Full Length ArticleMastering a 1.2 K hysteresis for martensitic para-ferromagnetic partial transformation in Ni-Mn(Cu)-Ga magnetocaloric material via binder jet 3D printing
Graphical abstract
Introduction
Worldwide energy consumption is increasing, and a large portion of this growth is generated by cooling technologies such as refrigerators and air conditioners [1]. Currently, refrigeration is produced through a vapor-compression cycle technology that has a maximum Carnot efficiency of 30–40 %, can be loud, and uses chlorofluorocarbons (CFC’s) and hydrochlorofluorocarbons (HCFC’s), hazardous gases which contribute to ozone depletion [2,3]. Recently, the possibility of using solid state magnetic refrigeration, based on the magnetocaloric effect (MCE), has been proposed as an alternative technology. Magnetic refrigeration presents several advantages compared to the vapor-compression cycle: it can be 20–30 % more efficient than the current technology, it is nearly silent because of the limited need for moving parts like the compressor in a typical system, and it is eco-friendly [2]. Nevertheless, many of the established MCE materials contain rare earth elements, such as Gd and La, which are economically strategic materials, and also present potential health risks to populations near to their mining sites and other occupational exposures [4,5].
Recently, two categories of the rare-earth-free Ni-Mn-based (In, Sn, Sb, Ga) Heusler-type magnetic shape memory alloys (SMAs), exhibiting a giant MCE due to the first order martensitic transformation (MT) near room temperature, have been researched: Mn-rich Ni-Mn-(In, Sn, Sb) metamagnetic SMAs (MetaMSMA) [[6], [7], [8], [9]] and Ni-Mn-Ga ferromagnetic SMAs (FSMAs) [10]. MetaMSMAs display a large drop of magnetisation (ΔM) in the temperature range of MT from the high-temperature ferromagnetic austenite to the low-temperature antiferromagnetic martensite, whereas in FSMAs the large drop of ΔM is obtained as a result of MT from the ferromagnetic martensite to the paramagnetic austenite. The adiabatically applied magnetic field induces these magnetostructural transformations producing cooling of MetaMSMAs, as a result of inverse MCE, and heating in the case of FSMAs resulting from a conventional MCE. The large values of the field-induced isothermal entropy change (ΔSm) and corresponding adiabatic temperature change (ΔTad) are the main parameters characterizing the MCE.
On the other hand, the typically large thermal hysteresis of MT (around 10 K) is a serious disadvantage of these materials since a very high magnetic field is required to achieve reversibility of a magnetostructural transformation [[11], [12], [13]]. Therefore, an important research goal to make these materials competitive is a narrowing of the thermal hysteresis of MT, which can be achieved primarily by tuning compositions. The other possible method, still not explored extensively in literature, is the exploration of partial transformations (minor loops) that can increase reversibility and decrease hysteresis [14].
Numerous sources compiling the current state of magnetocaloric cooling assert the need for a thermally efficient heat exchanger that has a high surface-to-volume ratio, in order to maximize heat transfer capabilities [13,[15], [16], [17]]. Such a heat exchanger is a challenge when fabrication or assembly techniques affect materials’ functionality, leaving some alloys that show promise in laboratory testing to exhibit only a modest MCE after fabrication [18,19]. Currently, some of the attempted fabrication routes for magnetocaloric heat exchangers are: selective laser melting [18], powder packed bed [20], composite compaction [21], or polymer bonding [19,22]; each method has some limited success but none of them has emerged as the sole solution to the fabrication question. Typically, Ni-Mn-based Heusler SMAs are manufactured as single crystals, thin films, foams, and polycrystals. Additive manufacturing (AM) can add the great possibility of fabricating complex shapes with controlled, designed porosity as explored through binder jet printing and laser-based manufacturing. Research studies in the area of additively manufactured MCE materials are sparse. Moore et al. studied the selective laser melting of magnetocaloric alloy La(Fe, Co, Si)13 through comparison of two different bulk geometries [18]. Laser powder bed fusion of Ni-Mn-Ga is described in the recent work by Laitinen et al. [23,24] and Nilsen et al. [25]. Mostafaei et al. and Caputo et al. studied binder jet 3D printing of Ni-Mn-Ga with compositions more suitable for purposes of the magnetic shape memory actuators than for potential magnetocaloric applications [[26], [27], [28], [29]]. Taylor et al. reported on the sintering of particle-based ink 3D printed elemental Ni, Mn, and Ga powder particle-containing inks [30]. Stevens et al. have introduced both direct laser deposition of Ni-Mn-Co-Sn MetaMSMAs and preliminary binder jet printing results for Ni-Mn(Cu)-Ga FSMA [31,32].
The present study explores a magnetocaloric material fabricated via binder jet 3D printing (BJ3DP), focusing on the Ni-Mn(Cu)-Ga FSMA, transforming martensitically near room temperature from the paramagnetic austenite into the ferromagnetic martensite. We found that the MT in this material can be realized with an extremely narrow thermal hysteresis of 1.2 K through a partial transformation still involving large values of ΔM, ΔSm and ΔTad. The relatively small values of both hysteresis and transformation interval gave rise to the stable cycling amplitude of ΔTad equal to about 2 K under 2 T at 304 K.
Section snippets
Materials and methods
Eight polycrystalline ingots with a nominal composition of Ni50.00Mn18.75Cu6.25Ga25.00 (at.%) were prepared by induction melting from high purity (99.99+ %) elemental Ni, Mn, Ga, and Cu in an argon atmosphere. As-cast ingots were ball milled and sieved to particle sizes below 106 μm. Approximately 300 g of powder was used to fabricate cylindrical (5 mm height and 10 mm diameter) coupons via the BJ3DP additive manufacturing method in an ExOne X-1 Lab printer, using ExOne Solvent Binder 04. For
Microstructure
The results of density analysis are shown in Table 2. It is worth noting that the evaluation region for each technique was different. Archimedes method measured the bulk density (94 % ± 1 pp [percentage points]). Micro-computed X-ray tomography (μCT) is only successful on small samples, so a sliver was cut from near the center of the workpiece (96 % ± 1 pp). The image analysis was performed on micrographs from the sample after it was cut in a half near the center, so is more representative of a
Analysis of transformation characteristics
Table 5 compiles the data obtained in the present work and compared to literature for similar FSMAs. Table 5 shows the slight increased value of the unit cell volume of martensitic phase calculated for BJ3PD sample, 99.73 Å3, compared to that calculated using data presented by Sarkar et al. [44], 97.54 Å3, or from Wroblewski et al. [48], 96.64 Å3. These variations can be related to the differences in the composition. Also, an influence of the possible antisite atomic disorder and/or
Conclusions
Additive manufacturing in the form of powder bed binder jet 3D printing is shown to be a viable method for producing magnetocaloric Ni-Mn(Cu)-Ga FSMAs. Post-processing included sintering in an argon-purged vacuum atmosphere followed by an air cool. Samples showed a ΔTad of 2 K under 2 T at 304 K. The subsequent cycling resulted in a stable ΔTad of approximately 1.65 K. The stable cycling of such a value of ΔTad is achieved owing to a record-breaking low hysteresis for FSMAs, of 1.2 K,
CRediT authorship contribution statement
Erica Stevens: Conceptualization, Methodology, Writing - original draft, Visualization, Investigation, Formal analysis. Katerina Kimes: Investigation, Formal analysis. Daniel Salazar: Investigation, Supervision, Writing - review & editing. Amir Mostafaei: Methodology, Investigation. Rafael Rodriguez: Investigation, Formal analysis. Aaron Acierno: Software, Formal analysis. Patricia Lázpita: Software, Formal analysis, Writing - review & editing. Volodymyr Chernenko: Conceptualization, Resources,
Declaration of Competing Interest
The authors report no declarations of interest.
Acknowledgements
This work was performed at the Nanoscale Fabrication and Characterization Facility, a laboratory of the Gertrude E. and John M. Petersen Institute of NanoScience and Engineering; at the Materials Micro-Characterization Laboratory containing the Fishione Center of Excellence for EM-sample Preparation; at the ANSYS Additive Manufacturing Research Laboratory; and at the Materials Characterization Laboratory housed within the University of Pittsburgh’s Department of Chemistry. This project was
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now at: Department of Mechanical, Materials and Aerospace Engineering, Illinois Institute of Technology, Chicago, IL, 60616, USA