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Chinese Journal of Materials Research  2026, Vol. 40 Issue (7): 481-496    DOI: 10.11901/1005.3093.2025.262
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Optimization of Mechanical Properties and High-pressure Strengthening Mechanism of FeCoNiCuSi x B1 - x High Entropy Alloys
BAO Fangxuan1,2, GONG Minglong1,2(), LIU Enrui1,2, LIU Fengfang2, BAI Jing1,2, GAO Qiuzhi1,2
1.School of Materials Science and Engineering, Northeastern University, Shenyang 110819, China
2.School of Resources and Materials, Northeastern University at Qinhuangdao, Qinhuangdao 066004, China
Cite this article: 

BAO Fangxuan, GONG Minglong, LIU Enrui, LIU Fengfang, BAI Jing, GAO Qiuzhi. Optimization of Mechanical Properties and High-pressure Strengthening Mechanism of FeCoNiCuSi x B1 - x High Entropy Alloys. Chinese Journal of Materials Research, 2026, 40(7): 481-496.

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Abstract  

First-principles calculations were used to investigate the effects of Si content and pressure on the phase structures and mechanical properties of FeCoNiCuSi x B1 - x (x = 0, 0.25, 0.5, 0.75, 1) high entropy alloys. Structural stability was evaluated by calculating relevant parameters based on the multicomponent phase formation criteria for high entropy alloys. The results show that the alloys exhibit a multiphase structure consisting of an FCC solid solution and intermetallic compounds. With increasing Si content, the FeCoNiCuSi x B1 - x high entropy alloys exhibit increased lattice constants, decreased density, and reduced elastic moduli (B, G, and E). The B/G ratio and Poisson's ratio initially decrease and then increase, indicating that the ductility initially decreases and subsequently improves with increasing Si content, while high Si contents reduce the tendency toward brittle fracture. Heat of formation analysis reveals that Si enhances the thermodynamic stability of the alloy system. Under pressures ranging from 0 to 100 GPa, FeCoNiCuSi0.5B0.5 high entropy alloy exhibits a reduced lattice constant, increased density, enhanced deformation resistance, and weakened pressure-induced elastic anisotropy approaching isotropic behavior. The yield strength increases with increasing pressure, and the alloy exhibits excellent comprehensive mechanical properties.

Key words:  metallic materials      high entropy alloy      first-principles      pressure      crystal structure      mechanical properties     
Received:  28 August 2025     
ZTFLH:  TG139  
Fund: National Natural Science Foundation of China(52471004)
Corresponding Authors:  GONG Minglong, Tel: 15230357760, E-mail: gongminglong@qhd.neu.edu.cn

URL: 

https://www.cjmr.org/EN/10.11901/1005.3093.2025.262     OR     https://www.cjmr.org/EN/Y2026/V40/I7/481

Fig.1  Structural model of FeCoNiCuSi x B1 - x high entropy alloys was constructed based on the VCA method (a) conventional modeling, (b) virtual crystal approximation method modeling
AlloysFeCoNiCuSiB
x = 0111101
x = 0.2511110.250.75
x = 0.511110.50.5
x = 0.7511110.750.25
x = 1111110
Table 1  Composition design of FeCoNiCuSi x B1 - x high entropy alloys
Fig.2  Convergence test of FeCoNiCuSi x B1 - x high entropy alloys (a) energy cutoff, (b) k-point
Alloysδ / %ΔSmix / J·K-1·mol-1ΔHmix / kJ·mol-1ΩΔχ / %VECγ
x = 014.8913.38-8.642.796.9698.21.575
x = 0.2513.0514.32-11.382.236.3218.251.571
x = 0.510.8414.53-13.841.825.518.31.566
x = 0.757.9714.32-16.021.524.4498.351.562
x = 12.9213.38-17.921.252.8718.41.101
Table 2  Phase formation determination parameters of FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents
Fig.3  Lattice constant and density in FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents
Fig.4  Ground-state total energy and heat of formation of FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents
AlloysC11Variation / %C12Variation / %C44Variation / %C11-C12C11+2C12
x = 01372.90688.20244.60684.72749.3
x = 0.251302.8-5.10647.5-5.92236.1-3.47655.32597.8
x = 0.51200-12.59589.2-14.39229.7-6.09610.82378.4
x = 0.751074.8-21.71555.5-19.28197.9-19.09519.32185.8
x = 1927.9-32.41542.4-21.20134.7-44.93385.52012.7
Table 3  Elastic constants (Cij, GPa) and their variation percentage in FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents
Fig.5  Elastic modulus and dislocation strain energy of FeCoNiCuSi x B1 - x high entropy alloys at different Si contents (a) elastic modulus, (b) strain energy per unit length of a single dislocation
AlloysBV/ GPaBR/ GPaBH/ GPaGV/ GPaGR/ GPaGH/ GPa
x = 0916.4916.4916.4283.7276.1279.9
x = 0.25866866866272.7265.8269.2
x = 0.5792.8792.8792.8260255257.5
x = 0.75728.6728.6728.6222.6218.7220.6
x = 1670.9670.9670.9157.9153.1155.5
Table 4  Bulk modulus B and shear modulus G of FeCoNiCuSi x B1 - x high entropy alloys calculated via VRH approximation with varying Si contents
AlloysC12-C44 / GPaνB/GHardness / GPaYield strength / GPa
x = 0443.60.3613.2712.94.3
x = 0.25411.40.3593.2212.814.27
x = 0.5359.50.3533.0813.044.35
x = 0.75357.60.3623.310.83.6
x = 1407.70.3924.316.222.07
Table 5  Cauchy pressure, Poisson's ratio ν, B/G, Hardness (Tian2012), and Yield strength of FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents
AlloysAUAGAZ
x = 00.1380.0140.714
x = 0.250.130.0130.721
x = 0.50.0980.010.752
x = 0.750.0890.0090.762
x = 10.1570.0150.699
Table 6  Anisotropy coefficients (AZ, AG, AU) of FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents
Fig.6  Three-dimensional surface plot of Young's modulus for FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents (a) x = 0, (b) x = 0.25, (c) x = 0.5, (d) x = 0.75, (e) x = 1
Fig.7  Energy factor K of FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents (a) screw dislocation (KScrew) and edge dislocation (Kedge), (b) mixed dislocation (Kmixed)
Fig.8  Total density of states of the FeCoNiCuSi x B1 - x high entropy alloys with varying Si contents
Fig.9  Lattice constant and density of FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures
Fig.10  Ground-state total energy and heat of formation of FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures
Pressure / GPaC11Variation / %C12Variation / %C44Variation / %C11-C12C11+2C12
012000589.20229.70610.82378.4
201309.39.11657.311.56261.914.026522623.9
401429.419.12739.225.46293.927.95690.22907.8
601528.927.41804.836.5932441.05724.13138.5
801647.137.26889.550.97353.453.85757.63426.1
1001742.245.18952.861.71381.966.26789.43647.8
Table 7  Elastic constants (Cij, GPa) and their variation percentages (%) in FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures
Fig.11  Elastic modulus and dislocation strain energy of FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures (a) elastic modulus, (b) strain energy per unit length of a single dislocation
Pressure / GPaBV / GPaBR / GPaBH / GPaGV / GPaGR / GPaGH / GPa
0792.8792.8792.8260255257.5
20874.6874.6874.6287.6284.3285.9
40969.3969.3969.3314.4312.4313.4
601046.21046.21046.2339.2338.2338.7
801142.01142.01142.0363.6363.1363.4
1001215.91215.91215.9387386.9387
Table 8  Bulk modulus B and Shear modulus G of FeCoNiCuSi0.5B0.5 high entropy alloy calculated via VRH approximation under different pressures
Pressure / GPaC12-C44 / GPaνB/GHardness / GPaYield strength / GPa
0359.50.35353.07913.044.35
20395.350.35263.05914.154.72
40445.320.35413.09314.914.97
60480.830.35393.08915.785.26
80536.070.35623.14316.265.42
100570.910.35613.142175.67
Table 9  Cauchy pressure, Poisson's ratio ν, B/G, Hardness (Tian2012), and Yield strength of FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures
Pressure / GPaAUAGAZ
00.0980.00970.7521
200.0580.00570.8034
400.0310.00310.8514
600.0150.00150.8950
800.00580.000570.9330
1000.001310.000130.9674
Table 10  Anisotropy coefficients (AU, AG, AZ) of FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures
Fig.12  Three-dimensional surface plot of Young's modulus for FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures (a) x = 0 GPa, (b) x = 20 GPa, (c) x = 40 GPa, (d) x = 60 GPa, (e) x = 80 GPa, (f) x = 100 GPa
Fig.13  Energy factor K of FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures (a) screw dislocation (KScrew) and edge dislocation (Kedge), (b) mixed dislocation (Kmixed)
Fig.14  Total density of states of the FeCoNiCuSi0.5B0.5 high entropy alloy under different pressures
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