magnetocrystalline anisotropy वाक्य
उदाहरण वाक्य
मोबाइल
- The magnetocrystalline anisotropy parameters have a strong dependence on temperature.
- The spin orbit interaction is one cause of magnetocrystalline anisotropy.
- This applies to a particle with uniaxial magnetocrystalline anisotropy.
- The expression omits magnetocrystalline anisotropy, which is unaffected by the presence of the antiferromagnet.
- There are several kinds of magnetic anisotropy, the most common of which is magnetocrystalline anisotropy.
- Due to its chemical composition and crystallographic structure Sendust exhibits simultaneously zero magnetostriction and zero magnetocrystalline anisotropy constant K 1.
- The magnetocrystalline anisotropy parameters are generally defined for ferromagnets that are constrained to remain undeformed as the direction of magnetization changes.
- To keep the lattice from deforming, a single domain ( uniformly magnetized ), the effect is to change the magnetocrystalline anisotropy parameters.
- Changing the magnetization of the material to any other direction takes additional energy, called the " " magnetocrystalline anisotropy energy " ".
- An isotropic point also occurs near the Verwey transition around 130 K, at which point the sign of the magnetocrystalline anisotropy constant changes from positive to negative.
- The magnetocrystalline anisotropy energy of a ferromagnetic crystal can be expressed as a power series of direction cosines of the magnetic moment with respect to the crystal axes.
- The Verwey transition is associated with, but distinct from, a magnetic isotropic point in magnetite, at which the first magnetocrystalline anisotropy constant changes sign from positive to negative.
- Desirable properties for an exchange bias material include a high N�el temperature, a large magnetocrystalline anisotropy and good chemical and structural compatibility with NiFe and Co, the most important ferromagnetic films.
- So flux closure domains will only form where the magnetostatic energy saved is greater than the sum of the " exchange energy " to create the domain wall, the magnetocrystalline anisotropy energy, and the magnetoelastic anisotropy energy.
- Some sources define a wall energy " E W " equal to the sum of the exchange energy and the magnetocrystalline anisotropy energy, which replaces " E ex " and " E k " in the above equation.
- The width of the domain wall varies due to the two opposing energies that create it : the magnetocrystalline anisotropy energy and the exchange energy ( J _ { \ mathrm { ex } } ), both of which tend to be as low as possible so as to be in a more favorable energetic state.
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