Magnetic Properties of Solids and Their Applications

Magnetic Properties of Solids

  • Materials can be classified based on their response to externally applied magnetic fields into three categories: diamagnetic, paramagnetic, and ferromagnetic.
    • These classifications differ significantly in their magnetic responses' strength.

1. Diamagnetism

  • All materials exhibit diamagnetism, which is a property that opposes applied magnetic fields.
  • It is characterized as a very weak effect and is present in all materials.
  • When a magnetic field is applied, diamagnetic materials develop an induced magnetic moment that opposes the field, thereby weakening it.
  • The absolute value of the magnetic susceptibility χ is typically in the range of ext{|χ| ext{~} 10^{-6} ext{ to } 10^{-4}}.
  • Common examples include:
    • Inert gases,
    • Bismuth,
    • Silver,
    • Water,
    • Hydrogen,
    • Carbon,
    • Copper,
    • Germanium,
    • Silicon.
  • Diamagnetism was discovered by Michael Faraday, who named the phenomenon.
  • Importantly, the magnetic susceptibility χ of diamagnetic materials does not depend on temperature or the intensity of the external magnetic field.

2. Paramagnetism

  • Paramagnetic materials are characterized by a magnetic susceptibility χ > 0, where they exhibit a weak amplification of the resultant magnetic field when placed in an applied magnetic field, following the relationship χ ext{~} 10^{-4} ext{ to } 10^{-3}.
  • Common paramagnetic materials include:
    • Aluminum,
    • Platinum,
    • Liquid oxygen,
    • Electron gas in metals,
    • Rare earth elements,
    • Alkaline and alkaline earth metals.
  • In such materials, the atomic magnetic moments align partially in the direction of the applied field, although thermal motion limits the degree of alignment.
  • Curie's Law applies to paramagnetic materials: the susceptibility follows the equation χ = rac{C}{T}, where C is Curie’s constant and T is the temperature. This law holds true for weak external fields and at moderate temperatures.
  • Paramagnetic materials can be magnetized to saturation at high external field values.

3. Ferromagnetism

  • Ferromagnetic materials demonstrate a very high magnetic susceptibility χ >> 0, and possess own magnetic fields significantly exceeding the external applied field (by hundreds or thousands of times).
  • Examples of ferromagnetic materials include:
    • Iron,
    • Nickel,
    • Cobalt,
    • Gadolinium,
    • Special alloys.
  • Specific characteristics include:
    • Magnetic hysteresis, where the magnetization depends on the historical value of the magnetic field.
    • The magnetic permeability C{ 8{B} = C{0} ext{H}} exhibits nonlinear behavior with respect to H_0.
  • The magnetic susceptibility of ferromagnets changes with temperature:
    • Each ferromagnetic material has a notable Curie Temperature (TC); for example, iron has TC = 768 °C, nickel has TC = 358 °C, and cobalt has TC = 1120 °C.
  • Magnetostriction: changes in dimensions occur during magnetization and demagnetization of ferromagnetic materials, useful for applications in ultrasonic devices.

4. Ferrites and Ferrimagnets

  • Ferrites are materials with ferromagnetic properties characterized by semiconductor properties, having a specific resistance ρ ext{~} 10^7 ext{ } ext{Ωm}.
  • Typical examples include magnetite (Fe₃O₄) and compounds like MeO ext{.Fe₂O₃}, where Me represents divalent metals (e.g., Mg, Ni, Co, Cr).
  • Ferrites are advantageous for high-frequency applications due to their low eddy current losses and relatively low Curie temperatures (30 to 700 °C).

5. Antiferromagnetism

  • Antiferromagnetic materials exhibit slightly greater magnetic susceptibility than paramagnets but become paramagnetic above a critical temperature (the Néel temperature).
  • Common examples include manganese, chromium, various oxides, sulfides, and halides.
  • Antiferromagnets exhibit antiparallel arrangements of identical spin magnetic moments in their structure.
  • Typical compounds include manganese oxide (MnO) and cobalt oxide (CoO).

Physical Nature of Magnetism

  • Atoms and molecules can possess or acquire magnetic moments in an external magnetic field:
    • The total magnetic moment of an atom is the vector sum of the orbital (p{ml}) and spin magnetic moments (p{ms}) of electrons, as well as that of the nucleus (p{mn}).
    • The equations governing these properties include:
      oldsymbol{p}{ma} = oldsymbol{p}{ml} + oldsymbol{p}{ms} + oldsymbol{p}{mn}
      oldsymbol{p}_{ml} = rac{e v r}{2 l}, where l denotes the orbital angular momentum.

Magnetocardiography (MCG)

  • MCG technique records the magnetic fields generated by the heart's electrical activity.
  • It offers spatially and temporally accurate measurements of weak heart magnetic fields.
  • MCG provides diagnostic information surpassing traditional electrocardiogram (ECG) readings in some cases.

Magnetotherapy

  • A therapeutic modality employing magnets (often made from ferrites) for health applications.
  • Magnets used may include static and electromagnetic types, with various application approaches.
  • Treatment options include permanent magnets or specialized devices integrating electromagnetic fields (e.g. jewelry, mattresses).

Electron Paramagnetic Resonance (EPR)

  • EPR studies the behavior of unpaired electrons in a magnetic field.
  • It involves the resonance condition h
    u_{res} = oldsymbol{oldsymbol{ ext{C{B}}}} ext{ and } ext{energy }
    u, where oldsymbol{oldsymbol{B}} represents the magnetic field.
  • EPR methods are pivotal in biological research, aiding in understanding free radical impact.
    • EPR's foundation lies in the magnetic moment leading to the splitting of spectral lines (Zeeman effect).

Nuclear Magnetic Resonance (NMR) and Magnetic Resonance Imaging (MRI)

  • NMR refers to the absorption and reemission of energy by atomic nuclei when subjected to magnetic fields.
  • Characterized by resonance frequency dependent on magnetic field strength and nucleus type, focusing on isotopes like ^{1}H and ^{13}C.
  • MRI employs hydrogen nuclei as a primary imaging method, enhancing the visualization of tissues due to their high mobility and concentration in human bodies.
  • Image resolution in MRI hinges on magnetic field strength, slice thickness, and tissue properties.
  • Contrast manipulations vary with T1 and T2 weighting, aiding in the differentiation of normal and pathological tissues.

Clinical Applications of MRI

  • MRI is particularly effective in visualizing soft tissues, aiding diagnoses in multiple medical fields including neurology, orthopedics, and vascular studies.
  • High-field MRI systems surpass low-field counterparts in image quality, making them optimal for specialized investigations.
  • The advent of advanced computers and imaging techniques continues to evolve MRI applications.