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Domain walls Subject

The rare earth-cohalt magnets are discussed here with a fairly applied bias. Relevant fundamental subjects are treated exhaustively elsewhere in this handbook series basic magnetic properties of the RE-elements by Legvold (1980), those of RE-TM intermetallics by Buschow (1980), and the theory of hard-magnetic behavior - small-particle magnetization reversal, domain-wall nucleation and motion, and the role of anisotropy in these - by Zijlstra (1982). Buschow (1988) discusses the various mechanisms thought to be controlling the coercivity in all REPM, and the... [Pg.135]

Many of the specific applications of ferrites depend on their behaviour at high frequencies. When subjected to an ac field, ferrite permeability shows several dispersions as the field frequency increases, the various magnetisation mechanisms become unable to follow the field. The dispersion frequency for each mechanism is different, since they have different time constants. Fig. 4.59. The low-frequency dispersions are associated with domain wall dynamics and the high-frequency dispersion, with spin resonance the latter, usually in the GHz range, is discussed in Section 4.6.2. [Pg.173]

At very high frequencies, domain walls are unable to follow the field and the only remaining magnetisation mechanism is spin rotation within domains. This mechanism eventually also shows a dispersion, which always takes the form of a resonance. Spins are subjected to the anisotropy field, representing spin-lattice coupling as an external field is applied (out of the spins easy direction), spins experience a torque. However, the response of spins is not instantaneous spins precess around the field direction for a certain time (the relaxation time, r) before adopting the new orientation. Fig. 4.62. The frequency of this precession is given by the Larmor frequency ... [Pg.177]

The discussion concerning the domination of the domain wall-clamping mechanisms in bulk ferroelectrics has been the subject of several reports [51-55, 65, 66, 73, 78] since the discovery of ferroelectric aging, and still remains an open question. Recently, it has been shown by calculations [77] that the clamping pressure exerted by oriented defect dipoles in a 1-D model is two to three orders of magnitude weaker than that exerted by the same amount of charges accumulated on grain boundaries. [Pg.744]

The spontaneous strain ( t i2)s may be reversed, as discussed earlier, with fig. 30.17, by applying a compressional stress along the orthorhombic h-axis. At very small applied stress, the crystal responds with a small elastic deformation until the critical threshold stress (to) is exceeded at which time domain walls nucleate and move until the region subjected to the stress has been switched to the opposite strain state. Decreasing this applied stress to zero leaves the crystal in the positive , Xs spontaneous strain state. [Pg.642]

CoWsider a plane wall of thickness 2L initially at a uniform temperature of T , as shown in Fig. 4—1 In. At lime t = 0, the wall is immersed in a fluid at temperature 7 and is subjected to convection heal transfer from both sides with a convection coefficient of h. The height and the widlh of the wall are large relative to its thickness, and thus heat conduction in the wall can be approximated to be one-dimensional. Also, there is thermal symmetry about the inidplane passing through.x = 0, and thus the temperature distribution must be symmetrical about tlie midplane. Therefore, the value of temperature at any -.T value in - A "S. t 0 at any time t must be equal to the value at f-.r in 0 X Z, at the same time. This means we can formulate and solve the heat conduction problem in the positive half domain O x L, and then apply the solution to the other half. [Pg.244]

Many pressure vessels used for isostatic pressing must be classified as thick walled . The literature on this subject is considerable but, unfortunately, in many countries rules for minimum requirements of design, fabrication, operation, inspection, and certification of such vessels is lacking. Design and fabrication are very much in the domain of specialists who rely to a great extent on past experience. [Pg.343]


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