ is the Landé g-factor and μB is the Bohr magneton
The effective magnetic moment can be determined experimentally from the Curie constant, C, obtained from susceptibility measurements
Van Vleck paramagnetism
Van Vleck paramagnetism is a form of temperature-independent paramagnetism that arises from the mixing of the ground state with excited states by the applied magnetic field
It occurs in materials with a non-magnetic ground state and low-lying excited states that can be mixed by the field
The Van Vleck susceptibility is given by the Van Vleck formula, which considers the matrix elements of the magnetic moment operator between the ground state and the excited states
Applications
The magnetic properties of diamagnetic and paramagnetic materials have numerous applications in various fields, ranging from medicine to materials science
These applications exploit the unique response of these materials to applied magnetic fields and their temperature-dependent behavior
Understanding the fundamental principles of diamagnetism and paramagnetism is crucial for developing new technologies and optimizing existing ones
Magnetic resonance imaging (MRI)
MRI is a non-invasive medical imaging technique that relies on the magnetic properties of hydrogen atoms in the body
It uses strong magnetic fields and radio waves to manipulate the spin of the hydrogen nuclei and generate detailed images of the body's internal structures
Paramagnetic contrast agents, such as gadolinium complexes, are often used to enhance the contrast between different tissues in MRI scans
Magnetic levitation
Magnetic levitation exploits the repulsive force experienced by diamagnetic materials in strong magnetic fields
It has applications in high-speed transportation, such as maglev trains, where the train is levitated above the track by powerful superconducting magnets
Diamagnetic levitation is also used in materials processing, such as containerless processing of high-purity materials, to avoid contamination from the container walls
Magnetic refrigeration
Magnetic refrigeration is an energy-efficient cooling technology that utilizes the magnetocaloric effect in paramagnetic materials
It involves the cyclic magnetization and demagnetization of a paramagnetic material, which causes a temperature change due to the coupling between the magnetic and thermal properties
Magnetic refrigeration has the potential to replace conventional vapor-compression refrigeration systems, offering higher efficiency and reduced environmental impact
Magnetic separation
Magnetic separation is a process that uses magnetic fields to separate magnetic materials from non-magnetic materials
It has applications in mineral processing, where paramagnetic minerals (ilmenite, wolframite) are separated from diamagnetic gangue minerals (quartz, calcite)
Magnetic separation is also used in biotechnology for the isolation and purification of biomolecules, such as proteins and nucleic acids, using paramagnetic beads coated with specific ligands
Key Terms to Review (19)
Curie Law: Curie Law states that the magnetization of a paramagnetic material is directly proportional to the applied magnetic field and inversely proportional to its temperature. This relationship highlights how the magnetic properties of materials change with temperature, particularly in paramagnets, where the alignment of magnetic moments occurs due to thermal energy.
Data Storage: Data storage refers to the methods and technologies used to retain digital information for future access and retrieval. It encompasses various forms of physical and non-physical mediums that can hold data, including hard drives, solid-state drives, and cloud storage. The effectiveness of data storage solutions is often measured by their speed, capacity, durability, and ability to manage different states of magnetic behavior, which ties closely into concepts like diamagnetism and paramagnetism.
Diamagnetic materials: Diamagnetic materials are substances that exhibit a weak and negative response to an external magnetic field, meaning they are repelled by the field. This behavior arises from the paired electrons in their atomic structure, which generate a very small magnetic field in the opposite direction to that of the applied field. As a result, diamagnetic materials do not retain any magnetization in the absence of an external magnetic field.
Electron spin: Electron spin is a fundamental property of electrons that describes their intrinsic angular momentum and magnetic moment, characterized as a form of quantum mechanical rotation. This property plays a crucial role in determining the magnetic behavior of materials, particularly in phenomena like diamagnetism and paramagnetism. Each electron can be thought of as a tiny magnet due to its spin, and the alignment of these spins in a material influences its overall magnetic characteristics.
Lenz's Law: Lenz's Law states that the direction of an induced electromotive force (emf) and the resulting current in a closed loop is such that it opposes the change in magnetic flux that produced it. This principle is rooted in the conservation of energy, ensuring that the induced current creates a magnetic field that counteracts the initial change. It plays a significant role in understanding both diamagnetism and paramagnetism, where the behavior of materials in response to external magnetic fields can be explained by how they interact with induced currents.
Magnetic domains: Magnetic domains are small regions within ferromagnetic materials where the magnetic moments of atoms are aligned in the same direction, resulting in a net magnetic field. Each domain acts like a tiny magnet, and the overall magnetic behavior of the material depends on how these domains are arranged and how they interact with each other. The presence and alignment of these domains play a crucial role in determining the magnetic properties of materials, particularly in relation to their behavior under external magnetic fields and their response in various magnetic phenomena.
Magnetic ordering: Magnetic ordering refers to the arrangement of magnetic moments in a material, which can exhibit various patterns of alignment depending on temperature and interactions between atoms. This concept is vital for understanding how different magnetic materials behave, including their response to external magnetic fields and their internal symmetry properties.
Magnetic susceptibility: Magnetic susceptibility is a measure of how much a material will become magnetized in response to an applied magnetic field. It quantifies the degree to which a material can be magnetized and indicates whether the material is diamagnetic, paramagnetic, or ferromagnetic. Understanding magnetic susceptibility helps in categorizing materials based on their magnetic behavior under external influences.
Magnetic susceptibility equation: The magnetic susceptibility equation is a mathematical representation that quantifies how much a material will become magnetized in an external magnetic field. This equation is crucial in understanding the behavior of materials in the presence of magnetic fields, particularly in distinguishing between different types of magnetic materials like diamagnetic and paramagnetic substances.
Michael Faraday: Michael Faraday was a pioneering scientist known for his fundamental contributions to the fields of electromagnetism and electrochemistry during the 19th century. His groundbreaking work laid the foundation for the understanding of electromagnetic induction, which is crucial for the development of technologies like electric generators and transformers, linking closely to the principles of diamagnetism and paramagnetism.
MRI Imaging: MRI imaging, or Magnetic Resonance Imaging, is a medical imaging technique that uses strong magnetic fields and radio waves to generate detailed images of organs and tissues inside the body. It plays a vital role in diagnosing and monitoring various medical conditions, providing high-resolution images without the use of ionizing radiation.
Negative susceptibility: Negative susceptibility refers to a phenomenon in which a material exhibits a decrease in magnetization when subjected to an external magnetic field. This behavior is primarily observed in diamagnetic materials, which develop an induced magnetic moment that opposes the applied magnetic field, leading to a negative response. This concept highlights how different materials interact with magnetic fields and emphasizes the contrasting properties of diamagnetism compared to paramagnetism.
Paramagnetic materials: Paramagnetic materials are substances that exhibit a weak attraction to magnetic fields due to the presence of unpaired electrons in their atomic or molecular structures. This characteristic results in the alignment of these unpaired spins when exposed to an external magnetic field, causing the material to become magnetized, albeit weakly. The behavior of paramagnetic materials is a crucial aspect of understanding the broader concepts of magnetism, especially in contrast to diamagnetism.
Pierre Curie: Pierre Curie was a pioneering French physicist known for his work in radioactivity, crystallography, and magnetism, and he is best remembered for his contributions to the understanding of piezoelectricity, diamagnetism, and ferromagnetism. His research laid important groundwork in these fields and helped shape modern physics by highlighting the connections between material properties and their physical behaviors under various conditions.
Positive susceptibility: Positive susceptibility is a measure of how much a material becomes magnetized in response to an external magnetic field, indicating that the material tends to be attracted to the magnetic field. This term is particularly relevant in understanding materials that exhibit paramagnetism, where the presence of unpaired electrons leads to a net magnetic moment, causing the material to align with the applied magnetic field and enhance it. In contrast to diamagnetic materials, which exhibit negative susceptibility, those with positive susceptibility show a stronger response when subjected to magnetic forces.
Squid magnetometry: Squid magnetometry is a highly sensitive technique used to measure magnetic fields, employing superconducting quantum interference devices (SQUIDs) to detect minute changes in magnetic flux. This method is particularly useful for studying the magnetic properties of various materials, providing insights into phenomena such as diamagnetism, paramagnetism, ferromagnetism, and antiferromagnetism. It allows researchers to explore the intricate relationships between temperature, magnetic fields, and the behavior of different materials at the atomic level.
Superconductivity: Superconductivity is a phenomenon where certain materials exhibit zero electrical resistance and the expulsion of magnetic fields when cooled below a specific critical temperature. This unique state leads to fascinating applications such as lossless power transmission, magnetic levitation, and advanced quantum computing. The underlying mechanisms of superconductivity involve interactions between electrons and phonons, which are crucial for understanding the behavior of these materials under varying conditions.
Vibrating Sample Magnetometry: Vibrating Sample Magnetometry (VSM) is a sensitive technique used to measure the magnetic properties of materials by analyzing the induced voltage in a coil caused by a sample vibrating in a magnetic field. This method allows researchers to determine key parameters such as magnetization, susceptibility, and coercivity of both diamagnetic and paramagnetic substances. The VSM is particularly valuable for studying materials at different temperatures and magnetic field strengths, providing insight into their magnetic behavior.
Weiss Mean Field Theory: Weiss Mean Field Theory is a theoretical framework used to describe magnetic phase transitions in materials by averaging the interactions between magnetic moments. This approach simplifies the complexities of many-body systems by treating the effect of neighboring spins on a given spin as a uniform or 'mean field'. This concept is particularly relevant in understanding phenomena like diamagnetism and paramagnetism, where the alignment of magnetic moments under external fields plays a crucial role.