Submitted:
29 April 2024
Posted:
30 April 2024
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Abstract
Keywords:
1. Introduction
2. Trends and Development of New Copper Alloys for Sliding Applications
3. Overview on Recent Copper Materials for Sliding Applications


4. CuAl8Fe5Ni4Zn4Sn1 as a New Lead-Free Copper Alloy for Sliding Applications
5. Strengthening Mechanisms of CuAl8Fe5Ni4Zn4Sn1
5.1. Initial Condition after Continuous Casting
- CuAl8Fe5Ni4Zn4Sn1 is a polymorph alloy with β-phase during solidification, which transforms into α- and κ-phases during cooling to room temperature. In such an alloy the solid-solid phase transformation during cooling after solidification has an additional impact on grain refinement. This is because from each mother grain there can result a plurality of daughter grains. The same behaviour can be observed in other polymorph copper alloys such as α/β brass [15].
- The iron content further contributes to the refinement of the microstructures. This effect is related to the iron, which is in solid solution in the copper matrix, as this proportion supports nucleation [20].
- The forementioned aspects count for other bronze alloys such as CuAl10Ni5Fe4 as well. Notwithstanding that, as-cast CuAl10Ni5Fe4 provides also fine grains, but a dendritic grain morphology. In comparison, CuAl8Fe5Ni4Zn4Sn1 does not only provide fine, but also globular microstructures. Therefore, further differences in the chemical compositions must be the reason for the globular microstructures of CuAl8Fe5Ni4Zn4Sn1;
- Most likely, the globular microstructures of CuAl8Fe5Ni4Zn4Sn1 can be explained by the effect of tin which is reported to shift the grain morphology of aluminium bronze to globulitic. This is due to the decline in nucleation temperatures, the reduction in undercooling intensity, and the decrease in cooling rate during solidification [21].
5.2. Hot Extrusion of Tubes
5.3. Effect of Cold Drawing and Straightening of the Extruded Tubes
5.4. Thermal Treatment after Cold Drawing of CuAl8Fe5Ni4Zn4Sn1
- Due to the friction between the tool surface and the tube material there occurs shear deformation in the near surface zones of the tube material;
- Furthermore, being surrounded by the neighbouring material in all directions this results in a triaxial stress state of the core, but the stress state near the tube surface is nearly plain;
- Bothe forementioned friction and adiabatic heating leads to increasing temperatures in the tube material. Therefore, also the temperature distribution in the tube cross section is inhomogeneous.
6. Summary
7. Outlook
Funding
Conflicts of Interest
References
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| Cu | Zn | Pb | Sn | Fe | Mn | Ni | Al | |
|---|---|---|---|---|---|---|---|---|
| Min | balance | 3.0 | - | 0.5 | 3.5 | - | 3.0 | 7.0 |
| Max | - | 5.0 | 0.1 | 2.0 | 5.5 | 0.5 | 5.0 | 9.0 |
| Mechanical property | Unit | Requirement* |
|---|---|---|
| 0.2%-Yield strength | MPa | Minimum 500 |
| Tensile strength | MPa | Minimum 700 |
| Elongation at break | % | Minimum 5 |
| Hardness Brinell | HBW | 210 |
| Bending fatigue strength | MPa | ~ 220 to 230 |
| Cu | Zn | Sn | Fe | Ni | Al | |
|---|---|---|---|---|---|---|
| Matrix | 74 | 4 | 1 | 3 | 3 | 15 |
| Coarse particles (centre) | 16 | 0 | 0 | 50 | 14 | 20 |
| Coarse particles (outer edge) | 32 | 0 | 0 | 14 | 22 | 32 |
| Coarse precipitations (Fe rich) | 13 | 0 | 0 | 47 | 14 | 26 |
| Coarse precipitations (Ni rich) | 50 | 3 | 0 | 19 | 22 | 6 |
| Fine precipitations (Fe rich) | 67 | 0 | 0 | 23 | 10 | 0 |
| Fine precipitations (Ni rich) | 83 | 5 | 0 | 3 | 5 | 4 |
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