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Magnetism Nomenclature

Transport Phenomena in Microfluidic Systems, First Edition. Pradipta Kumar Panigrahi. [Pg.277]

The magnetization (M) of a block of ferromagnetic material is initially zero when the material is not magnetized. The application of external magnetic field (//e t) leads to a net [Pg.278]


Nomenclature. The calihration between the magnetic and the stripping methods can be determined through the model... [Pg.502]

Figure 9.2 Magnetic entropy versus temperature for a hypothetical paramagnet at two distinct magnetic fields. Hf represents the final field and the initial, although this nomenclature is arbitrary and there is... Figure 9.2 Magnetic entropy versus temperature for a hypothetical paramagnet at two distinct magnetic fields. Hf represents the final field and the initial, although this nomenclature is arbitrary and there is...
Fig. 5 Membrane models for NMR structure analysis, (a) An isotropic detergent micelle (left) is compared to the dimensions of lipid bilayers (right), (b) Macroscopically oriented membrane samples can be prepared on solid support, as nanodiscs, or as magnetically oriented bicelles. (c) Nomenclature and variability of liposomes small (SUV, 20-40 nm), intermediate (IUV, 40-60 nm), large (LUV, 100-400 nm), and giant unilamellar vesicles (GUV, 1 pm) multi-lamellar (MLV), oligo-lamellar (OLV) and highly heterogeneous multi-oligo-lamellar vesicles (MOLV)... Fig. 5 Membrane models for NMR structure analysis, (a) An isotropic detergent micelle (left) is compared to the dimensions of lipid bilayers (right), (b) Macroscopically oriented membrane samples can be prepared on solid support, as nanodiscs, or as magnetically oriented bicelles. (c) Nomenclature and variability of liposomes small (SUV, 20-40 nm), intermediate (IUV, 40-60 nm), large (LUV, 100-400 nm), and giant unilamellar vesicles (GUV, 1 pm) multi-lamellar (MLV), oligo-lamellar (OLV) and highly heterogeneous multi-oligo-lamellar vesicles (MOLV)...
A brief review is given here of the spectroscopic vector model of an atom or ion. In crystal-field theory, the wave function of the isolated ion is taken as the unperturbed state, and the perturbing effect of the electric and magnetic fields is computed. Thus crystal field theory uses the language, nomenclature, and methods employed in the theory of atomic spectra. A complete discussion of these methods can be found in books by Condon and Shortley (5) and by Griffith (/). [Pg.100]


See other pages where Magnetism Nomenclature is mentioned: [Pg.277]    [Pg.277]    [Pg.174]    [Pg.1279]    [Pg.458]    [Pg.760]    [Pg.887]    [Pg.888]    [Pg.236]    [Pg.176]    [Pg.1030]    [Pg.143]    [Pg.14]    [Pg.315]    [Pg.212]    [Pg.43]    [Pg.703]    [Pg.462]    [Pg.30]    [Pg.2]   


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