Synthesis and decomposition mechanisms of Mg2FeH6 studied by in-situ synchrotron X-ray diffraction and high-pressure DSC
Introduction
There is plenty of available renewable energy sources, e.g., sun- and wind-energy, but unfortunately, they are unevenly distributed both geographically and over time. Therefore, efficient storage and distribution of renewable energy is of significant importance, and hydrogen has been suggested as an attractive future energy carrier [1]. The only drawback is that the lightest element of all, hydrogen, occurs as a gas at ambient conditions and is difficult to store in a compact and efficient way [2]. Solid-state hydrogen storage appears to be the only method with sufficient potential storage capacity to realize the so-called ‘hydrogen-economy’ [1], [3].
Due to moderate gravimetric (5.47 wt%) and extremely high volumetric (150 kg/m3) hydrogen storage capacities, the complex magnesium iron hydride, Mg2FeH6, is considered as an attractive material for hydrogen storage [4]. Furthermore, Mg2FeH6 is also remarkable, due to low cost and high abundance of magnesium and iron. Many ternary intermetallic hydrides are used today in commercial applications, e.g., LaNi5H6 and FeTiH2, despite their relatively lower hydrogen storage capacities of ∼2 wt% and ∼100 kg/m3 [5]. Complex hydrides formed by covalently bonded hydrogen constitute an attractive alternative class of materials and boron and aluminum hydrides, such as BH4− and AlH4−, currently receive much attention [6], [7], [8]. Several other new complex ions have recently been described, e.g., Sc(BH4)4−, Zn2(BH4)5−, [Zn(BH4)3]nn−, Zn(BH4)Cl2− [9], [10], [11], [12]. This work explores the synthesis and characterization of the ternary magnesium iron hydride Mg2FeH6 based on the FeH64− complex.
The synthesis of Mg2FeH6 is complicated by the lack of an Mg2Fe intermetallic phase in the equilibrium magnesium–iron phase diagram. Several approaches have been utilized for synthesis of Mg2FeH6, often based on mechanical milling, reactive mechanical alloying in a hydrogen atmosphere, or sintering at elevated temperatures and hydrogen pressures, typically in the range 300–550 °C and 20–120 bar. In general, the yield of Mg2FeH6 fabricated by sintering, mechanical milling, or reactive mechanical milling is >50% depending on both the initial materials and the processing conditions [4], [13], [14].
Recently, Polanski et al. [15] successfully synthesized Mg2FeH6 by a novel synthetic route combining high energy mechanical ball-milling of 2MgH2–Fe under argon, sintering in Sievert's apparatus under hydrogen pressures of 85–100 bar, and heat treatment in the range from RT to 500 °C with heating rates of 5–20 °C/min. Despite a relatively short reaction time in the range of 20 min to 2 h for the complete process, a yield of >90% product was reached.
Bogdanović et al. [16] performed accurate and systematic thermodynamic and microstructural investigations of Mg2FeH6 with the use of combined high resolution transmission electron microscopy (TEM) and Energy Dispersive X-ray Spectroscopy (EDS). Based on ex-situ results, they concluded that the ternary Mg–Fe–H hydride is most likely formed from elemental Mg, Fe and H2 with no MgH2 as an intermediate phase. They also demonstrated good cycling behavior of the Mg–Fe–H system. The energy and electronic structure of Mg2FeH6 were studied by Zhou et al. [17] using first-principles plane-wave pseudopotential methods. The authors stated (contrary to Bogdanović) that Mg2FeH6 is created by a direct reaction of MgH2 with Fe.
In this study, further knowledge of the synthesis and decomposition of Mg2FeH6 is obtained using in-situ synchrotron radiation X-ray diffraction. The ternary Mg2FeH6 is synthesized at a synchrotron beamline from a pre-milled MgH2 + Fe mixture, and the same sample is then studied during hydrogen release and uptake. Thermal effects occurring during the reaction are studied by (HP-DSC) under similar conditions. The combination of these two methods gives unique results, adding more details to the state-of-the-art in research in this area.
Section snippets
Experimental procedure
Magnesium hydride powder (ABCR, 98% based on magnesium) (2.425 g) and elemental Fe powder (ABCR, 99.9%) (2.575 g) were mixed and ball-milled in a planetary Fritsch P6 mill for 1 h at 650 rpm. A stainless steel milling jar with a volume of 80 mL was used together with 30 stainless steel balls of 10 mm in diameter giving a sample-to-ball ratio of ∼1:25. Dry hexane was added to the milling vessel to enhance heat exchange and increase milling yield. All handling of chemicals and products were performed
Results and discussion
In-situ (SR-PXD) patterns measured for a MgH2–Fe (2:1) sample heated to 500 °C under a hydrogen pressure of p(H2) = 100 bar are shown in Fig. 1. Bragg reflections from the MgH2 and Fe mixture can be observed up to a temperature of 380 °C at p(H2) = 100 bar where the diffracted intensity starts to decrease and Bragg reflections from Mg2FeH6 appear. The magnesium hydride diffraction lines disappear at T = 470 °C. No diffraction from magnesium is observed during the reaction due to the high hydrogen pressure
Conclusions
The reaction mechanisms of both synthesis and decomposition of Mg2FeH6 were studied. It was shown that the formation of Mg2FeH6 consists of two steps that always involve MgH2 as a precursor. No magnesium was observed as an intermediate phase during the synthesis from a mixture of MgH2 and Fe. The decomposition of Mg2FeH6 appears to be a single-step reaction at the selected physical conditions which will be analyzed further in our future research. The characteristic transformation temperatures
Acknowledgments
This work was supported by the Polish Ministry of Sciences and Higher Education, Key Project POIG.01.03.01-14-016/08. The authors also appreciate financial support from the Danish Research Councils under the Program Danscatt.
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