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Magnetic stiffness

The rotordynamic study of a machine with magnetic bearings is quite different from the one of either oil-film or rolling-element bearings. The stiffness and damping properties of magnetic bearings can... [Pg.2535]

Improved rotor dynamic stability. The active magnetic bearing s ability to vary stiffness and damping permits rotation about the rotor s inertial axis, eliminating vibration and noise. [Pg.333]

T. E. Oliphant, A. Manduca, R. L. Ehman and J. F. Greenleaf, Complex-valued stiffness reconstruction for magnetic resonance elastography by algebraic inversion of the differential equation, Magn. Reson. Med., 2001, 45, 299-310. [Pg.241]

By using two traps, it is possible to maintain a constant force [91]. This is also possible with magnetic tweezers. However, because of the low stiffness of the magnetic trap, the spatial resolution due to thermal flucmations is limited to a few tens of nanometers. [Pg.68]

Aromatic ring currents[45, 46] or the charge stiffness[47] provide a related application of correction vectors, now associated with magnetic fields. Ring currents are the diamagnetic susceptibility of 4n+2 systems. The correction vector in monocycles is obtained from... [Pg.657]

Figure 3. Exchange energy as a function of the wave vector of the magnetization inhomogenity Lindhard function (solid line) and exchange-stiffness or continuum approximation (dashed line). For late 3d elements (Cu), k/2kf = 1 corresponds to modulation wavelength of 0.23 nm... Figure 3. Exchange energy as a function of the wave vector of the magnetization inhomogenity Lindhard function (solid line) and exchange-stiffness or continuum approximation (dashed line). For late 3d elements (Cu), k/2kf = 1 corresponds to modulation wavelength of 0.23 nm...
In noncubic materials, A must be replaced by the 3x3 exchange-stiffness tensor A v, and the energy is X J A v dM/dxy dM/dxv dV. Here the indices ju and v denote the spatial coordinates x, y, and z of the bonds. The energy is anisotropic with respect to the nabla operator = d/d (bond anisotropy) but isotropic with respect to the magnetization M. By contrast, the relativistic anisotropic exchange Xa i Ha(i VMa VMP dV is isotropic with respect to V but anisotropic with respect to M. [Pg.48]

Here Ms(r) is the spontaneous magnetization, A)(r) is the first uniaxial anisotropy constant, A(r) denotes the exchange stiffness, and n(r) is the unit vector of the local anisotropy direction. H is the external magnetic field, and Hd is the magnetostatic self-interaction field. The latter can be written as... [Pg.58]


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