SAE AS5491C
SAE AS5491C 2007-NOV-01 Calculaton of Electron Vacancy Number n Superalloys
Purpose
This SAE Aerospace Standard (AS) establishes a uniform procedure for calculation of electron vacancy numbers in superalloys. It is intended for use by suppliers of raw materials and parts, typically castings, for which control of electron vacancy number is required by the raw material specification.
Application
This procedure has been used to estimate the potential for alloy phase instability by calculation of the density of electrons per atom in nickel-based superalloys.
Background
Complex, highly alloyed superalloys have been observed, for some alloy chemistries and under certain conditions, to form precipitated phases which can adversely affect strength and ductility. These phases, typically of a crystalline structure known as topologically close-packed, or TCP, appear after extended exposure at temperatures in the range from 1300 to 1650 °F (704 to 899 °C). Such phases include sigma (s), mu (µ), or Laves. Their tendency to precipitate from the alloy matrix has been related by researchers such as Boesch and Slaney (see 2.1) and Woodyatt, et al. (see 2.2) to the density of electrons per atom as expressed by the electron vacancy number Nv
where:
Nv is the electron vacancy number for the alloy
mi is the atomic mass fraction of the ith element in the alloy composition, and
(Nv)i is the electron vacancy number of the ith element.
Determination of the electron vacancy concentration requires an understanding of the phases which precipitate in superalloys as well as the sequence in which they form in the gamma matrix. In general, this sequence is (a) the precipitation of borides, (b) the precipitation of carbides, and (c) the formation of gamma prime. When these phase reactions are considered, and adjustments made to the composition to take them into account, the residual matrix composition may be determined. From that residual matrix the electron vacancy number is then calculated.
The sequence of precipitation of strengthening phases is addressed as follows:
Nickel, chromium, titanium, and molybdenum form a boride as (Mo0.5, Ti0.15, Cr0.25, Ni0.10)3B2.
All carbon is assumed to form carbides of the type MC and M23C6. It is assumed that MC carbides take half the carbon, reacting in sequence with tantalum, columbium, zirconium, titanium, and vanadium. The remaining carbon then reacts with chromium, molybdenum, and tungsten to form Cr21(Mo,W)2C6.
Gamma prime is formed from the remaining aluminum, titanium, hafnium, columbium, tantalum, 50 percent of the original amount of vanadium, and 3 percent of the original amount of chromium by combining with three times that total in nickel, i.e., Ni3 (Al, Ti, Cb, Hf, Ta, 0.5V, 0.03Cr).
The remaining chromium content is adjusted for that lost due to formation of borides, carbides, and gamma prime.
The remaining nickel content is adjusted for that tied up in boride and gamma prime formation.