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Mooraj et al. J Mater Inf 2023;3:4 https://dx.doi.org/10.20517/jmi.2022.41 Page 33 of 45

[193]
Figure 16. (A) XRD patterns of (AlCoCrFeNi) Ni . This figure is quoted with permission from Chen et al. , copyright 2018, Elsevier;
100-x x [193]
(B) XRD patterns of (CoCrCuFeNi) Mo . This figure is quoted with permission from Chen et al. , copyright 2018, Elsevier; (C) XRD
100-x x
patterns of 31 samples fabricated by L-DED in the Mo-Ta-Nb-W alloy system. This figure is quoted with permission from Moorehead
[194]
et al. ; (D) XRD patterns of CoCrFeNiNb printed in the authors’ lab.
x
phase shows thinner magnetic stripe domains than the FCC phase, which leads to lower eddy losses as the
BCC phase fraction increases.

Zhang et al. studied the effect of composition and phase fraction in a FeCoNi(CuAl)x alloy system on the
[201]
magnetic and mechanical properties . The general trend from Figure 17B shows that the saturation
magnetization (M ) decreases with increasing Cu and Al content and shows a slight increase from x = 0.8 to
s
x = 0.9. Fe, Co, and Ni are all ferromagnetic elements, while Cu and Al are not, so the authors rationalize the
decrease in M originating from the increase in non-ferromagnetic components. Borkar et al. also studied
s [202]
the effect of the Co/Cr ratio on the microstructure and magnetic properties of AlCo Cr FeNi . Increasing
x 1-x
the Co/Cr ratio leads to increased M as the magnetization depends heavily on the composition, as shown in
s
Figure 17C.