**Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function**

M. Helena Braga, Michael J. Wolverton, Maria H. de Sá and Jorge A. Ferreira *1CEMUC, Engineering Physics Department, FEUP, Porto University 2LANSCE, Los Alamos National Laboratory 3LNEG 1,3Portugal 2USA* 

### **1. Introduction**

The worldwide demand for energy in the 21st century is growing at an alarming rate. The European "World Energy Technology and Climate Policy Outlook" [WETO] predicts an average growth rate of 1.8% per annum for the period 2000-2030 for the world energy demand (European Commission, 2003). The increased demand is being met largely by reserves of fossil fuel that emit both greenhouse gases and other pollutants. Since the rate of fossil fuel consumption is higher than the rate of fossil fuel production by nature, these reserves are diminishing and they will become increasingly expensive.

Against this background, the transition towards a sustainable, carbon-free and reliable energy system capable of meeting the increasing energy demands becomes imperative. Renewable energy resources, such as wind, solar, water, wave or geothermal, can offer clean alternatives to fossil fuels. Despite of their obvious advantages renewable energy sources have also some drawbacks in their use because they are unevenly distributed both over time and geographically. Most countries will need to integrate several different energy sources and an advanced energy storage system needs to be developed.

### **1.1 Hydrogen storage: A brief overview**

Hydrogen has also attracted intensive attention as the most promising secure energy carrier of the future (Jain, 2009) due to its prominent advantages such as being:

1. Environmentally friendly. It is a "clean, green" fuel because when it burns in oxygen there is no pollutants release, only heat and water are generated:

$$2\text{H}\_2\text{ (g)} + \text{O}\_2\text{ (g)} \rightleftharpoons 2\text{H}\_2\text{O (g)} \text{ , } \Delta\text{H} = 120 \text{ kJ/g } \text{H}\_2\tag{1}$$

2. Easy to produce. Hydrogen is the most abundant element in the Universe and is found in great abundance in the world, allowing it to be produced locally and easily from a great variety of sources like water, biomass and organic matter;

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 3

Magnesium metal is hexagonal with P63/mmc space group (α-structure) but the absorption of hydrogen induces a structural change into the tetragonal rutile-type structure α-MgH2

Fig. 1. Crystal structure of magnesium (left) and magnesium hydride (right) obtained with

At high temperature and pressure, the latter phase undergoes polymorphic transformations to form two modifications: -MgH2 and -MgH2, having an orthorhombic structure and a hexagonal structure, respectively (Schlapbach & Züttel, 2001). Other high-pressure metastable phases have also been reported (Cui et al., 2008; Ravindran et al., 2004). The charge density distribution in these materials has also been investigated and revealed a strong ionic character. The charge density determination of MgH2 by means of synchrotron X-ray powder diffraction at room temperature, the maximum entropy method (MEM) and Rietveld refinement revealed that the ionic charge of Mg and H can be expressed by Mg1.91+ and H0.26-, respectively, denoting that Mg in MgH2 is fully ionized, but the H atoms are in a weak ionic state (Noritake et al., 2003). The high strength of these bonds results however in an unacceptably high thermodynamic stability which diminishes the potentialities of using MgH2 in practical applications. The hydrogen desorption temperature is well above 573 K, which is related to its high dissociation enthalpy (75 kJ/mol H2) under standard conditions of pressure (Schlapbach & Züttel, 2001). In addition, the high directionality of the ionic bonds in this system leads to large activation barriers for atomic motion, resulting in slow

Several solutions were envisaged to circumvent these drawbacks. They can be accomplished to some extent by changing the microstructure of the hydride by ball-milling it (Huot et al., 1999; Zaluski et al., 1997). In this process the material is heavily deformed, and crystal defects such as dislocations, stacking faults, vacancies are introduced combined with an increased number of grain boundaries, which enhance the diffusivity of hydrogen into and out of the material (Suryanarayana, 2008). Alloying the system with other metallic additives, like 3d elements (Ti, Fe, Ni, Cu or Al), or LaNi5, FeTi, Pd, V among others and oxides like V2O5 or Nb2O5 can also be a way of improving kinetic and/or thermodynamic properties by changing the chemical interaction between the atoms (Reule et al., 2000; Rude et al., 2011; Tan et al., 2011a). The use of a proper destabilization or catalyst element/alloy into the system has also been shown to improve adsorption/desorption kinetics and to lower the adsorption temperature (Beattie et al., 2011). Furthermore, substantial improvements in the hydridingdehydriding properties can be achieved by nanoengineering approaches using nanosized reactants or by nanoconfinement of it (Jeon et al., 2011; Jurczyk et al., 2011; Vajo, 2011; Zaluska

(P42/mnm) (Aguey-Zinsou & Ares-Fernández, 2010) (see Fig. 1).

Materials Design® software

hydrogen sorption kinetics (Vajo & Olson, 2007).

Mg (s) + H2 (g) MgH2 (s) (3)

3. Light. Hydrogen is the Nature's simplest and lightest element with only one proton and one electron with high energy per unit mass.

Nonetheless, opposing to the advantages of hydrogen as an energy carrier is the difficulty in storing it. Hydrogen storage remains a problem, in particular for mobile/vehicular applications (Felderhoff et al., 2007). High-pressure hydrogen gas requires very large volumes compared to petrol, for producing the same amount of energy. On the other hand, liquid hydrogen storage systems are not viable for vehicular applications due to safety concerns in addition to volumetric constraints. Thus, hydrogen storage viability has prompted an extensive effort to develop solid hydrogen storage systems but no fully satisfactory solutions have been achieved to date (Churchard et al., 2011).

The goal is to find a material capable of simultaneously absorbing hydrogen strongly enough to form a stable thermodynamic state, but weakly enough to release it on-demand with a small temperature rise (Jeon et al., 2011) in a safe, compact, robust, and efficient manner. There have been many materials under development for solid hydrogen storage, including metal hydrides (MHx), via the chemical reaction of H2 with a metal or metal alloy (M):

$$\text{(x/2) }\mathrm{H\_2}\text{ (g) + M (s) \rightleftharpoons MH\_x (s)}\tag{2}$$

Generally, a typical hydriding reaction is known to involve several steps: (1) gas permeation through the particle bed, (2) surface adsorption and hydrogen dissociation, (3) migration of hydrogen atoms from the surface into the bulk, (4) diffusion through the particle and finally (5) nucleation and growth of the hydride phase. Any delay in one of these steps will reduce the kinetic properties of the process (Schimmel et al., 2005).

#### **1.2 Magnesium hydride**

Magnesium-based hydrogen storage alloys have been considered most promising solid hydrogen storage materials due to their high gravimetric hydrogen storage densities and volumetric capacity (see Table 1 adapted from (Chen & Zhu, 2008) for comparison) associated to the fact that magnesium is abundant in the earth's crust, non toxic and cheap (Grochala & Edwards, 2004; Jain et al., 2010; Schlapbach & Züttel, 2001).


Table 1. Structure and hydrogen storage properties of typical metal hydrides

Magnesium can be transformed in a single step to MgH2 hydride with up to 7.6 wt% of hydrogen with a volumetric storage efficiency of 110g H2/l (Milanese et al., 2010a), according to:

3. Light. Hydrogen is the Nature's simplest and lightest element with only one proton and

Nonetheless, opposing to the advantages of hydrogen as an energy carrier is the difficulty in storing it. Hydrogen storage remains a problem, in particular for mobile/vehicular applications (Felderhoff et al., 2007). High-pressure hydrogen gas requires very large volumes compared to petrol, for producing the same amount of energy. On the other hand, liquid hydrogen storage systems are not viable for vehicular applications due to safety concerns in addition to volumetric constraints. Thus, hydrogen storage viability has prompted an extensive effort to develop solid hydrogen storage systems but no fully

The goal is to find a material capable of simultaneously absorbing hydrogen strongly enough to form a stable thermodynamic state, but weakly enough to release it on-demand with a small temperature rise (Jeon et al., 2011) in a safe, compact, robust, and efficient manner. There have been many materials under development for solid hydrogen storage, including metal hydrides

Generally, a typical hydriding reaction is known to involve several steps: (1) gas permeation through the particle bed, (2) surface adsorption and hydrogen dissociation, (3) migration of hydrogen atoms from the surface into the bulk, (4) diffusion through the particle and finally (5) nucleation and growth of the hydride phase. Any delay in one of these steps will reduce

Magnesium-based hydrogen storage alloys have been considered most promising solid hydrogen storage materials due to their high gravimetric hydrogen storage densities and volumetric capacity (see Table 1 adapted from (Chen & Zhu, 2008) for comparison) associated to the fact that magnesium is abundant in the earth's crust, non toxic and cheap

Metal Hydrides Structure Mass % Peq, T LaNi5 LaNi5H6 Hexagonal 1.4 2 bar, 298 K CaNi3 CaNi3H4.4 Hexagonal 1.8 0.5 bar, 298 K ZrV2 ZrV2H5.5 Hexagonal 3.0 10-8 bar, 323 K TiFe TiFeH1.8 Cubic 1.9 5 bar, 303 K

Monoclinic (LT)

Ti-V-based Ti-V-based-H4 Cubic 2.6 1 bar, 298 K Mg MgH2 Tetragonal 7.6 1 bar, 573 K

Magnesium can be transformed in a single step to MgH2 hydride with up to 7.6 wt% of hydrogen with a volumetric storage efficiency of 110g H2/l (Milanese et al., 2010a),

Table 1. Structure and hydrogen storage properties of typical metal hydrides

(x/2) H2 (g) + M (s) MHx (s) (2)

/ Cubic (HT) 3.6 1 bar, 555 K

satisfactory solutions have been achieved to date (Churchard et al., 2011).

(MHx), via the chemical reaction of H2 with a metal or metal alloy (M):

(Grochala & Edwards, 2004; Jain et al., 2010; Schlapbach & Züttel, 2001).

the kinetic properties of the process (Schimmel et al., 2005).

**1.2 Magnesium hydride** 

Mg2Ni Mg2NiH4

according to:

one electron with high energy per unit mass.

$$\text{Mg (s)} + \text{H}\_2\text{ (g)} \ncong\\ \text{MgH}\_2\text{ (s)}\tag{3}$$

Magnesium metal is hexagonal with P63/mmc space group (α-structure) but the absorption of hydrogen induces a structural change into the tetragonal rutile-type structure α-MgH2 (P42/mnm) (Aguey-Zinsou & Ares-Fernández, 2010) (see Fig. 1).

Fig. 1. Crystal structure of magnesium (left) and magnesium hydride (right) obtained with Materials Design® software

At high temperature and pressure, the latter phase undergoes polymorphic transformations to form two modifications: -MgH2 and -MgH2, having an orthorhombic structure and a hexagonal structure, respectively (Schlapbach & Züttel, 2001). Other high-pressure metastable phases have also been reported (Cui et al., 2008; Ravindran et al., 2004). The charge density distribution in these materials has also been investigated and revealed a strong ionic character. The charge density determination of MgH2 by means of synchrotron X-ray powder diffraction at room temperature, the maximum entropy method (MEM) and Rietveld refinement revealed that the ionic charge of Mg and H can be expressed by Mg1.91+ and H0.26-, respectively, denoting that Mg in MgH2 is fully ionized, but the H atoms are in a weak ionic state (Noritake et al., 2003). The high strength of these bonds results however in an unacceptably high thermodynamic stability which diminishes the potentialities of using MgH2 in practical applications. The hydrogen desorption temperature is well above 573 K, which is related to its high dissociation enthalpy (75 kJ/mol H2) under standard conditions of pressure (Schlapbach & Züttel, 2001). In addition, the high directionality of the ionic bonds in this system leads to large activation barriers for atomic motion, resulting in slow hydrogen sorption kinetics (Vajo & Olson, 2007).

Several solutions were envisaged to circumvent these drawbacks. They can be accomplished to some extent by changing the microstructure of the hydride by ball-milling it (Huot et al., 1999; Zaluski et al., 1997). In this process the material is heavily deformed, and crystal defects such as dislocations, stacking faults, vacancies are introduced combined with an increased number of grain boundaries, which enhance the diffusivity of hydrogen into and out of the material (Suryanarayana, 2008). Alloying the system with other metallic additives, like 3d elements (Ti, Fe, Ni, Cu or Al), or LaNi5, FeTi, Pd, V among others and oxides like V2O5 or Nb2O5 can also be a way of improving kinetic and/or thermodynamic properties by changing the chemical interaction between the atoms (Reule et al., 2000; Rude et al., 2011; Tan et al., 2011a). The use of a proper destabilization or catalyst element/alloy into the system has also been shown to improve adsorption/desorption kinetics and to lower the adsorption temperature (Beattie et al., 2011). Furthermore, substantial improvements in the hydridingdehydriding properties can be achieved by nanoengineering approaches using nanosized reactants or by nanoconfinement of it (Jeon et al., 2011; Jurczyk et al., 2011; Vajo, 2011; Zaluska

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 5

 NiMg2 (s) +2H2 (g) NiMg2H4 (s) (5) Results obtained by A. Zaluska and co-workers (Zaluska et al., 1999b) showed that ballmilling the mixtures MgH2 and NiMg2H4 results in a synergetic effect of desorption, allowing the mixture to operate at temperatures as low as 493 K – 513 K, with good absorption / desorption kinetics and with total hydrogen capacity exceeding 5 wt.%. They point out however that the ball-milled mixtures of the hydrides behave differently from two metal phases that are firstly ball-milled and then hydrogenated. In the latter case volume changes occur during hydrogenation with associated volume expansion of the material, in contrast to what happen in their study in which NiMg2H4 promoted the hydrogen release from an adjacent MgH2 matrix since they undergo a significant volume contraction, which

Many more studies have focused on changes in the hydriding/dehydriding properties of Ni-Mg binary alloys with compositional changes and changes in processing variables. Nonetheless, we highlight the study of C. D. Yim and collaborators (Yim et al., 2007) that showed that the NiMg2 compound acted as a catalyst in the dissociation of the hydrogen molecule, which resulted in a faster nucleation of magnesium hydride compared to pure Mg. It also revealed that the capacity and kinetics of hydriding were larger and faster when the average size of the hydriding phase was smaller and the volume fraction of the phase boundary was larger, since phase boundaries between the eutectic α-Mg and NiMg2 phases

In the full hydrogenated state, the NiMg2H4 structure consists of tetrahedral [NiH4]4 complexes in a framework of magnesium ions and two different forms exist, hightemperature (HT) and low-temperature (LT). Under the partial pressure of 1 atm of hydrogen, the HT cubic structure phase transforms into a LT monoclinically distorted structure between 518 and 483 K (Zhang et al., 2009). The LT phase has also two modifications the untwined (LT1) and micro-twinned (LT2), which depend on the thermomechanical history of the sample (Cermak & David, 2011). The hydride formation enthalpy for the NiMg2H4 has been determined experimentally for the HT form, and it is in the rangeof -64.3 to -69.3 kJ/mol H2, for the LT form this value ranges from -68.6 to -81.0

In the pioneer work of Reilly and Wiswall (Reilly & Wiswall, 1968) it was pointed out the catalytical effect of NiMg2 on the hydrogen desorption characteristics of MgH2. Recently, Cermak and David (Cermak & David, 2011) showed that NiMg2, and more efficiently the LT1 phase of NiMg2H4, were responsible for the catalytic effect of Ni reported in the literature. The fact that NiMg2 is a metal whereas NiMg2H4 behaves like a semiconductor has opened the way to the possibility of using this system also as a switchable mirror upon hydrogenation and dehydrogenation (Setten et al., 2007). A switchable mirror will switch from mirror to transparent material upon hydrogenation. A more detailed study of Ni-Mg-

Despite all the interest and extensive research on the above referred systems, a problem still remains; the hydrogen holding capacities of these materials are considerably less than that of MgH2 (Sabitu et al., 2010). A way to overcome this limitation was found by combining MgH2 with LiBH4 (which involves the formation of MgB2 and Li-Mg alloy (Yu et al., 2006)) since pure LiBH4 has high gravimetric and volumetric hydrogen densities, 18.5 wt. % and

facilitates their dehydrogenation.

kJ/mol H2 (Tan et al., 2011b).

acted as a fast diffusion path for atomic hydrogen.

based hydrides can be found in (Orimo & Fujii, 2001).

et al., 1999a; Zhao-Karger et al., 2010). The latter allows shorter diffusion distances and larger surface area, resulting in faster reaction kinetics. It can also introduce alternative mechanisms to hydrogen exchange modifying the thermodynamic stability of the process.

As previously referred, an alternative approach for altering the thermodynamics of hydrogenation-dehydrogenation is achieved by using additives that promote hydride destabilization by alloy or compound formation in the dehydrogenated state. This approach is known as chemical destabilization. The principle underlying this approach is that the additives are capable to form compounds or alloys in the dehydrogenated state that are energetically favourable with respect to the products of the reaction without additives. Destabilization occurs because the system can cycle between the hydride and the additive instead of the elemental metal. A generalized enthalpy diagram illustrating this approach destabilization of the generic hydride AH2 through alloy formation (ABx) promoted by the presence of the alloying species B - was given by Vajo and Olson (Vajo & Olson, 2007), and is shown in Fig. 2.

Fig. 2. Generalized enthalpy diagram illustrating destabilization through alloy formation upon dehydrogenation (adapted from Vajo & Olson, 2007)

#### **1.3 Cu-Mg, Ni-Mg and other MgH2 destabilizing systems**

The work of Reilly and Wiswall provided the first evidences of this concept (Reilly & Wiswall, 1967, 1968). In their work, they showed that MgH2 can be destabilized by Cu2Mg. The formation of CuMg2 occurs upon dehydrogenation at lower reaction temperatures than those obtained with just pure MgH2. The compound CuMg2 crystallizes in the orthorhombic structure (Braga et al., 2010c) and has a hydrogen capacity of 2.6 wt. % at 573 K (Jurczyk et al., 2007). The hydride formation enthalpy is approximately 5 kJ/mol H2 lower than that of the hydrogenation of MgH2 from Mg and this process obeys to the following scheme (Reilly & Wiswall, 1967):

$$\text{2CuMg}\_2\text{(s)} + \text{3H}\_2\text{(g)} \rightleftharpoons \text{3MgH}\_2\text{(s)} + \text{Cu}\_2\text{Mg}\text{(s)}\tag{4}$$

The intermetallic cubic compound Cu2Mg does not hydrogenate under conventional hydrogenation conditions and seems to improve dehydrogenation kinetics (as compared to MgH2) due to improve resistance towards oxygen contamination (Andreasen et al., 2006; Kalinichenka et al., 2011; Reilly & Wiswall, 1967). As to the hexagonal intermetallic compound NiMg2, Reilly and Wiswall (Reilly & Wiswall, 1968) established that it reversibly reacts with hydrogen to form a ternary hydride Mg2NiH4, with a hydrogen content of 3.6 wt. %, according to the following scheme:

et al., 1999a; Zhao-Karger et al., 2010). The latter allows shorter diffusion distances and larger surface area, resulting in faster reaction kinetics. It can also introduce alternative mechanisms

As previously referred, an alternative approach for altering the thermodynamics of hydrogenation-dehydrogenation is achieved by using additives that promote hydride destabilization by alloy or compound formation in the dehydrogenated state. This approach is known as chemical destabilization. The principle underlying this approach is that the additives are capable to form compounds or alloys in the dehydrogenated state that are energetically favourable with respect to the products of the reaction without additives. Destabilization occurs because the system can cycle between the hydride and the additive instead of the elemental metal. A generalized enthalpy diagram illustrating this approach destabilization of the generic hydride AH2 through alloy formation (ABx) promoted by the presence of the alloying species B - was given by Vajo and Olson (Vajo & Olson, 2007), and

A + H2 **Dehydrogenated state:** H large T high

ABx + H2 **Stabilized alloyed state:** H smaller T lower

Fig. 2. Generalized enthalpy diagram illustrating destabilization through alloy formation

The work of Reilly and Wiswall provided the first evidences of this concept (Reilly & Wiswall, 1967, 1968). In their work, they showed that MgH2 can be destabilized by Cu2Mg. The formation of CuMg2 occurs upon dehydrogenation at lower reaction temperatures than those obtained with just pure MgH2. The compound CuMg2 crystallizes in the orthorhombic structure (Braga et al., 2010c) and has a hydrogen capacity of 2.6 wt. % at 573 K (Jurczyk et al., 2007). The hydride formation enthalpy is approximately 5 kJ/mol H2 lower than that of the hydrogenation of MgH2 from Mg and this process obeys to the following scheme (Reilly

 2CuMg2 (s) +3H2 (g) 3MgH2 (s) +Cu2Mg (s) (4) The intermetallic cubic compound Cu2Mg does not hydrogenate under conventional hydrogenation conditions and seems to improve dehydrogenation kinetics (as compared to MgH2) due to improve resistance towards oxygen contamination (Andreasen et al., 2006; Kalinichenka et al., 2011; Reilly & Wiswall, 1967). As to the hexagonal intermetallic compound NiMg2, Reilly and Wiswall (Reilly & Wiswall, 1968) established that it reversibly reacts with hydrogen to form a ternary hydride Mg2NiH4, with a hydrogen content of 3.6

to hydrogen exchange modifying the thermodynamic stability of the process.

AH2 + xB **Hydrogenated state** 

upon dehydrogenation (adapted from Vajo & Olson, 2007)

**1.3 Cu-Mg, Ni-Mg and other MgH2 destabilizing systems** 

is shown in Fig. 2.

 

 

& Wiswall, 1967):

wt. %, according to the following scheme:

ENTHALPY

$$\text{NiMg}\_2\text{(s)} + 2\text{H}\_2\text{(g)} \ncong\\ \text{NiMg}\_2\text{H}\_4\text{(s)}\tag{5}$$

Results obtained by A. Zaluska and co-workers (Zaluska et al., 1999b) showed that ballmilling the mixtures MgH2 and NiMg2H4 results in a synergetic effect of desorption, allowing the mixture to operate at temperatures as low as 493 K – 513 K, with good absorption / desorption kinetics and with total hydrogen capacity exceeding 5 wt.%. They point out however that the ball-milled mixtures of the hydrides behave differently from two metal phases that are firstly ball-milled and then hydrogenated. In the latter case volume changes occur during hydrogenation with associated volume expansion of the material, in contrast to what happen in their study in which NiMg2H4 promoted the hydrogen release from an adjacent MgH2 matrix since they undergo a significant volume contraction, which facilitates their dehydrogenation.

Many more studies have focused on changes in the hydriding/dehydriding properties of Ni-Mg binary alloys with compositional changes and changes in processing variables. Nonetheless, we highlight the study of C. D. Yim and collaborators (Yim et al., 2007) that showed that the NiMg2 compound acted as a catalyst in the dissociation of the hydrogen molecule, which resulted in a faster nucleation of magnesium hydride compared to pure Mg. It also revealed that the capacity and kinetics of hydriding were larger and faster when the average size of the hydriding phase was smaller and the volume fraction of the phase boundary was larger, since phase boundaries between the eutectic α-Mg and NiMg2 phases acted as a fast diffusion path for atomic hydrogen.

In the full hydrogenated state, the NiMg2H4 structure consists of tetrahedral [NiH4]4 complexes in a framework of magnesium ions and two different forms exist, hightemperature (HT) and low-temperature (LT). Under the partial pressure of 1 atm of hydrogen, the HT cubic structure phase transforms into a LT monoclinically distorted structure between 518 and 483 K (Zhang et al., 2009). The LT phase has also two modifications the untwined (LT1) and micro-twinned (LT2), which depend on the thermomechanical history of the sample (Cermak & David, 2011). The hydride formation enthalpy for the NiMg2H4 has been determined experimentally for the HT form, and it is in the rangeof -64.3 to -69.3 kJ/mol H2, for the LT form this value ranges from -68.6 to -81.0 kJ/mol H2 (Tan et al., 2011b).

In the pioneer work of Reilly and Wiswall (Reilly & Wiswall, 1968) it was pointed out the catalytical effect of NiMg2 on the hydrogen desorption characteristics of MgH2. Recently, Cermak and David (Cermak & David, 2011) showed that NiMg2, and more efficiently the LT1 phase of NiMg2H4, were responsible for the catalytic effect of Ni reported in the literature. The fact that NiMg2 is a metal whereas NiMg2H4 behaves like a semiconductor has opened the way to the possibility of using this system also as a switchable mirror upon hydrogenation and dehydrogenation (Setten et al., 2007). A switchable mirror will switch from mirror to transparent material upon hydrogenation. A more detailed study of Ni-Mgbased hydrides can be found in (Orimo & Fujii, 2001).

Despite all the interest and extensive research on the above referred systems, a problem still remains; the hydrogen holding capacities of these materials are considerably less than that of MgH2 (Sabitu et al., 2010). A way to overcome this limitation was found by combining MgH2 with LiBH4 (which involves the formation of MgB2 and Li-Mg alloy (Yu et al., 2006)) since pure LiBH4 has high gravimetric and volumetric hydrogen densities, 18.5 wt. % and

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 7

respectively. They attributed the decrement in the absorption capacity to the formation of the intermetallic phase Cu2Mg, which does not absorb the hydrogen but itself behaves like a catalyst. However, in the case of nanocrystalline CuxNi10-xMg20 (x = 0 - 4) alloys synthesized by melt-spinning technique, it was found (Zhang et al., 2010a, 2010b) that the substitution of Ni by Cu does not change the major phase NiMg2 although it leads to a refinement of grains with increased cell volume and the formation of a secondary phase CuMg2. This in turn leads to a decrease of the hydride stability with a clear improve of the hydrogen desorption capacity and kinetics of the alloys. The presence of CuMg2 seems to act as a catalyst for the hydride-dehydride reactions of Mg and Mg-based alloys. Similar behaviour was found in Cu0.25Ni0.75Mg2 and Cu0.4Ni0.6Mg2 alloys that were prepared by mechanical alloying and subsequent thermal treatment (Simičić et al., 2006). The latter effect was also investigated on Cu1-xNixMg2 (x = 0 - 1) alloys by Hsu and collaborators (Hsu et al., 2010). They observed that by substituting Cu by Ni in CuMg2, the cell volume decreased (since the radius of Cu atom is slightly larger than Ni atom) and with increasing Ni content, the effect of Ni is actually effective in MgH2 and Mg2NiH4 destabilization, leading to a decrease of desorption temperature in these two phases. They also showed that substituted nickel caused the hydriding reaction because absorption kinetics and hydrogen storage capacity increased

An alternative route to be considered is to explore other hydrides besides MgH2 for solid hydrogen storage. One of most interesting is lithium hydride, because it contains 12.5 wt.% hydrogen. Nonetheless, the desorption temperature is 1183 K for an equilibrium pressure of 1 bar (Vajo et al., 2004). However, it has been shown (Chen et al., 2003) that when LiH (see Fig. 3) reacts with lithium amide (LiNH2) by thoroughly mixing the substances, hydrogen is released at temperatures around 423 K, with formation of lithium imide (Li2NH) or Li-rich imide (LixNH3-X) and lithium nitride (Li3N) depending on the temperature and molar ratio


2LiH (s) +LiNH2 (s) (x-1) H2 (g) + LixNH3-x (s) + (3-x) LiH(s) (7)


Fig. 3. Crystal structure of lithium hydride obtained with Materials Design® software

with the rise of Ni-substitution contents.

of (LiH/LiNH2) according to the following schemes:

**1.4 Lithium hydride** 

121 kg H2/m3, respectively (Bösenberg et al., 2010; Xia et al., 2011). However, although the reaction enthalpy is lowered and the hydrogen storage capacity increases (10.5 wt. %), the sorption and absorption processes occurs at high temperatures with relatively slow kinetic even though more additives are being tested in order to overcome this problem (Fernández et al., 2011; Xia et al., 2011). Alternatively, the study of the destabilization of MgH2 with TiH2 has also been taken experimentally (Choi et al., 2008; Sohn et al., 2011). Observations point to a substantially reduced apparent activation energy of 107-118 kJ/mol and significantly faster kinetics, compared with the 226 kJ/mol for the similarly milled MgH2. The latter system constitutes a promising material to be used in practical applications for hydrogen storage.

The combined destabilization effect of Ni-Mg and Cu-Mg intermetallics towards MgH2 was also tested and the Mg-rich ternary Cu-Ni-Mg alloys were recognized to have high potential for solid state hydrogen storage and have attracted many research interests. The study recently reported by Tan and co-workers (Tan et al., 2011b) elucidates about the influence of Cu substitution on the hydrogen sorption properties of magnesium rich Ni-Mg films. This study shows a two-step hydrogen absorption process. The first step is due to the absorption of Mg not alloyed in the form of NiMg2 and/or CuMg2, hereafter denoted as "free Mg" and is very quick, because it is mainly catalyzed by the intermetallic phase, NiMg2. But the second step, due to the hydrogen absorption of intermetallic NiMg2 and/or CuMg2 ("bonded Mg") is significantly slow. The Cu substitution shows positive effects on desorption kinetics during full capacity hydrogen cycling, but shows strongly negative effects on absorption kinetics, particularly for the second absorption step, due to the segregation of CuMg2 towards the grain boundaries of MgH2, forming a closed shell that traps the hydrogen in MgH2. The authors also reported that the Cu substitution has no Thermo-destabilization effect on MgH2, but since a significant amount can be dissolved in NiMg2, even at elevated temperatures, thermo-destabilization of NiMg2H4 and better desorption kinetics are observed. Hong and collaborators (Hong et al., 2011) on their study on the hydrogen storage properties of x wt.% Cu-23.5 wt.% Ni-Mg (x = 2.5, 5 and 7.5) prepared by rapid solidification process and crystallization heat treatment have also reported that the NiMg2 phase has higher hydriding and dehydriding rates than Mg under similar conditions and that the addition of a smaller amount of Cu is considered favourable to the enhancement of the hydriding and dehydriding rates of the sample. The 2.5 wt.% Cu-23.5 wt.% Ni-Mg alloy had the highest hydriding and dehydriding rates. These observations are in line with the ones previously reported by the group of Milanese (Milanese et al., 2010b; 2008), who also observed the high sorption capacity and good sorption performance of Cu-Ni-Mg mixtures and proposed a two steps sorption process with different kinetics. The first step corresponds to the quick hydrogenation of "free Mg", according to reaction (3). After this step, absorption keeps on with a slower rate corresponding to the second step, hydrogenation of the "bonded Mg" phases, NiMg2 and CuMg2, according to reactions (4) and (5). They also showed that Ni is more effective than Cu in catalyzing the desorption reactions and that NiMg2H4 and Cu2Mg phases destabilized each other with the beneficial effect of decreasing the dissociation temperature of about 50 K in comparison to the MgH2, from "free Mg". The positive effect of Cu as a catalyst on the hydrogenation and thermodynamic properties of NiMg2 mixed by ball milling technique was also studied and recently reported by Vyas and co-workers (Vyas et al., 2011) showing that hydrogen storage capacity and enthalpy of formation of NiMg2 with 10 wt.% Cu reduces to 1.81 wt.% and 26.69 kJ (mol H)-1 from 3.56 wt.% and 54.24 kJ (mol H)-1 for pure NiMg2 at 573 K, respectively. They attributed the decrement in the absorption capacity to the formation of the intermetallic phase Cu2Mg, which does not absorb the hydrogen but itself behaves like a catalyst. However, in the case of nanocrystalline CuxNi10-xMg20 (x = 0 - 4) alloys synthesized by melt-spinning technique, it was found (Zhang et al., 2010a, 2010b) that the substitution of Ni by Cu does not change the major phase NiMg2 although it leads to a refinement of grains with increased cell volume and the formation of a secondary phase CuMg2. This in turn leads to a decrease of the hydride stability with a clear improve of the hydrogen desorption capacity and kinetics of the alloys. The presence of CuMg2 seems to act as a catalyst for the hydride-dehydride reactions of Mg and Mg-based alloys. Similar behaviour was found in Cu0.25Ni0.75Mg2 and Cu0.4Ni0.6Mg2 alloys that were prepared by mechanical alloying and subsequent thermal treatment (Simičić et al., 2006). The latter effect was also investigated on Cu1-xNixMg2 (x = 0 - 1) alloys by Hsu and collaborators (Hsu et al., 2010). They observed that by substituting Cu by Ni in CuMg2, the cell volume decreased (since the radius of Cu atom is slightly larger than Ni atom) and with increasing Ni content, the effect of Ni is actually effective in MgH2 and Mg2NiH4 destabilization, leading to a decrease of desorption temperature in these two phases. They also showed that substituted nickel caused the hydriding reaction because absorption kinetics and hydrogen storage capacity increased with the rise of Ni-substitution contents.

#### **1.4 Lithium hydride**

6 Neutron Diffraction

121 kg H2/m3, respectively (Bösenberg et al., 2010; Xia et al., 2011). However, although the reaction enthalpy is lowered and the hydrogen storage capacity increases (10.5 wt. %), the sorption and absorption processes occurs at high temperatures with relatively slow kinetic even though more additives are being tested in order to overcome this problem (Fernández et al., 2011; Xia et al., 2011). Alternatively, the study of the destabilization of MgH2 with TiH2 has also been taken experimentally (Choi et al., 2008; Sohn et al., 2011). Observations point to a substantially reduced apparent activation energy of 107-118 kJ/mol and significantly faster kinetics, compared with the 226 kJ/mol for the similarly milled MgH2. The latter system constitutes a promising material to be used in practical applications for hydrogen

The combined destabilization effect of Ni-Mg and Cu-Mg intermetallics towards MgH2 was also tested and the Mg-rich ternary Cu-Ni-Mg alloys were recognized to have high potential for solid state hydrogen storage and have attracted many research interests. The study recently reported by Tan and co-workers (Tan et al., 2011b) elucidates about the influence of Cu substitution on the hydrogen sorption properties of magnesium rich Ni-Mg films. This study shows a two-step hydrogen absorption process. The first step is due to the absorption of Mg not alloyed in the form of NiMg2 and/or CuMg2, hereafter denoted as "free Mg" and is very quick, because it is mainly catalyzed by the intermetallic phase, NiMg2. But the second step, due to the hydrogen absorption of intermetallic NiMg2 and/or CuMg2 ("bonded Mg") is significantly slow. The Cu substitution shows positive effects on desorption kinetics during full capacity hydrogen cycling, but shows strongly negative effects on absorption kinetics, particularly for the second absorption step, due to the segregation of CuMg2 towards the grain boundaries of MgH2, forming a closed shell that traps the hydrogen in MgH2. The authors also reported that the Cu substitution has no Thermo-destabilization effect on MgH2, but since a significant amount can be dissolved in NiMg2, even at elevated temperatures, thermo-destabilization of NiMg2H4 and better desorption kinetics are observed. Hong and collaborators (Hong et al., 2011) on their study on the hydrogen storage properties of x wt.% Cu-23.5 wt.% Ni-Mg (x = 2.5, 5 and 7.5) prepared by rapid solidification process and crystallization heat treatment have also reported that the NiMg2 phase has higher hydriding and dehydriding rates than Mg under similar conditions and that the addition of a smaller amount of Cu is considered favourable to the enhancement of the hydriding and dehydriding rates of the sample. The 2.5 wt.% Cu-23.5 wt.% Ni-Mg alloy had the highest hydriding and dehydriding rates. These observations are in line with the ones previously reported by the group of Milanese (Milanese et al., 2010b; 2008), who also observed the high sorption capacity and good sorption performance of Cu-Ni-Mg mixtures and proposed a two steps sorption process with different kinetics. The first step corresponds to the quick hydrogenation of "free Mg", according to reaction (3). After this step, absorption keeps on with a slower rate corresponding to the second step, hydrogenation of the "bonded Mg" phases, NiMg2 and CuMg2, according to reactions (4) and (5). They also showed that Ni is more effective than Cu in catalyzing the desorption reactions and that NiMg2H4 and Cu2Mg phases destabilized each other with the beneficial effect of decreasing the dissociation temperature of about 50 K in comparison to the MgH2, from "free Mg". The positive effect of Cu as a catalyst on the hydrogenation and thermodynamic properties of NiMg2 mixed by ball milling technique was also studied and recently reported by Vyas and co-workers (Vyas et al., 2011) showing that hydrogen storage capacity and enthalpy of formation of NiMg2 with 10 wt.% Cu reduces to 1.81 wt.% and 26.69 kJ (mol H)-1 from 3.56 wt.% and 54.24 kJ (mol H)-1 for pure NiMg2 at 573 K,

storage.

An alternative route to be considered is to explore other hydrides besides MgH2 for solid hydrogen storage. One of most interesting is lithium hydride, because it contains 12.5 wt.% hydrogen. Nonetheless, the desorption temperature is 1183 K for an equilibrium pressure of 1 bar (Vajo et al., 2004). However, it has been shown (Chen et al., 2003) that when LiH (see Fig. 3) reacts with lithium amide (LiNH2) by thoroughly mixing the substances, hydrogen is released at temperatures around 423 K, with formation of lithium imide (Li2NH) or Li-rich imide (LixNH3-X) and lithium nitride (Li3N) depending on the temperature and molar ratio of (LiH/LiNH2) according to the following schemes:

$$\text{1-Below 593 K:} \qquad \text{LiH (s)} + \text{LiNH}\_2\text{(s)} \rightarrow 2\text{H}\_2\text{(g)} + \text{Li}\_2\text{NH (s)}\tag{6}$$

$$\text{2LiH (s) + LiNH\_2 (s) \rightarrow (x-1) H\_2 (g) + Li\_kNH\_{3x} (s) + (3-x) LiH(s)}\tag{7}$$

$$\text{- }\text{At higher temperatures:}\ 2\text{LiH}\ (\text{s}) + \text{LiNH}\_2\ (\text{s}) \rightarrow \text{H}\_2\ (\text{g}) + \text{Li}\_3\text{N}\ (\text{s})\tag{8}$$

Fig. 3. Crystal structure of lithium hydride obtained with Materials Design® software

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 9

interactions measured in barns (1 barn = 10-28 m2). In general these scattering cross

INS has numerous advantages to other common techniques of obtaining vibrational spectra such as infrared (IR) and Raman spectroscopy. INS spectroscopy is hyper sensitive to the presence of hydrogen. The protium (1H) nucleus has scattering cross sections of σcoh = 1.8 and σinc = 80.2 barns respectively. This means neutron scattering in materials containing natural abundance hydrogen is largely inelastic. Additionally, the incoherent cross section of 1H is one to two orders of magnitude higher than any other isotope (Ross, 2008). This means that in hydrides INS spectra are dominated by vibrational modes of hydrogen almost exclusively. This hyper sensitivity to hydrogen means that hydride phases are detectible even when present in relatively miniscule concentration. Another advantage of INS is the complete absence of selection rules for the excitation of vibrational modes. Lattice modes (i.e. phonons) are excited with equal opportunity to molecular vibrations. Because both IR and Raman spectroscopy rely upon different types of charge symmetry interactions, many materials have vibrational modes that cannot be excited by Raman or IR. In particular lattice modes are far more easily observable in INS spectra than any other type of vibrational spectroscopy. INS is also more useful for comparison with *ab initio* calculated density of states because relative excitation amplitudes are simply dependent upon the magnitude of motion and σinc of the excited nucleus (Squires, 1978; Ross, 2008). Free software, such as a-Climax is available to generate a theoretical INS spectrum from the density of states output files from numerous common *ab initio* packages such as Gaussian, AbInit and Dmol

For these reasons INS is extremely useful in identifying the presence of different hydride phases which may not be structurally apparent (for example, due to structural disorder). A good example is the INS study of Schimmel et al. on MgH2 produced from Mg processed by high energy ball milling. Ball milling of Mg to reduce particle size, and introduce fractures, defects, and faults has a beneficial effect of increasing hydride formation rate, and reducing the temperature required for absorption. Comparison of the INS spectra of the MgH2 produced from ball milled Mg with well-ordered MgH2 revealed a partial composition of γ-MgH2, which is metastable and normally exists only at high temperatures (Schimmel et al, 2005). Presence of γ-MgH2 was indicative of internal stress from mechanical processing. However after hydrogen sorption cycling, γ-MgH2 was no longer observable in the INS spectrum of the ball milled material, while the fast kinetics and lower sorption temperature remained. In this way INS was indispensable in revealing that the particle size reduction is more significant in the role of lowering temperature and increasing sorption kinetics than the creation of faults and internal stresses after the high energy ball milling of Mg

Neutron diffraction also provides some unique advantages versus more conventional diffraction methods such as X-ray diffraction (XRD). Elastic neutron and X-ray scattering are similar in that both result in interference patterns according to Bragg scattering conditions (Squires, 1978). In XRD the intensity of a given Bragg reflection varies with the atomic number (Z) of the atom at the lattice site. This means that the exact position of hydrogen in a structure is practically impossible to determine with XRD. In ND the relative intensities of reflections are independent of Z, and instead depend on the coherent scattering cross section (σcoh). This means that deuterium (2H; σcoh = 5.6, σinc = 2.0) is just as readily observable as

sections do not follow any specific trend regarding nucleus size.

(Ramirez, 2004).

(Schimmel, 2005; Ross, 2008).

From a detailed analysis of high-resolution synchrotron x-ray diffraction data for the lithium amide (LiNH2) - lithium imide (Li2NH) hydrogen storage system (David et al., 2007), the authors were able to propose an alternative mechanism that does not need to have the materials mechanically milled to enhance mixing, as previously recognized by Chen and collaborators (Chen et al., 2003) as essential. The mechanism they propose for the transformation between lithium amide and lithium imide during hydrogen cycling is a bulk reversible reaction that occurs in a non-stoichiometric manner within the cubic anti-fluoritelike Li-N-H structure, based on both Li+ and H+ mobility within the cubic lithium imide. Concluding that increasing the Li+ mobility and/or disorder it is likely to improve the hydrogen cycling in this and related Li-based systems. Recently, further systematical evaluation of the decompositions of LiNH2 and Li2NH was carried out by Zhang and Hu (Zhang & Hu, 2011), who also examined the effect of Cl- anion on the decomposition process. Cl- is widely employed as a promoter to improve various catalysts. As a result, decomposition mechanisms were established. The decomposition of LiNH2 producing Li2NH and NH3 occurs in two steps at the temperature range of 573-723 K. LiNH2 decomposes into a stable intermediate species (Li1.5NH1.5) and then into Li2NH. Furthermore, Li2NH is decomposed into Li, H2, and N2 without formation of Li3N at the temperature range of 823-1023 K. The introduction of Cl- can decrease the decomposition *temperature of Li2NH by about 110 K.* 

### **1.5 Neutron techniques associated with hydrogen solid storage**

Though some progress have been made, the state-of-art materials are still far from meeting the aimed targets for hydrogen solid storage material (Churchard et al., 2011). This huge task can be facilitated by employing state-of-the-art techniques like, computational first-principles calculations to evaluate the thermodynamic properties of the potential materials (Alapati et al., 2007; Siegel et al., 2007; Yang et al., 2007). This allows a quick screen of a large number of potential candidates, searching for thermodynamically suitable ones (saving time and money). Once thermodynamic appropriate materials have been found other considerations such as structure and dynamics of the materials during hydrogenation/dehydrogenation will become crucial in order to understand the fundamental properties of hydrogen storage, in realistic conditions and hence design new hydrogen storage materials.

Neutron scattering techniques are highly suitable for structure and dynamics studies related to hydrogen in solids and bound on surfaces. The energy distribution of thermal neutrons is nearly ideal for the study of condensed matter in general because it is of the same order of magnitude as most molecular and lattice excitations and the de Broglie wavelengths of thermal neutrons match quite well with interatomic distances in most solids (Squires, 1978). Neutrons have some unique advantages over photons and electrons as scattering media which are of particular use for the analysis of hydrides. For these purposes the two most useful neutron scattering interactions are coherent elastic scattering for Neutron Diffraction (ND) and incoherent Inelastic Neutron Scattering (INS) to measure vibrational density of states. The distinction of coherent and incoherent scattering interactions is important to the unique advantages offered by ND and INS respectively. This is because the relative scattering intensity of a given interaction is dependent highly upon the nucleus involved, and as such is isotope dependant. Each isotope has a different scattering cross section for both coherent (σcoh) and incoherent (σinc)

From a detailed analysis of high-resolution synchrotron x-ray diffraction data for the lithium amide (LiNH2) - lithium imide (Li2NH) hydrogen storage system (David et al., 2007), the authors were able to propose an alternative mechanism that does not need to have the materials mechanically milled to enhance mixing, as previously recognized by Chen and collaborators (Chen et al., 2003) as essential. The mechanism they propose for the transformation between lithium amide and lithium imide during hydrogen cycling is a bulk reversible reaction that occurs in a non-stoichiometric manner within the cubic anti-fluoritelike Li-N-H structure, based on both Li+ and H+ mobility within the cubic lithium imide. Concluding that increasing the Li+ mobility and/or disorder it is likely to improve the hydrogen cycling in this and related Li-based systems. Recently, further systematical evaluation of the decompositions of LiNH2 and Li2NH was carried out by Zhang and Hu (Zhang & Hu, 2011), who also examined the effect of Cl- anion on the decomposition process. Cl- is widely employed as a promoter to improve various catalysts. As a result, decomposition mechanisms were established. The decomposition of LiNH2 producing Li2NH and NH3 occurs in two steps at the temperature range of 573-723 K. LiNH2 decomposes into a stable intermediate species (Li1.5NH1.5) and then into Li2NH. Furthermore, Li2NH is decomposed into Li, H2, and N2 without formation of Li3N at the temperature range of 823-1023 K. The introduction of Cl- can decrease the decomposition

Though some progress have been made, the state-of-art materials are still far from meeting the aimed targets for hydrogen solid storage material (Churchard et al., 2011). This huge task can be facilitated by employing state-of-the-art techniques like, computational first-principles calculations to evaluate the thermodynamic properties of the potential materials (Alapati et al., 2007; Siegel et al., 2007; Yang et al., 2007). This allows a quick screen of a large number of potential candidates, searching for thermodynamically suitable ones (saving time and money). Once thermodynamic appropriate materials have been found other considerations such as structure and dynamics of the materials during hydrogenation/dehydrogenation will become crucial in order to understand the fundamental properties of hydrogen storage, in

Neutron scattering techniques are highly suitable for structure and dynamics studies related to hydrogen in solids and bound on surfaces. The energy distribution of thermal neutrons is nearly ideal for the study of condensed matter in general because it is of the same order of magnitude as most molecular and lattice excitations and the de Broglie wavelengths of thermal neutrons match quite well with interatomic distances in most solids (Squires, 1978). Neutrons have some unique advantages over photons and electrons as scattering media which are of particular use for the analysis of hydrides. For these purposes the two most useful neutron scattering interactions are coherent elastic scattering for Neutron Diffraction (ND) and incoherent Inelastic Neutron Scattering (INS) to measure vibrational density of states. The distinction of coherent and incoherent scattering interactions is important to the unique advantages offered by ND and INS respectively. This is because the relative scattering intensity of a given interaction is dependent highly upon the nucleus involved, and as such is isotope dependant. Each isotope has a different scattering cross section for both coherent (σcoh) and incoherent (σinc)

*temperature of Li2NH by about 110 K.* 

**1.5 Neutron techniques associated with hydrogen solid storage** 

realistic conditions and hence design new hydrogen storage materials.

interactions measured in barns (1 barn = 10-28 m2). In general these scattering cross sections do not follow any specific trend regarding nucleus size.

INS has numerous advantages to other common techniques of obtaining vibrational spectra such as infrared (IR) and Raman spectroscopy. INS spectroscopy is hyper sensitive to the presence of hydrogen. The protium (1H) nucleus has scattering cross sections of σcoh = 1.8 and σinc = 80.2 barns respectively. This means neutron scattering in materials containing natural abundance hydrogen is largely inelastic. Additionally, the incoherent cross section of 1H is one to two orders of magnitude higher than any other isotope (Ross, 2008). This means that in hydrides INS spectra are dominated by vibrational modes of hydrogen almost exclusively. This hyper sensitivity to hydrogen means that hydride phases are detectible even when present in relatively miniscule concentration. Another advantage of INS is the complete absence of selection rules for the excitation of vibrational modes. Lattice modes (i.e. phonons) are excited with equal opportunity to molecular vibrations. Because both IR and Raman spectroscopy rely upon different types of charge symmetry interactions, many materials have vibrational modes that cannot be excited by Raman or IR. In particular lattice modes are far more easily observable in INS spectra than any other type of vibrational spectroscopy. INS is also more useful for comparison with *ab initio* calculated density of states because relative excitation amplitudes are simply dependent upon the magnitude of motion and σinc of the excited nucleus (Squires, 1978; Ross, 2008). Free software, such as a-Climax is available to generate a theoretical INS spectrum from the density of states output files from numerous common *ab initio* packages such as Gaussian, AbInit and Dmol (Ramirez, 2004).

For these reasons INS is extremely useful in identifying the presence of different hydride phases which may not be structurally apparent (for example, due to structural disorder). A good example is the INS study of Schimmel et al. on MgH2 produced from Mg processed by high energy ball milling. Ball milling of Mg to reduce particle size, and introduce fractures, defects, and faults has a beneficial effect of increasing hydride formation rate, and reducing the temperature required for absorption. Comparison of the INS spectra of the MgH2 produced from ball milled Mg with well-ordered MgH2 revealed a partial composition of γ-MgH2, which is metastable and normally exists only at high temperatures (Schimmel et al, 2005). Presence of γ-MgH2 was indicative of internal stress from mechanical processing. However after hydrogen sorption cycling, γ-MgH2 was no longer observable in the INS spectrum of the ball milled material, while the fast kinetics and lower sorption temperature remained. In this way INS was indispensable in revealing that the particle size reduction is more significant in the role of lowering temperature and increasing sorption kinetics than the creation of faults and internal stresses after the high energy ball milling of Mg (Schimmel, 2005; Ross, 2008).

Neutron diffraction also provides some unique advantages versus more conventional diffraction methods such as X-ray diffraction (XRD). Elastic neutron and X-ray scattering are similar in that both result in interference patterns according to Bragg scattering conditions (Squires, 1978). In XRD the intensity of a given Bragg reflection varies with the atomic number (Z) of the atom at the lattice site. This means that the exact position of hydrogen in a structure is practically impossible to determine with XRD. In ND the relative intensities of reflections are independent of Z, and instead depend on the coherent scattering cross section (σcoh). This means that deuterium (2H; σcoh = 5.6, σinc = 2.0) is just as readily observable as

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 11

as previously referred (4). As a result of this reaction and since CuMg2 does not form a hydride, CuMg2 was abandoned as a candidate material for hydrogen storage (Reilly & Wiswall, 1967; Schlapbach & Züttel, 2001) until the late destabilization studies that were previously cited. The hexagonal structure of CuLixMg2-x, suggested the possibility of using this phase as a hydrogen storage material (Braga & Malheiros, 2007a, 2007b) because CuLixMg2-x has the same space group (P6222) as NiMg2 and NiMg2(H,D)0.3 (lattice parameters are almost identical: a = b = 5.250 Å and c = 13.621 Å (at 300 K) for CuLixMg2-x and a = b = 5.256 Å and c = 13.435 Å for NiMg2(H,D)0.3 (Senegas et al., 1984)). Therefore, we hypothesized that CuLixMg2-x (x = 0.08) would be a hydrogen storage material, just like NiMg2 - a hypothesis that has been confirmed by now (Braga & Malheiros, 2007a, 2007b;

The change of the CuMg2 orthorhombic (Fddd) structure to a hexagonal structure (P6222) upon addition of a small amount of Li has been firmly established (Braga et al., 2007). Isostructural phases to CuLixMg2-x are the hexagonal phase NiMg2 and NiMg2H0.24-0.30 (Senegas et al., 1984). For the NiMg-hydrides, several hydrogen positions were reported: In NiMg2H0.29 the hydrogen atoms occupy Wyckoff 6f positions and could occupy the interstitial Wyckoff 6h position (Senegas et al., 1984). Other possibilities would be that the H atoms would just occupy interstitial Wyckoff 12k position (in NiMg2H0.26) or the Wyckoff 12k and 6j positions in NiMg2H0.24 (Senegas et al., 1984). This suggests a number of possible

Interestingly V. Hlukhyy and collaborators (Hlukhyy et al., 2005) have reported a result closely related to our observations in the Sn-doped Ni-Mg system. These authors show that the synthesis of alloys in the Ni-Mg system is affected by the presence of small amounts of Sn (forming NiMg2-xSnx with x = 0.22 and 0.40). The replacement of Mg by Sn produces changes in the structure of NiMg2, this time making the alloy change from the NiMg2 type (hexagonal) to the CuMg2 type (orthorhombic). While the structure of NiMg1.85Sn0.15 is still of NiMg2 type, the structure of NiMg1.78Sn0.22 and NiMg1.60Sn0.40 is already of the CuMg2 type. These results represent obviously the converse of our own observations in the CuMg2

Fig. 4. Phase diagrams of Ni-Mg and Cu-Mg (Ansara et al., 1998)

structure, and reaffirm our results with respect to CuLixMg2-x.

Braga et al., 2010a).

sites for Li in CuLixMg2-x.

most metal atoms. This allows for the observation of hydride phase transitions which differ only by the hydrogen occupation sites, such as in interstitial hydrides. ND also allows metals with similar Z values such as Ni (Z=28, σcoh = 13.4) and Cu (Z=29, σcoh = 7.5) to be easily distinguished, unlike in XRD. A great deal of caution must be taken to ensure that 2H is not displaced by 1H during sample preparation and handling, as the large σinc of 1H will create a substantial background signal. Another advantage of ND is that intensity does not diminish greatly with scattering angle as it does in XRD (Massa, 2004). Beyond these differences, crystal structure determination techniques are very similar for ND and XRD. Common approaches include a combination of a structure solution method and the Rietveld refinement method.

ND and INS carry some common advantages and disadvantages intrinsic with the use of neutrons as a scattering medium. Common advantages are associated with the highly penetrating quality of neutron radiation through most materials. This provides some possibilities for variable depth of measurements. If the neutron beam is directed at a relatively thin portion of the sample, a greater quantity of surface and shallow depth material is surveyed, whereas in relatively thick segments predominantly material deep within the sample is surveyed. The high penetration of neutrons also allows for relatively clear in-situ measurements in a wide range of sample environments such as high pressure gas cells, furnaces, cryogenic refrigerators, anvil cells and other environments requiring obtrusive equipment. This allows for detailed structure and dynamics studies of metastable hydride phases, and phase transitions which occur only in extreme conditions.

There are numerous inconveniences associated with neutrons as well. The most prevalent and obvious is the relative scarcity and cost of neutron sources, which typically take two forms: a research reactor or a spallation source (fed by a high energy proton accelerator). Another drawback is the time required to conduct a measurement, which can range from several hours to several days (per measurement). This is due to the short range of nuclear forces and relatively low probability of a scattering event, which is the same reason neutron radiation penetrates so effectively. Because of the long measurement time and high operational cost beam time is allocated very carefully at neutron sources, and flight paths are rarely left idle during neutron production. ND and INS require larger sample sizes, often multiple grams, to increase the scattering rate.

### **2. Hydrides of Cu and Mg intermetallic systems**

We have studied the Cu-Li-Mg system as a hydrogen storage system and, at the same time, as a catalyst of the hydrogen storage process, namely for the Ti/TiH2 system (Braga & Malheiros, 2007a, 2007b; Braga et al., 2010a, 2010b). The only ternary compound the Cu-Li-Mg system holds is CuLixMg2-x (x = 0.08) with hexagonal P6222 structure (Braga et al., 2010c). Since the phase diagrams of Cu-Mg and Ni-Mg are similar (see Fig. 4), and Cu and Ni have similar electron affinities, it was thought in the sixties that CuMg2 would store hydrogen, too.

However this is not the case (Reilly & Wiswall, 1967). NiMg2 has a hexagonal structure (P6222), but CuMg2 has an orthorhombic structure (Fddd), and this structural difference is assumed to be the reason that NiMg2 stores H2 forming a hydride, but CuMg2 does not. CuMg2 decomposes into Cu2Mg and MgH2 (Reilly & Wiswall, 1967) upon hydrogen loading

most metal atoms. This allows for the observation of hydride phase transitions which differ only by the hydrogen occupation sites, such as in interstitial hydrides. ND also allows metals with similar Z values such as Ni (Z=28, σcoh = 13.4) and Cu (Z=29, σcoh = 7.5) to be easily distinguished, unlike in XRD. A great deal of caution must be taken to ensure that 2H is not displaced by 1H during sample preparation and handling, as the large σinc of 1H will create a substantial background signal. Another advantage of ND is that intensity does not diminish greatly with scattering angle as it does in XRD (Massa, 2004). Beyond these differences, crystal structure determination techniques are very similar for ND and XRD. Common approaches include a combination of a structure solution method and the Rietveld

ND and INS carry some common advantages and disadvantages intrinsic with the use of neutrons as a scattering medium. Common advantages are associated with the highly penetrating quality of neutron radiation through most materials. This provides some possibilities for variable depth of measurements. If the neutron beam is directed at a relatively thin portion of the sample, a greater quantity of surface and shallow depth material is surveyed, whereas in relatively thick segments predominantly material deep within the sample is surveyed. The high penetration of neutrons also allows for relatively clear in-situ measurements in a wide range of sample environments such as high pressure gas cells, furnaces, cryogenic refrigerators, anvil cells and other environments requiring obtrusive equipment. This allows for detailed structure and dynamics studies of metastable

There are numerous inconveniences associated with neutrons as well. The most prevalent and obvious is the relative scarcity and cost of neutron sources, which typically take two forms: a research reactor or a spallation source (fed by a high energy proton accelerator). Another drawback is the time required to conduct a measurement, which can range from several hours to several days (per measurement). This is due to the short range of nuclear forces and relatively low probability of a scattering event, which is the same reason neutron radiation penetrates so effectively. Because of the long measurement time and high operational cost beam time is allocated very carefully at neutron sources, and flight paths are rarely left idle during neutron production. ND and INS require larger sample sizes,

We have studied the Cu-Li-Mg system as a hydrogen storage system and, at the same time, as a catalyst of the hydrogen storage process, namely for the Ti/TiH2 system (Braga & Malheiros, 2007a, 2007b; Braga et al., 2010a, 2010b). The only ternary compound the Cu-Li-Mg system holds is CuLixMg2-x (x = 0.08) with hexagonal P6222 structure (Braga et al., 2010c). Since the phase diagrams of Cu-Mg and Ni-Mg are similar (see Fig. 4), and Cu and Ni have similar electron affinities, it was thought in the sixties that CuMg2 would store

However this is not the case (Reilly & Wiswall, 1967). NiMg2 has a hexagonal structure (P6222), but CuMg2 has an orthorhombic structure (Fddd), and this structural difference is assumed to be the reason that NiMg2 stores H2 forming a hydride, but CuMg2 does not. CuMg2 decomposes into Cu2Mg and MgH2 (Reilly & Wiswall, 1967) upon hydrogen loading

hydride phases, and phase transitions which occur only in extreme conditions.

often multiple grams, to increase the scattering rate.

**2. Hydrides of Cu and Mg intermetallic systems** 

refinement method.

hydrogen, too.

Fig. 4. Phase diagrams of Ni-Mg and Cu-Mg (Ansara et al., 1998)

as previously referred (4). As a result of this reaction and since CuMg2 does not form a hydride, CuMg2 was abandoned as a candidate material for hydrogen storage (Reilly & Wiswall, 1967; Schlapbach & Züttel, 2001) until the late destabilization studies that were previously cited. The hexagonal structure of CuLixMg2-x, suggested the possibility of using this phase as a hydrogen storage material (Braga & Malheiros, 2007a, 2007b) because CuLixMg2-x has the same space group (P6222) as NiMg2 and NiMg2(H,D)0.3 (lattice parameters are almost identical: a = b = 5.250 Å and c = 13.621 Å (at 300 K) for CuLixMg2-x and a = b = 5.256 Å and c = 13.435 Å for NiMg2(H,D)0.3 (Senegas et al., 1984)). Therefore, we hypothesized that CuLixMg2-x (x = 0.08) would be a hydrogen storage material, just like NiMg2 - a hypothesis that has been confirmed by now (Braga & Malheiros, 2007a, 2007b; Braga et al., 2010a).

The change of the CuMg2 orthorhombic (Fddd) structure to a hexagonal structure (P6222) upon addition of a small amount of Li has been firmly established (Braga et al., 2007). Isostructural phases to CuLixMg2-x are the hexagonal phase NiMg2 and NiMg2H0.24-0.30 (Senegas et al., 1984). For the NiMg-hydrides, several hydrogen positions were reported: In NiMg2H0.29 the hydrogen atoms occupy Wyckoff 6f positions and could occupy the interstitial Wyckoff 6h position (Senegas et al., 1984). Other possibilities would be that the H atoms would just occupy interstitial Wyckoff 12k position (in NiMg2H0.26) or the Wyckoff 12k and 6j positions in NiMg2H0.24 (Senegas et al., 1984). This suggests a number of possible sites for Li in CuLixMg2-x.

Interestingly V. Hlukhyy and collaborators (Hlukhyy et al., 2005) have reported a result closely related to our observations in the Sn-doped Ni-Mg system. These authors show that the synthesis of alloys in the Ni-Mg system is affected by the presence of small amounts of Sn (forming NiMg2-xSnx with x = 0.22 and 0.40). The replacement of Mg by Sn produces changes in the structure of NiMg2, this time making the alloy change from the NiMg2 type (hexagonal) to the CuMg2 type (orthorhombic). While the structure of NiMg1.85Sn0.15 is still of NiMg2 type, the structure of NiMg1.78Sn0.22 and NiMg1.60Sn0.40 is already of the CuMg2 type. These results represent obviously the converse of our own observations in the CuMg2 structure, and reaffirm our results with respect to CuLixMg2-x.

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 13

obtained are in close agreement with those obtained from ND after Rietveld refinement - CuLixMg2-x (x = 0.08). Nonetheless, no conclusions about Li site occupancies could be drawn from the use of the referred means. DFT shows that there isn't a clear preference, in terms of energy, for the different Li site occupancies. Then again, a technique that gives information about the average site occupancies - like the Rietveld refinement - is also inadequate to clarify this problem; therefore we have used PDF to determine Li preferred sites. With PDF fittings we were allowed to go further (see Fig. 5b). PDF does not see the average but the local structure and with PDF, all results but those in which Li would substitute Mg1 sites (1/2, 0, z), gave negative occupancies for Li. For Li substituting Mg1 we've obtained an average composition for CuLixMg2-x (x = 0.07) which is in agreement with the other obtained results.

To study the hydrogen storage in the Cu-Li-Mg system several techniques were used (Braga et al., 2010a). Besides absorption/desorption, Differential Scanning Calorimetry, Thermal Gravimetry Analysis (DSC/TGA), X-ray Diffraction (XRD) both at the laboratory and at the Synchrotron, we have used Neutron Diffraction and Inelastic Neutron Scattering. Owing to the low X-ray scattering power of hydrogen, neutron diffraction experiments on deuterides

Most atomic arrangements were determined on powders of different samples yet we have also used a bulk sample machined into a cylinder to obtain ND data in both the surface and

The data were usually analyzed by the Rietveld method, yet in some cases in which the background was noisier we have used the biased method (Larson & von Dreele, 2004). For better convergence, the number of refined parameters in particular those of the atomic

ND results obtained from the High-Intensity Powder Diffractometer HIPD at LANSCE, Los Alamos National Laboratory, for a sample initially containing 78 wt.% CuLi0.08Mg1.92 + 22 wt.%Cu2Mg (from here on "initially containing" means before hydrogen/deuterium absorption) and that was deuterated *ex situ* at 473 K at P ≤ 50 atm in order to determine the crystal structure of the first deuteride phase formed in the sample (see Fig. 6 left). This

The CuLi0.08Mg1.92D5 crystal structure was determined to be monoclinic P121, with a = 15.14 Å, b = 6.88 Å, c = 5.55 Å and = 91.73º according to the formula CuLi0.08Mg1.92D5 = 0.5(Mg32+.[CuD4]23-.MgD2) corresponding to 4.4 wt% D per formula unit. CuLi0.08Mg1.92D5 is the first deuteride/hydride to be formed. This result is interesting by itself, but the presence of MgD2 in the diffraction pattern, highlights even further the possibilities of applications of this compound. According to these results, it can be obtained MgH(D)2 from a sample that did not contain "free" Mg or CuMg2. Furthermore, the deuteration process occurred at 473 K, which is considerably lower than the hydrogen absorption temperature reported for

The experiments with the bulk sample at SMARTS, LANSCE, Los Alamos National Laboratory, show that before MgD2 is observed, CuLi0.08Mg1.92D5 is already distinguishable at the surface even in a sample that initially contained CuMg2 (see Fig. 7). Therefore, it

For further information please see (Braga et al., 2010c).

**2.2 Hydrogen storage in the Cu-Li-Mg-H(D) system** 

are necessary as previously highlighted in section 1.5.

the center of the sample during deuterium uptake.

displacement amplitudes are reduced by constraints.

pattern was refined using Rietveld's method.

CuMg2 (4) (Reilly & Wiswall, 1967).

#### **2.1 The CuLi0.08Mg1.92 compound**

We have used neutron diffraction to refine the composition of CuLixMg2-x, site occupancies and lattice parameters at different temperatures. In Fig. 5, results from the Time-of-flight (TOF) Neutron Powder Diffractometer (NPDF) at the Los Alamos Neutron Science Center (LANSCE) are shown. It was analyzed a sample containing 37.5 at.% of CuLi0.08Mg1.92, 45.1 at.% of CuMg2 and 17.4 at.% of Cu2Mg. The structure was refined using the General Structure Analysis System (GSAS), a Rietveld profile analysis program developed by A. C. Larson and R. B. von Dreele (Larson & von Dreele, 2004).

Fig. 5. a) Neutron diffraction pattern of a sample containing CuLi0.08Mg1.92, CuMg2 and CuMg2. The highlighted peak corresponds to the (101) reflection for the CuLi0.08Mg1.92 compound which is not overlapped by other phases. b) Pair Distribution Function (PDF) fitting for the same conditions of the pattern in a).

Furthermore, we've fitted the NPDF data using the Pair Distribution Function (PDF) in which G(r) was obtained via the Fourier Transform of the total diffraction pattern as indicated below:

$$\mathcal{G}(r) = 4\pi r \mathbb{E}\left[\rho(r) - \rho\_0\right] = \frac{2}{r} \Big|\_{0}^{r} Q \Big[S(Q) - 1\Big] \sin(Qr) dQ \tag{9}$$

where *r* is the microscopic pair density, 0 is the average atomic number density, and r the radial distance. Q is the momentum transfer ( *Q* 4 sin / ). *S Q* is the normalized structure function determined from the experimental diffraction intensity (Egami & Billinge, 2003). PDF yields the probability of finding pairs of atoms separated by a distance r. PDF fittings were performed using the software PDFgui (Farrow et al., 2007).

Besides Neutron Diffraction, we have used theoretical complementary methods to determine the stoichiometry of the CuLixMg2-x compound. We relied on the Density Functional Theory (DFT) (Hohenberg & Kohn, 1964) to calculate the structure that minimized the Electronic Energy at 0 K, without accounting for the zero point energy. The latter energy gives us a good estimation of the Enthalpy of Formation at 0 K especially since we were relating data for stoichiometries that did not differ too much and for similar crystal structures. The results obtained are in close agreement with those obtained from ND after Rietveld refinement - CuLixMg2-x (x = 0.08). Nonetheless, no conclusions about Li site occupancies could be drawn from the use of the referred means. DFT shows that there isn't a clear preference, in terms of energy, for the different Li site occupancies. Then again, a technique that gives information about the average site occupancies - like the Rietveld refinement - is also inadequate to clarify this problem; therefore we have used PDF to determine Li preferred sites. With PDF fittings we were allowed to go further (see Fig. 5b). PDF does not see the average but the local structure and with PDF, all results but those in which Li would substitute Mg1 sites (1/2, 0, z), gave negative occupancies for Li. For Li substituting Mg1 we've obtained an average composition for CuLixMg2-x (x = 0.07) which is in agreement with the other obtained results. For further information please see (Braga et al., 2010c).

### **2.2 Hydrogen storage in the Cu-Li-Mg-H(D) system**

12 Neutron Diffraction

We have used neutron diffraction to refine the composition of CuLixMg2-x, site occupancies and lattice parameters at different temperatures. In Fig. 5, results from the Time-of-flight (TOF) Neutron Powder Diffractometer (NPDF) at the Los Alamos Neutron Science Center (LANSCE) are shown. It was analyzed a sample containing 37.5 at.% of CuLi0.08Mg1.92, 45.1 at.% of CuMg2 and 17.4 at.% of Cu2Mg. The structure was refined using the General Structure Analysis System (GSAS), a Rietveld profile analysis program developed by A. C.

Fig. 5. a) Neutron diffraction pattern of a sample containing CuLi0.08Mg1.92, CuMg2 and CuMg2. The highlighted peak corresponds to the (101) reflection for the CuLi0.08Mg1.92 compound which is not overlapped by other phases. b) Pair Distribution Function (PDF)

a)

Mg2-x

Furthermore, we've fitted the NPDF data using the Pair Distribution Function (PDF) in which G(r) was obtained via the Fourier Transform of the total diffraction pattern as indicated below:

> <sup>0</sup> 0 <sup>2</sup> *Gr r r* <sup>4</sup> *Q S Q Qr dQ* 1 sin *r*

normalized structure function determined from the experimental diffraction intensity (Egami & Billinge, 2003). PDF yields the probability of finding pairs of atoms separated by a distance r. PDF fittings were performed using the software PDFgui (Farrow et al., 2007).

Besides Neutron Diffraction, we have used theoretical complementary methods to determine the stoichiometry of the CuLixMg2-x compound. We relied on the Density Functional Theory (DFT) (Hohenberg & Kohn, 1964) to calculate the structure that minimized the Electronic Energy at 0 K, without accounting for the zero point energy. The latter energy gives us a good estimation of the Enthalpy of Formation at 0 K especially since we were relating data for stoichiometries that did not differ too much and for similar crystal structures. The results

(9)

0 is the average atomic number density, and

**(Å)**

). *S Q* is the

b)

 

 

r the radial distance. Q is the momentum transfer ( *Q* 4 sin /

**2.1 The CuLi0.08Mg1.92 compound** 

Larson and R. B. von Dreele (Larson & von Dreele, 2004).

CuLi0.083Mg1.917 (37.5 at%)

CuLi0.083Mg1.917 (37.5 at%)

Mg (17.4 at%)

Mg (17.4 at%)

(45.1 at%)

(45.1 at%)

**I obs Icalc Ibkg Iobs - Icalc**

(101) CuLix

**I obs Icalc Ibkg Iobs - Icalc**

fitting for the same conditions of the pattern in a).

1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5 5.0

1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5 5.0

+ CuMg2

+ CuMg2

**wRp = 0.0344 Rp = 0.0261**

**wRp = 0.0344 Rp = 0.0261**

**T = 300 K bank 46**

**T = 300 K bank 46**

+ Cu2

+ Cu2

**d (Å)**

**d (Å)**

*r* is the microscopic pair density,

where

0.0

0.0

0.5

0.5

1.0

1.0

1.5

1.5

**Normalized Intensity**

**Normalized Intensity**

2.0

2.0

2.5

2.5

To study the hydrogen storage in the Cu-Li-Mg system several techniques were used (Braga et al., 2010a). Besides absorption/desorption, Differential Scanning Calorimetry, Thermal Gravimetry Analysis (DSC/TGA), X-ray Diffraction (XRD) both at the laboratory and at the Synchrotron, we have used Neutron Diffraction and Inelastic Neutron Scattering. Owing to the low X-ray scattering power of hydrogen, neutron diffraction experiments on deuterides are necessary as previously highlighted in section 1.5.

Most atomic arrangements were determined on powders of different samples yet we have also used a bulk sample machined into a cylinder to obtain ND data in both the surface and the center of the sample during deuterium uptake.

The data were usually analyzed by the Rietveld method, yet in some cases in which the background was noisier we have used the biased method (Larson & von Dreele, 2004). For better convergence, the number of refined parameters in particular those of the atomic displacement amplitudes are reduced by constraints.

ND results obtained from the High-Intensity Powder Diffractometer HIPD at LANSCE, Los Alamos National Laboratory, for a sample initially containing 78 wt.% CuLi0.08Mg1.92 + 22 wt.%Cu2Mg (from here on "initially containing" means before hydrogen/deuterium absorption) and that was deuterated *ex situ* at 473 K at P ≤ 50 atm in order to determine the crystal structure of the first deuteride phase formed in the sample (see Fig. 6 left). This pattern was refined using Rietveld's method.

The CuLi0.08Mg1.92D5 crystal structure was determined to be monoclinic P121, with a = 15.14 Å, b = 6.88 Å, c = 5.55 Å and = 91.73º according to the formula CuLi0.08Mg1.92D5 = 0.5(Mg32+.[CuD4]23-.MgD2) corresponding to 4.4 wt% D per formula unit. CuLi0.08Mg1.92D5 is the first deuteride/hydride to be formed. This result is interesting by itself, but the presence of MgD2 in the diffraction pattern, highlights even further the possibilities of applications of this compound. According to these results, it can be obtained MgH(D)2 from a sample that did not contain "free" Mg or CuMg2. Furthermore, the deuteration process occurred at 473 K, which is considerably lower than the hydrogen absorption temperature reported for CuMg2 (4) (Reilly & Wiswall, 1967).

The experiments with the bulk sample at SMARTS, LANSCE, Los Alamos National Laboratory, show that before MgD2 is observed, CuLi0.08Mg1.92D5 is already distinguishable at the surface even in a sample that initially contained CuMg2 (see Fig. 7). Therefore, it

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 15

Fig. 8. ND refined pattern of the center and surface of a bulk cylinder sample initially containing CuLi0.08Mg1.92, Cu2Mg, and CuMg2 obtained in SMARTS during an *in situ* reaction with D2 at 523 K and ~34 atm. Besides the texture effect that might be present in a bulk sample, it seems that the center initially contained more CuLi0.08Mg1.92 than the surface.

light particles (Elsasser et al., 1998).

Experimental information about the metal–hydrogen interactions can be obtained by measuring lattice vibrations via INS, as previously highlighted in section 1.5. Because of the large difference between the masses of metal and H atoms in transition-metal–hydrogen systems, the acoustic dispersion branches of the phonon spectra can be attributed to the motion of the metal atoms, the optic branches to the vibrations of the light H atoms relative to the metal lattice. The densities of states of optic phonons typically show a pronounced maximum at the energy of the lattice vibrations at the point in the centre of the phonon Brillouin zone (*q* = 0) e.g. in (Fukay, 1993). These phonon modes describe the vibration of the undistorted H sublattice relative to the rigid metal sublattice. Hence, they contain the metal–hydrogen interaction only. This is usually stronger than the H–H interaction, which leads to the dispersion of the optic branches. In the limit of very low H concentrations, the H vibrations can be imagined as independent vibrations of local Einstein oscillators at interstitial H sites. For both the lattice vibrations at the point and the local vibrations, one can observe transitions from the ground state, the quantum-mechanical zero-point vibration of the H atoms, to the first excited states, e.g. by measuring optic phonon excitations, and transitions to higher excited states. Their energies, intensities and symmetry splittings yield an insight into the shapes of the potential and the wavefunctions for the vibrations of the

We have measured samples of the Cu-Li-Mg-H system by means of INS measured with the Filter Difference Spectrometer FDS, at LANSCE, Los Alamos National Laboratory. There is no doubt about the sequence of events; first there is the formation of CuLi0.08Mg1.92H5 (see Fig. 9a) and then in subsequent cycles the formation of MgH2 (see Fig. 9b), either for

DSC/TGA experiments show that CuLi0.08Mg1.92H5 starts desorbing hydrogen at 313 K to 328 K. In this range of temperatures the sample can release up to 1.3 wt.% (results for a isothermal experiment with a sample initially containing approximately 78 wt.% of CuLi0.08Mg1.92 and 22 wt.% of Cu2Mg - which does not absorb hydrogen at the temperature and pressure that were used). In Fig. 10 it can be seen that 0.5 wt.% of a sample initially containing 61 wt.%

disproportionation of CuLi0.08Mg1.92H5 or from hydrogenation of CuMg2.

Fig. 6. (left) Rietveld refinement of a sample containing CuLi0.08Mg1.92, Cu2Mg, MgD2 and CuLi0.08Mg1.92D5 obtained in HIPD. wRp and Rp are the reliability factors as defined in (Larson & von Dreele, 2004). (right) ND pattern of the center of a bulk cylinder sample containing CuLi0.08Mg1.92, Cu2Mg, CuMg2 obtained from the Spectrometer for Materials Research at Temperature and Stress SMARTS during an *in situ* reaction with D2 at 523 K and ~34 atm. Both patterns show experimental, refined and difference between experimental and calculated intensities.

Fig. 7. (left and right) ND pattern of the surface of a bulk cylinder sample initially containing CuLi0.08Mg1.92, Cu2Mg, and CuMg2 obtained in SMARTS during an *in situ* reaction with D2 at 523 K and ~34 atm. (right) it is highlighted that MgD2 cannot justify some existing peaks. Both patterns show experimental, refined and difference between experimental and calculated intensities.

seems that CuLi0.08Mg1.92D5 will have a catalytic and destabilizing roll that was additionally observed with the Ti/TiH2 systems (Braga et al., 2010b).

Fig. 6. (left) Rietveld refinement of a sample containing CuLi0.08Mg1.92, Cu2Mg, MgD2 and CuLi0.08Mg1.92D5 obtained in HIPD. wRp and Rp are the reliability factors as defined in (Larson & von Dreele, 2004). (right) ND pattern of the center of a bulk cylinder sample containing CuLi0.08Mg1.92, Cu2Mg, CuMg2 obtained from the Spectrometer for Materials Research at Temperature and Stress SMARTS during an *in situ* reaction with D2 at 523 K and ~34 atm. Both patterns show experimental, refined and difference between experimental

Fig. 7. (left and right) ND pattern of the surface of a bulk cylinder sample initially containing CuLi0.08Mg1.92, Cu2Mg, and CuMg2 obtained in SMARTS during an *in situ* reaction with D2 at 523 K and ~34 atm. (right) it is highlighted that MgD2 cannot justify some existing peaks. Both patterns show experimental, refined and difference between experimental and

seems that CuLi0.08Mg1.92D5 will have a catalytic and destabilizing roll that was additionally

and calculated intensities.

calculated intensities.

observed with the Ti/TiH2 systems (Braga et al., 2010b).

Fig. 8. ND refined pattern of the center and surface of a bulk cylinder sample initially containing CuLi0.08Mg1.92, Cu2Mg, and CuMg2 obtained in SMARTS during an *in situ* reaction with D2 at 523 K and ~34 atm. Besides the texture effect that might be present in a bulk sample, it seems that the center initially contained more CuLi0.08Mg1.92 than the surface.

Experimental information about the metal–hydrogen interactions can be obtained by measuring lattice vibrations via INS, as previously highlighted in section 1.5. Because of the large difference between the masses of metal and H atoms in transition-metal–hydrogen systems, the acoustic dispersion branches of the phonon spectra can be attributed to the motion of the metal atoms, the optic branches to the vibrations of the light H atoms relative to the metal lattice. The densities of states of optic phonons typically show a pronounced maximum at the energy of the lattice vibrations at the point in the centre of the phonon Brillouin zone (*q* = 0) e.g. in (Fukay, 1993). These phonon modes describe the vibration of the undistorted H sublattice relative to the rigid metal sublattice. Hence, they contain the metal–hydrogen interaction only. This is usually stronger than the H–H interaction, which leads to the dispersion of the optic branches. In the limit of very low H concentrations, the H vibrations can be imagined as independent vibrations of local Einstein oscillators at interstitial H sites. For both the lattice vibrations at the point and the local vibrations, one can observe transitions from the ground state, the quantum-mechanical zero-point vibration of the H atoms, to the first excited states, e.g. by measuring optic phonon excitations, and transitions to higher excited states. Their energies, intensities and symmetry splittings yield an insight into the shapes of the potential and the wavefunctions for the vibrations of the light particles (Elsasser et al., 1998).

We have measured samples of the Cu-Li-Mg-H system by means of INS measured with the Filter Difference Spectrometer FDS, at LANSCE, Los Alamos National Laboratory. There is no doubt about the sequence of events; first there is the formation of CuLi0.08Mg1.92H5 (see Fig. 9a) and then in subsequent cycles the formation of MgH2 (see Fig. 9b), either for disproportionation of CuLi0.08Mg1.92H5 or from hydrogenation of CuMg2.

DSC/TGA experiments show that CuLi0.08Mg1.92H5 starts desorbing hydrogen at 313 K to 328 K. In this range of temperatures the sample can release up to 1.3 wt.% (results for a isothermal experiment with a sample initially containing approximately 78 wt.% of CuLi0.08Mg1.92 and 22 wt.% of Cu2Mg - which does not absorb hydrogen at the temperature and pressure that were used). In Fig. 10 it can be seen that 0.5 wt.% of a sample initially containing 61 wt.%

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 17

The DSC/TGA results show that the system containing CuLi0.08Mg1.92 and Cu2Mg can destabilize MgH2 in a more efficient way than Cu2Mg by itself can. In fact, in a DSC experiment in which kinetics must be accounted for, MgH2 will release hydrogen at 553-573

A sample with 60.5 at% of CuLi0.08Mg1.92, 23.9 at% of CuMg2 and 15.6 at% of Cu2Mg was mechanically alloyed to titanium resulting into Cu-Li-Mg+Ti samples. The brittle CuLiMg alloy was mixed with Ti (99.9% purity, 325 mesh, Alfa Aesar) so that 68.2 at% / 47.3 wt% of the final mixture was Ti. The mixture was ball-milled for 3 h in a dry box under a He protective atmosphere. The Cu-Li-Mg+Ti mixture was then sealed inside a stainless steel crucible and kept at 473 K for 9h under D2 at P = 34 bar. These samples were then cooled to 5

**initial mixture:** (CuLi0.08Mg1.92, CuMg2

**hydrides (at 100 K):** CuLi0.08Mg1.92D5

, Cu2 Mg) + Ti

, MgD2

**1.8 1.9 2.0 2.1 2.2 2.3 2.4 2.5 2.6**

**from the init. mixture:** (CuLi0.08Mg1.92, CuMg2

**hydrides (at 300 K):** CuLi0.08Mg1.92D5

, Cu2 Mg)

, TiD2

**d(Å)**

Fig. 11. Comparison of Cu-Li-Mg+Ti-D neutron diffraction pattern refinements from

, Cu2 Mg)

, TiD2, MgD2

**1.2 1.4 1.6 1.8 2.0 2.2 2.4 2.6 2.8 3.0 3.2 3.4**

**d(Å)**

**0.0**

**0.2**

**0.4**

**Intensity (a.u.)**

**0.6**

**T = 300 K**

TiD2 - tetragonal TiD2 - cubic

measurements taken at T= 100K, 200K, and 300K.

**1.8 1.9 2.0 2.1 2.2 2.3 2.4 2.5 2.6**

**T = 200 K from the init. mixture:** (CuLi0.08Mg1.92, CuMg2

**hydrides (at 200 K):** CuLi0.08Mg1.92D5

**d(Å)**

**-0.1**

**0.0**

**0.2**

**Intensity (a.u.)**

**0.4**

**0.6**

**0.0**

**0.1**

**0.2**

**0.3**

**Intensity (a.u.)**

**0.4**

**0.5**

**0.6**

**0.7**

K, which can only be obtained when particles are reduced to nanopowders.

**2.3 Hydrogen storage in the Cu-Li-Mg-H(D)+Ti system** 

**T = 100 K**

K (HIPD, neutron powder diffraction) over a period of 2 to 3 hours.

Fig. 9. a) INS spectra for NiMg2H4 (1st and 2nd hydrogenation cycles) and for two samples containing CuLi0.08Mg1.92 (close circles below correspond to a sample that also contained Cu2Mg and the open circles above correspond to sample that contained Cu2Mg and CuMg2 as well). All samples show the formation of a similar monoclinic structure. As in NiMg2H4, in which Ni is bonded to four atoms of H forming the tetrahedral complex [NiH4]4-, Cu is also bonded to four atoms of H forming the tetrahedral complex [CuH4]3-, which was previously referred on (Yvon & Renaudin, 2005). b) Sample initially containing approximately 61 wt.% of CuLi0.08Mg1.92, 23 wt.% of CuMg2 and 16 wt.% of Cu2Mg, after the 3rd hydrogenation cycle at 473 K, and ~50 atm. It is clear the formation of MgH2 with a peak at ~620 cm-1.

Fig. 10. TGA of two samples initially containing approximately 61 wt.% of CuLi0.08Mg1.92, 23 wt.% of CuMg2 and 16 wt.% of Cu2Mg. Samples were measured after hydrogenation but they are not expected to be saturated in hydrogen prior to the experiment.

of CuLi0.08Mg1.92, 23 wt.% of CuMg2 and 16 wt.% of Cu2Mg can be released at T < 350 K. In spite of the fact that there was some visible oxidation during this run, we think it was worth showing this initial desorption. This initial desorption seems to be due to CuLi0.08Mg1.92H5. At ~473 K, hydrogen starts to be desorbed at a different rate, probably due to the disproportionation of CuLi0.08Mg1.92H5, with the formation of MgH2, which will start releasing hydrogen at 553-573 K. Additionally, MgH2 can be formed upon hydrogenation of CuMg2.

The DSC/TGA results show that the system containing CuLi0.08Mg1.92 and Cu2Mg can destabilize MgH2 in a more efficient way than Cu2Mg by itself can. In fact, in a DSC experiment in which kinetics must be accounted for, MgH2 will release hydrogen at 553-573 K, which can only be obtained when particles are reduced to nanopowders.

#### **2.3 Hydrogen storage in the Cu-Li-Mg-H(D)+Ti system**

16 Neutron Diffraction

**0.00 0.25 0.50 0.75 1.00 1.25 1.50 1.75 2.00**

a) b)

**300 350 400 450 500 550 600 650 700**

Fig. 10. TGA of two samples initially containing approximately 61 wt.% of CuLi0.08Mg1.92, 23 wt.% of CuMg2 and 16 wt.% of Cu2Mg. Samples were measured after hydrogenation but

of CuLi0.08Mg1.92, 23 wt.% of CuMg2 and 16 wt.% of Cu2Mg can be released at T < 350 K. In spite of the fact that there was some visible oxidation during this run, we think it was worth showing this initial desorption. This initial desorption seems to be due to CuLi0.08Mg1.92H5. At ~473 K, hydrogen starts to be desorbed at a different rate, probably due to the disproportionation of CuLi0.08Mg1.92H5, with the formation of MgH2, which will start releasing hydrogen at 553-573 K. Additionally, MgH2 can be formed upon hydrogenation of CuMg2.

**T (K**)

**1.6 wt.%**

**1.4 wt.%**

**~473 K** 

Fig. 9. a) INS spectra for NiMg2H4 (1st and 2nd hydrogenation cycles) and for two samples containing CuLi0.08Mg1.92 (close circles below correspond to a sample that also contained Cu2Mg and the open circles above correspond to sample that contained Cu2Mg and CuMg2 as well). All samples show the formation of a similar monoclinic structure. As in NiMg2H4, in which Ni is bonded to four atoms of H forming the tetrahedral complex [NiH4]4-, Cu is also bonded to four atoms of H forming the tetrahedral complex [CuH4]3-, which was previously referred on (Yvon & Renaudin, 2005). b) Sample initially containing approximately 61 wt.% of CuLi0.08Mg1.92, 23 wt.% of CuMg2 and 16 wt.% of Cu2Mg, after the 3rd hydrogenation cycle at

473 K, and ~50 atm. It is clear the formation of MgH2 with a peak at ~620 cm-1.

**315 K**

**0.5 wt.%**

they are not expected to be saturated in hydrogen prior to the experiment.

**I (a. u.)**

**400 600 800 1000 1200 1400 1600 1800 2000**

**wavenumber (cm-1)**

**400 600 800 1000 1200 1400 1600 1800 2000**

**wavenumber** (**cm-1**)

**97.4 97.6 97.8 98.0 98.2 98.4 98.6 98.8 99.0 99.2 99.4**

**m (wt.%)**

**NiMg2H4 1st cycle CuLixMg2-x-H 1st cycle NiMg2H4 2nd cycle CuLixMg2-x-H 1st cycle** 

**I (a. u.)**

A sample with 60.5 at% of CuLi0.08Mg1.92, 23.9 at% of CuMg2 and 15.6 at% of Cu2Mg was mechanically alloyed to titanium resulting into Cu-Li-Mg+Ti samples. The brittle CuLiMg alloy was mixed with Ti (99.9% purity, 325 mesh, Alfa Aesar) so that 68.2 at% / 47.3 wt% of the final mixture was Ti. The mixture was ball-milled for 3 h in a dry box under a He protective atmosphere. The Cu-Li-Mg+Ti mixture was then sealed inside a stainless steel crucible and kept at 473 K for 9h under D2 at P = 34 bar. These samples were then cooled to 5 K (HIPD, neutron powder diffraction) over a period of 2 to 3 hours.

Fig. 11. Comparison of Cu-Li-Mg+Ti-D neutron diffraction pattern refinements from measurements taken at T= 100K, 200K, and 300K.

Hydrides of Cu and Mg Intermetallic Systems: Characterization and Catalytic Function 19

would like to acknowledge the Lujan Center's, LANSCE, instrument scientists for their

Aguey-Zinsou, K. & Ares-Fernández, J. (2010). Hydrogen in magnesium: new perspectives

Alapati, S., Johnson, J. & Sholl, D. (2007). Using first principles calculations to identify new

Andreasen, A., Sørensen, M., Burkarl, R., Møller, B., Molenbroek, A., Pedersen, A., Vegge, T.

Ansara, I., Dinsdale, A. & Rand, M. (Ed(s)). (1998). *COST 507, Thermochemical database for* 

Beattie, S., Setthanan, U. & McGrady, G. (2011). Thermal desorption of hydrogen from

Bösenberg, U., Ravnsbæk, D., Hagemann, H., D'Anna, V., Minella, B., Pistidda, C., Beek, W.,

Braga, M., Acatrinei, A., Hartl, M., Vogel, S., Proffen, T. & Daemen, L. (2010a). New

Braga, M., Ferreira, J., Siewenie, J., Proffen, Th., Vogel, S. & Daemen, L. (2010c). Neutron

Braga, M. & Malheiros, L. (2007a). CuMg2-YLiX alloy for hydrogen storage. International

Braga, M. & Malheiros, L. (2007b). CuMg2-YLiX alloy for hydrogen storage. National patent,

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2010), pp. 526-543, ISSN 1754-5706

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ISSN 1932-7455

ISSN 0272-9172

PT 103368 (A)

**5. References** 

Cu-Li-Mg+Ti-D neutron diffraction samples were quenched and measured at the lowest temperature, 5K, first with 60K, 100K, 200K and 300K measurements taken subsequently. For diffraction patterns collected at 5K – 100K there is *no evidence* of any titanium deuteride phases. This is immediately obvious in Fig. 11 which shows a comparison of the 100, 200 and 300 K Cu-Li-Mg+Ti-D. Bragg peaks belonging to tetragonal TiD2 begin to appear in the 200K pattern of the Cu-Li-Mg+Ti-D sample. The refinement at 100 K includes the 5 phases: CuMg2, Cu2Mg, CuLi0.08Mg1.92, CuLi0.08Mg1.92D5 and α-Ti; at 200 K: CuMg2, Cu2Mg, CuLi0.08Mg1.92, CuLi0.08Mg1.92D5 and MgD2 plus tetragonal TiD2 and at 300 K: CuMg2, Cu2Mg, CuLi0.08Mg1.92, CuLi0.08Mg1.92D5 plus cubic TiD2 and represents an excellent fit to the data as confirmed by the residual. At 300K a structural phase transition (tetragonal to cubic) occurs in TiD2 (Yakel*,* 1958). The appearance of the TiD2 cubic phase in the 300K diffraction pattern is confirmed by refinement as shown in Fig. 11.

Fig. 11 shows the changes in the Cu-Li-Mg+Ti-D sample as the temperature is increased from 100K to 300K: The CuLi0.08Mg1.92D5, MgD2 and α-Ti phases are progressively reduced in intensity while TiD2 appears at 200K transforming from tetragonal to cubic at 300K. Since there was no further exposure of the sample to deuterium, the formation of TiD2 must have been facilitated through *solid state diffusion* of deuterium from a separate phase. The decrease in intensity of Bragg peaks belonging to the Cu-Li-Mg-D phase implicates that the mechanism involves solid state transfer of deuterium from Cu-Li-Mg-D to Ti.

DSC/TGA measurements show the dehydrogenation of CuLi0.08Mg1.92H5 accounts for approximately third of the total mass loss. Given that no other hydride phases were present in any significant quantity, and that MgH2 began dehydrogenation at 553 K in the Cu-Li-Mg-H samples, the mass loss beginning at 590 K is due to the release of hydrogen from TiH2. This demonstrates a significant catalytic effect for desorption as well given that TiH2 ordinarily does not dissociate until well above 723 K (Gibb & Kruschwitz, 1950). For further information please check (Braga et al., 2010b).

### **3. Conclusion**

The hydrogen storage world still offers a considerable amount of challenges since no universal solution has been found. Eventually, different solutions will be proposed to suite different applications.

The Cu-Li-Mg system provides other possibilities for catalytic and destabilization effects yet not fully explored.

There are several techniques that can be employed to study systems containing hydrogen. Nonetheless, Neutron Scattering is a very useful resource, in particular, Neutron Diffraction. In the latter, crystal structure of deuteride phases are directly studied since deuterium can be detected by ND and accurate results can be obtained either in *ex situ* or *in situ* experiments as shown previously.

### **4. Acknowledgments**

The authors would like to acknowledge FCT – Portugal and FEDER - EU, for the PTDC/CTM/099461/2008 project. This work has benefited from the use of HIPD, NPDF, SMARTS and FDS at LANSCE, LANL, funded by DOE, DE-AC52-06NA25396. The authors would like to acknowledge the Lujan Center's, LANSCE, instrument scientists for their support and helpful discussions.

### **5. References**

18 Neutron Diffraction

Cu-Li-Mg+Ti-D neutron diffraction samples were quenched and measured at the lowest temperature, 5K, first with 60K, 100K, 200K and 300K measurements taken subsequently. For diffraction patterns collected at 5K – 100K there is *no evidence* of any titanium deuteride phases. This is immediately obvious in Fig. 11 which shows a comparison of the 100, 200 and 300 K Cu-Li-Mg+Ti-D. Bragg peaks belonging to tetragonal TiD2 begin to appear in the 200K pattern of the Cu-Li-Mg+Ti-D sample. The refinement at 100 K includes the 5 phases: CuMg2, Cu2Mg, CuLi0.08Mg1.92, CuLi0.08Mg1.92D5 and α-Ti; at 200 K: CuMg2, Cu2Mg, CuLi0.08Mg1.92, CuLi0.08Mg1.92D5 and MgD2 plus tetragonal TiD2 and at 300 K: CuMg2, Cu2Mg, CuLi0.08Mg1.92, CuLi0.08Mg1.92D5 plus cubic TiD2 and represents an excellent fit to the data as confirmed by the residual. At 300K a structural phase transition (tetragonal to cubic) occurs in TiD2 (Yakel*,* 1958). The appearance of the TiD2 cubic phase in the 300K diffraction

Fig. 11 shows the changes in the Cu-Li-Mg+Ti-D sample as the temperature is increased from 100K to 300K: The CuLi0.08Mg1.92D5, MgD2 and α-Ti phases are progressively reduced in intensity while TiD2 appears at 200K transforming from tetragonal to cubic at 300K. Since there was no further exposure of the sample to deuterium, the formation of TiD2 must have been facilitated through *solid state diffusion* of deuterium from a separate phase. The decrease in intensity of Bragg peaks belonging to the Cu-Li-Mg-D phase implicates that the

DSC/TGA measurements show the dehydrogenation of CuLi0.08Mg1.92H5 accounts for approximately third of the total mass loss. Given that no other hydride phases were present in any significant quantity, and that MgH2 began dehydrogenation at 553 K in the Cu-Li-Mg-H samples, the mass loss beginning at 590 K is due to the release of hydrogen from TiH2. This demonstrates a significant catalytic effect for desorption as well given that TiH2 ordinarily does not dissociate until well above 723 K (Gibb & Kruschwitz, 1950). For further

The hydrogen storage world still offers a considerable amount of challenges since no universal solution has been found. Eventually, different solutions will be proposed to suite

The Cu-Li-Mg system provides other possibilities for catalytic and destabilization effects yet

There are several techniques that can be employed to study systems containing hydrogen. Nonetheless, Neutron Scattering is a very useful resource, in particular, Neutron Diffraction. In the latter, crystal structure of deuteride phases are directly studied since deuterium can be detected by ND and accurate results can be obtained either in *ex situ* or *in situ*

The authors would like to acknowledge FCT – Portugal and FEDER - EU, for the PTDC/CTM/099461/2008 project. This work has benefited from the use of HIPD, NPDF, SMARTS and FDS at LANSCE, LANL, funded by DOE, DE-AC52-06NA25396. The authors

mechanism involves solid state transfer of deuterium from Cu-Li-Mg-D to Ti.

pattern is confirmed by refinement as shown in Fig. 11.

information please check (Braga et al., 2010b).

**3. Conclusion** 

different applications.

experiments as shown previously.

**4. Acknowledgments** 

not fully explored.


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**2** 

*1,2,3,5USA 4Australia* 

**Neutron Diffraction Measurements** 

Xiaohua Cheng1,\*, Henry J. Prask2,3, Thomas Gnaeupel-Herold2,3,

The primary objective of the current study was to quantify the magnitude and distribution of residual stresses in various welded details in non-magnetic super-austenitic AL-6XN stainless steel I-beams through saw cutting and neutron diffraction methods. The welded details included transverse groove welds and simulated bulkhead attachment welded details, both of which duplicated details in previous fatigue test specimens [Fisher et al., 2001; Cheng et al., 2003a]. It was expected that the results of a study of residual stresses could be used to analyze the effect of residual stresses on fatigue strength. This Chapter presents a description of specimen materials, specimen preparation, neutron diffraction

Residual stresses are introduced into structural steel components during manufacturing and fabricating processes. For welded structures, weld process, weld sequence, component size and setup restraint, temperature or cooling rate difference, and material composition and properties are primary factors that affect residual stresses. Residual stresses can have significant impact on ultimate strength, stability, fatigue strength and toughness depending on their magnitude and distribution with respect to stresses from applied external loads and

**1. Introduction** 

**2.1 Background** 

dead loads.

 \*

measurement plan, method and results.

**2. Background, materials and testing methods** 

 formerly with ATLSS Reserach Center, Lehigh University, USA \*\* formerly with NIST Center for Neutron Research, USA

**for Residual Stresses in AL-6XN** 

**Stainless Steel Welded Beams** 

*1New Jersey Department of Transportation, Trenton, NJ 2NIST Center for Neutron Research, Gaithersburg, MD* 

*4Australian Nuclear Science & Technology Organization 5ATLSS Research Center, Lehigh University, Bethlehem, PA* 

Vladimir Luzin4,\*\* and John W. Fisher5

*3University of Maryland, College Park, MD* 

*Hydrogen Energy,* (In press - available online 20 July 2011), doi:10.1016/j.ijhydene.2011.05.143, ISSN 0360-3199

