GEC PATAN SEM 5 2015 Engineering Electromagnetics Magnetic Materials Prepared by Vaghela Krincle R. 130220111114.

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Presentation transcript:

GEC PATAN SEM Engineering Electromagnetics Magnetic Materials Prepared by Vaghela Krincle R

Introduction ► Question: Why do some materials respond to magnetic fields, while others do not? ► Answer: Magnetic materials have a property known as Magnetization as quantified in the relative permeability constant (  r ).

Description of Magnetic Material Properties ► For accurate quantitative prediction: Quantum Theory is required ► For qualitative description: Orbital Mechanics Model suffices

Orbital Mechanics Model ► Atom has electrons that orbit around its nucleus making a miniature current loop that results in an orbital magnetic moment ► Electron spins around its own axis to produce a significant spin magnetic moment

Orbital Mechanics Model ► The relative contribution of the magnetic moments of each atom and the molecular makeup of a material classifies it as – Diamagnetic – Paramagnetic – Ferromagnetic – Antiferromagnetic – Ferrimagnetic – Superparamagnetic ► Any atom with a magnetic moment in the presence of an applied magnetic field will experience a torque that tends to align it

Domain ► Definition: a region within a ferromagnetic material having a large dipole moment due to collections of associated atoms with uncompensated spin moments ► Shape, size & direction of moment: varies between neighboring regions within a crude sample that cancels the effect overall See also magnetic dipole moments and domains of ferromagnetic materials as illustrated in Fig WW pp. 139, 140.

Alignment of Magnetic Domains ► Alignment: may be achieved by an applied magnetic field ► Upon removal of the external magnetic field, domains do not all return to their original state and thus exhibit a magnetic history known as hysteresis (an interesting & practical effect unique to ferromagnetic materials) ► Examples: Ferromagnetic elements & compounds Fe, Ni, Co, BiMn, CuMnSn, etc.

Other Examples of Magnetic Materials Each Class Class of Magnetic Material Ex’s: Elements & Compounds Diamagnetic Bi, H, He, NaCl, Au, Cu, Si, Ge, etc. Paramagnetic K, O, etc. Antiferromagnetic MnO, NiO, FeS, CoCl 2, etc. Ferrimagnetic Fe 3 O 4 (iron oxide magnetite), NiFe 2 O 4 (nickel ferrite), etc. Superparamagnetic Ferromagnetic particles in a nonferromagnetic matrix

Qualitative Summary of Magnetic Material Properties Class m orb vs. m spin B int vs. B appl Comments Dia- m orb = -m spin < weak effect Para- m orb +m spin small > weak effect Antiferro- << <<  int. canc. Ferro- << << >> >> Domains! Domains! Ferri- << << > High resist. High resist. Superpara- << << > Matrix Matrix

Applications of Magnetic Materials ► Ferromagnetic Materials: Permanent Magnets, Magnetic Data Storage, etc. ► Ferrimagnetic Materials: Ferrites commonly used for transformer and/or toroid cores due to their higher resistance that reduces eddy currents that cause ohmic loss ► Superparamagnetic: used to create recording tape for audio or video application

Summary ► Forces on moving charge in a magnetic field may result in – Forces on current carrying conductors – Torques on current loops ► Magnetization results from miniature bound current loops of electrons with – Orbital magnetic moments – Spin magnetic moments

Summary ► Different classes of materials exist, some have weaker and some stronger magnetic effects ► The permeability constant (  ) indicates the magnetization and magnetic effects of a linear, isotropic material ► Some ferromagnetic materials have practical nonlinear or anisotropic effects ► Applications of magnetic materials include: permanent magnets, data storage, motors, generators, transformer/toroid cores, etc.