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Magnetization

physical science Maturity 11-13 Next article →

Magnetization is a fundamental concept in classical electromagnetism. It is a vector field that expresses the density of magnetic dipole moments within a material. These moments can be permanent or induced by an outside force. Physicists and engineers define magnetization as the quantity of magnetic moment per unit volume. This is represented by the symbol M. It describes how a material responds to an applied magnetic field. It also shows how the material changes that magnetic field. Scientists use these measurements to calculate the resulting magnetic forces.

Bound currents
Bound currents

The origin of these magnetic moments lies at the microscopic level. They come from tiny electric currents caused by the motion of electrons in atoms. The spin of electrons or atomic nuclei also creates these moments. When these tiny movements align, they create net magnetization. This process is very similar to electric polarization. In electrostatics, electric polarization measures how a material responds to an electric field. Magnetization is the magnetic version of this same concept. It is measured in amperes per meter (A/m) using SI units.

Materials respond to magnetic fields in several distinct ways. Paramagnetic materials show a weak induced magnetization when a field is applied. This magnetism disappears as soon as the external field is removed. In contrast, ferromagnetic and ferrimagnetic materials show very strong magnetization. These materials can stay magnetized even after the external field is gone. This ability allows them to become permanent magnets. Magnetization is not always uniform. It can vary between different points within the same material.

In physics, magnetization is closely linked to other magnetic properties. It helps define the auxiliary magnetic field, known as H. In many materials, a linear relationship exists between M and H. This relationship involves the volume magnetic susceptibility, represented by the Greek letter chi. It also involves the magnetic permeability, or mu, of the material. In ferromagnets, this one-to-one correspondence does not exist. Instead, these materials experience magnetic hysteresis. This means the magnetization depends on the material's previous magnetic history.

Magnetization also creates what is known as magnetization current. When microscopic currents induced by magnetization do not balance out, new currents appear. These are called bound volume currents and bound surface currents. These currents contribute to the total current density in Maxwell's equations. This total density includes the free current from moving charges. It also includes the contribution from the magnetization itself. In certain math models, the term minus the gradient of M acts like a fictitious magnetic charge density.

Bound currents
Bound currents

We can also change the direction of magnetization through a process called reversal. This is also known as switching. It occurs when the magnetization vector re-orients by 180 degrees. This means the magnetic direction flips to its opposite stable orientation. This process is vital for modern technology. It is the fundamental mechanism used in magnetic data storage, such as hard disk drives. There are three known ways to reverse a metallic magnet. One is by applying a magnetic field. Another is via spin injection using a beam of particles. The third is using circularly polarized light.

Sometimes, it is necessary to perform demagnetization. This is the reduction or total elimination of magnetization. One common method is heating an object above its Curie temperature. At this temperature, thermal fluctuations provide enough energy to destroy the magnetic order. Another method involves using an electric coil with alternating current. This creates fields that oppose the existing magnetization. This is useful for removing unwanted magnetic fields that interfere with computers or cell phones.

A more recent discovery is ultrafast demagnetization. This method uses intense laser pulses that last only a femtosecond. This process is extremely fast, occurring in less than a picosecond. It is considered a non-equilibrium process because it does not rely on heat. The laser pulse deposits energy directly into the material's electrons. This energy moves to the spin system through electron-magnon scattering. This causes the magnetic order to collapse before the material's lattice even heats up. This discovery is a major area of research for future high-speed spintronic devices.

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