Download Handbook of Magnetic Materials, Volume Volume 2 (Handbook on by E.P. Wohlfarth PDF

By E.P. Wohlfarth

The instruction manual of Magnetic fabrics has a twin objective; as a textbook, it offers an creation to a given subject inside of magnetism, and as a piece of reference, it serves scientists lively in magnetism learn. to meet those pursuits, every one bankruptcy within the guide is written by way of prime professionals within the box, and combines state of the art examine effects with an in depth compilation of archival wisdom. Magnetism is a quickly increasing box which continuously maintains to surround new phenomena. Examples of such subfields of magnetism are quadrupolar interactions, magnetic superconductors, and quasiscrystals: subject matters which are all coated within the current quantity. the single universal floor among those new fabrics and ferromagnets, is the ownership of a magnetic second; the sequence identify has been a bit adjusted to mirror this. yet in response to culture, the instruction manual of Magnetic fabrics maintains to permit readers to acquaint themselves in nice intensity with themes in the course of the whole breadth of magnetism study.

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Extra resources for Handbook of Magnetic Materials, Volume Volume 2 (Handbook on Ferromagnetic Materials)

Example text

U. 8 X Fig. 19. Effective moment per Fe 3+ ion in (1) tetrahedral sites for {Y3_xCax}[Fe2_xZrx](Fe3)Oi2 system; in (2) tetrahedral sites for {Y3}[Fe2-xScx](Fe3)Oi2 system; in (3) tetrahedrai sites for {Y3}[Fe2-xMgx](Fe3-xSix)Oi2 system; in (4) octahedral sites for {Y3-xCax}[Fe2l(Fe3-xSix)On system. 3-xSix)Oi2 specimens (Geller et al. 1964a). opposite lattice above a certain value. The cause for the decrease in effective moment is the canting of the Fe 3÷ ion moments in the lattice as a consequence of the antiferromagnetic interaction between ions in the same lattice.

2. Iron-~,ilicon phase diagram . . . . . . . . . . 3. Physical avd trechanical properties . . . . . . . . 4. netic properties . . . . . . . . . . 5. Magnetic ploperties contlol, core loss . . . . . . . . 6. N e w high J'nducticn crier_ted materials . . . . . . . . 7. Olher iron-silicon alloy ( e v e l o p m e n t s . . . . . . . . 8. Core loss limits of electrical steel . . . . . . . . . 4. I r o n - a l u m i n u m avd iron-aluminum-silicon alloys .

Geller et al. tB per ion. Again the anisotropy introduced by Pr 3÷ is very high a n d M z = L - 2 S = 3 txB (table 9) so that the orbital contribution (L = 5) to the moment has been substantially reduced by the crystalline surroundings. 45. (Loriers and Villers 1961, unpublished work of Gilleo referred to in Geller et al. 1962; Espinosa 1962) because of the very large size of La 3+ in comparison with y3+. There is no effect on the magnetic moment at T = 0 K (Geller et al. 1963a). FERROMAGNETIC INSULATORS; GARNETS 33 c.

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