Elsevier

Intermetallics

Volume 136, September 2021, 107256
Intermetallics

Crystallization mechanism of Zr55Cu30Al10Ni5 metallic glass in an extended range of heating rates

https://doi.org/10.1016/j.intermet.2021.107256Get rights and content

Highlights

  • The crystallization of Zr55 BMGs during non-isothermal heating process is analyzed.

  • The crystallization morphologies are different after slow and rapid heating.

  • The numerical model is established to describe the fast crystallization during SLM.

  • The activation energy of dendritic and nanocrystallization is separately calculated.

Abstract

The crystallization mechanisms of Zr55Cu30Al10Ni5 (Zr55) amorphous alloys from slow continuous heating to rapid laser heating are investigated. The multiphase nanocrystalline structures such as CuZr2-type, NiZr2-type and Al2Zr3-type phases with various compositions are observed at heating rates lower than 50 K/s, while the CuZr2-type/ZrCu-type eutectic dendrites are produced at heating rates higher than 50 K/s. A numerical model is established to calculate the onset crystallization temperatures as a function of the heating rates. This model indicates that in addition to rapid dendritic growth from a certain number of quenched-in nuclei, the non-Arrhenius behavior of high diffusion coefficient in the supercooled liquid region contribute to the serious crystallization during rapid heating process. The activation energy of dendritic crystallization is obviously smaller than that of multiphase nanocrystallization, which is due to a much smaller scale of diffusion distance and larger atomic diffusivity during dendritic growth.

Introduction

Bulk metallic glasses (BMGs) have been considered as potential structural materials in engineering fields due to their unique properties associated with disordering atomic structure [[1], [2], [3]]. However, the widespread applications of BMGs are constrained by the critical size limitation of the as-cast BMGs prepared by conventional copper mold casting method [4]. In recent years, selective laser melting (SLM) and laser direct manufacturing (LDM) techniques have attracted tremendous attentions in fabricating BMGs owning to their advantages on manufacturing the complex BMGs components without size limitation [[5], [6], [7]]. For instance, SLM technique has been introduced to fabricate various BMGs and BMGs composites [[8], [9], [10], [11]].

During SLM of Zr55Cu30Al10Ni5 (Zr55) metallic glass, the amorphous remelted zone (RZ) of the already-deposited layer kept the amorphous state [12], while a certain degree of crystallization still occurred in the heat affected zone (HAZ). The repeated reheating annealing/tempering treatment on the already-deposited amorphous layers during subsequent deposition led to the crystallization of HAZ. It had been demonstrated that the micro-scale coarse dendrites on the top of HAZ were formed upon rapid heating process [13]. In contrast, the nanocrystals were usually observed following non-isothermal and isothermal crystallization of BMGs upon slow heating process by using DSC [[14], [15], [16]]. Thus, the crystallization behaviors of BMGs during the rapid heating process and slow heating process are obviously different. H. Sun et al. revealed that the crystallization of HAZ was dominated by the rapid spherulitic growth from pre-existing nuclei, and they constructed a numerical model to calculate the spherulitic growth rate during LDM of a ZrCuNiAlNb metallic glass [17]. Here, the kinetic coefficient for crystal growth ukin was obtained from the measurements of the viscosity η if the Stokes-Einstein (S-E) relation was invoked [18]. However, the S-E relation which links the viscosity η and the effective diffusion coefficient D broke down in the supercooled liquids for some cases, such as a Ni-Ti [19], Cu–Zr and Ni–Zr glass-forming alloys [20]. Thus, it is still unclear whether the calculation of dendritic growth rate during SLM depends on the S-E relationship. The numerical model used to describe the fast crystallization of HAZ needs to be reestablished.

In general, the RZ of the already-deposited layer will experience the reciprocating non-isothermal annealing treatment during SLM, and the temperature values corresponding to the maximum nucleation rate and maximum growth rate of crystals are different. Therefore, the crystallization mechanism of BMGs is considered to be strongly dependent on thermal history. In this work, the crystallization characteristics of Zr55 BMGs under a wide range of non-isothermal heating process at the heating rates from lower than 30 K/s to about 104 K/s are discussed. The formation mechanism of dendrite in the HAZ is theoretically analyzed, which will lay a theoretical foundation for accurately control the crystallization of HAZ during SLM of Zr55 BMGs.

Section snippets

Experimental procedures

Amorphous plates of Zr55Cu30Al10Ni5 (nominal at. %) with a size of 60 × 12 × 2 mm3 were produced by vacuum arc melting the high purity elemental constituents and homogenizing at least three times in the melting chamber, and then casting into a Cu mold under high purity argon atmosphere. The as-cast amorphous samples with dimensions of 3 × 3 × 0.5 mm3 were heated to 900 K at heating rates ranging from 0.17 K/s to 3.33 K/s using MettlerToledo differential scanning calorimeter (DSC). The value of

Results

Fig. 1 shows the XRD diffraction patterns of the Zr55 amorphous samples heated at constant rates ranging from 0.5 K/s to ~104 K/s. Compared with the broad diffuse scattering peak for the as-cast amorphous plate, multiple sharp crystallization peaks can be observed for the samples. The crystals produced at slow heating rates of 0.5–30 K/s have similar crystalline structures, which is composed of NiZr2-type, Al2Zr3-type and CuZr2-type phases. However, the structures formed at rapid heating rates

Discussion

Above microstructural investigation shows that the crystal structure of dendrites in the SLMed and Gleeble-heated samples is markedly different from that of the nanocrystals in the DSC-heated samples. The multiphase nanocrystals with different compositions and structures are observed distributed homogeneously throughout DSC-heated samples, while the micro-sale eutectic dendrites are found within the amorphous matrix of Gleeble-heated and SLMed samples. The growth of ZrCu-type dendrites occurs

Conclusions

  • (1)

    The obvious microstructural difference is observed between the crystallization in the low and high heating treatments. The nanocrystalline phases such as CuZr2-type, NiZr2-type and Al2Zr3-type with various compositions are observed at heating rates lower than 50 K/s. While micro-scale eutectic dendrites are examined at heating rates higher than 50 K/s.

  • (2)

    The numerical models constructed by the S-E relation and Ediger relation are suitable to describe the nanocrystallization and the dendritic

Declaration of competing interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

This work was supported by the Scientific Research Plan Projects of Shaanxi Education Department (Grant No. 20JK0657), the Natural Science Foundation of Shaanxi Province (Grant No. 2020JQ-824) and the National Natural Science Foundation of China (Grant No. 52001244).

References (38)

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