Technical Notes - Precipitation and Diffuse Scattering in an Fe-Mo-Co Alloy

The American Institute of Mining, Metallurgical, and Petroleum Engineers
A. H. Geisler F. E. Steigert
Organization:
The American Institute of Mining, Metallurgical, and Petroleum Engineers
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2
File Size:
139 KB
Publication Date:
Jan 1, 1952

Abstract

THE permanent magnet alloy comol, which contains 17 pct Mo, 12 pct Co, balance Fe, exhibits a precipitation reaction analogous to that at the iron end of the binary Fe-Mo system. The equilibrium precipitate, (P,), has a structure isomorphous with Fe,Mo, which is rhombohedra1 with parameters a = 8.97A and a = 3038.6&apos; according to the work of Arnfelt and Westgren.&apos; In the ternary alloy the parameters are a = 8.87A and a = 31°0.5&apos;. Oscillating crystal patterns of a single matrix crystal, M, in which P, was precipitated by slow cooling from 1300°C, showed that the orientation relationship of the two lattices is as follows: (110)P3 // (110)* (111)p3 // (110)m There are crystallites of P, in 12 different orientations in a single crystal of the parent solid solution. Microscopic examination shows that the crystallites are generally plate-like with their lateral dimensions parallel to (110) matrix planes. When precipitation in a supersaturated alloy quenched from 1300°C progressed isothermally at temperatures between 600" to 800°C, the evolution of the P, structure could be traced. Diffuse diffraction effects in Laue patterns provided early evidence of the precipitation process. Analyses of these by a previously described technique2 showed that they corresponded to rod-like elements parallel to <110> matrix directions in reciprocal space. With further aging to promote growth of the precipitate, the rod-like elements contracted to points in reciprocal space for normal Bragg reflection from the precipitate as shown by the left diagram in Fig. 1. Thus the diffuse scattering was attributed to the small thickness of the plate-like particles which was inadequate for sharp diffraction. When the precipitate particles were first thick enough to give normal diffraction their structure was different from that of the equilibrium precipitate, P,. The first structure, P1, presumably is a coherent transition struc-
Citation

APA: A. H. Geisler F. E. Steigert  (1952)  Technical Notes - Precipitation and Diffuse Scattering in an Fe-Mo-Co Alloy

MLA: A. H. Geisler F. E. Steigert Technical Notes - Precipitation and Diffuse Scattering in an Fe-Mo-Co Alloy. The American Institute of Mining, Metallurgical, and Petroleum Engineers, 1952.

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