Influence of Synthesis Gas Components on Hydrogen Storage Properties of Sodium Aluminum Hexahydride

A systematic study of different ratios of CO, CO2, N2 gas components on the hydrogen storage properties of the Na3AlH6 complex hydride with 4 mol% TiCl3, 8 mol% aluminum and 8 mol% activated carbon is presented in this paper. The different concentrations of CO and CO2 in H2 and CO, CO2, N2 in H2 mixture were investigated. Both CO and CO2 gas react with the complex hydride forming Al oxy-compounds, NaOH and Na2CO3 that consequently cause serious decline in hydrogen storage capacity. These reactions lead to irreversible damage of complex hydride under the current experimental condition. Thus, after 10 cycles with 0.1 vol % CO + 99.9 vol %H2 and 1 vol % CO + 99 vol %H2, the dehydrogenation storage capacity of the composite material decreased by 17.2% and 57.3%, respectively. In the case of investigation of 10 cycles with 1 vol % CO2 + 99 vol % H2 gas mixture, the capacity degradation was 53.5%. After 2 cycles with 10 vol % CO +90 vol % H2, full degradation was observed, whereas after 6 cycles with 10 vol % CO2 + 90 vol % H2, degradation of 86.8% was measured. While testing with the gas mixture of 1.5 vol % CO + 10 vol % CO2 + 27 vol % H2 + 61.5 vol % N2, the degradation of 94% after 6 cycles was shown. According to these results, it must be concluded that complex aluminum hydrides cannot be used for the absorption of hydrogen from syngas mixtures without thorough purification.


Introduction
Hydrogen storage is a key enabling technology for bringing forward hydrogen and fuel cell technologies in applications including transportation, stationary and portable power. For these applications, the volumetric and gravimetric hydrogen storage capacities are essential. Hydrogen can be physically stored as a gas under high pressure (35-70 MPa in high-pressure tanks) or as a liquid at cryogenic temperatures, since hydrogen boils at 20 K at ambient pressure. Besides, hydrogen can be stored in materials by adsorption (in the high surface solids, e.g., carbon materials or metal organic frameworks (MOFs) at temperatures < 77 K) or absorption (within solids, e.g., metal hydrides, complex metal hydrides, and alloys). In comparison to other methods, storage of absorbed hydrogen within metal hydrides or complex metal hydrides can offer high volumetric storage capacity up to 150 kg m −3 [1,2].
Sodium aluminum hexahydride-Na 3 AlH 6 with Ti catalysts was tested in our prior research as a storage material for the use in a lightweight aluminum alloy storage tank [3]. It was shown that the storage material could practically absorb/release up to 2.0 wt % of hydrogen during the hydrogenation/dehydrogenation processes. Although the material exhibits stable behavior of the kinetics performance, the capacity and the cyclic stability of the material still needs further optimization for commercial applications. Hydrogen which Hydrogen 2021, 2 148 can be used for recharging metal hydrides is a constituent of synthesis gas that is usually generated by the endothermic steam reforming of hydrocarbons, partial oxidation of methane, or gasification of coal and biomass [4,5]. The majority of hydrogen is produced by steam reforming of natural gas that is reacting with steam in the presence of Ni catalyst [6] as follows (Equation (1)): Partial oxidation of methane occurs when a sub-stoichiometric fuel-air mixture combusted forming a hydrogen-rich synthesis gas in an exothermic process according to Equation (2) [7]: Autothermal reforming combines the steam reforming process and fuel oxidation in one unit. The energy for the endothermic steam reforming is provided by the exothermic oxidation resulting in an overall reaction enthalpy close to zero (Equation (3)) [8]: During the above-mentioned synthesis gas processes, various gas compositions can be expected at the outlet of the appropriate reactor [9]. The resulting gas contents are shown in Table 1. The highest hydrogen content can be achieved during steam reforming and the lowest hydrogen content in the partial oxidation process. The synthesis gas components such as CO, CO 2 , CH 4 , N 2 , and H 2 O are suspected to be harmful for complex metal hydrides. Limited information could be found on the influence of these gas constituencies on complex metal hydrides. In 2007, Sandia National Laboratories published the results of reactivity of sodium alanate with O 2 , H 2 O, and CO 2 . It was shown that sodium alanate reacts exothermically with H 2 O and O 2 producing various Na-O compounds and H 2 [10]. The gas-solid reaction of CO 2 with alanates was investigated by Hugelshofer et al. where the authors observed the formation of intermediates like aluminum formate and methoxy compounds which then got converted into methane and metal oxides as final products [11]. The influences of gas components on other metal hydrides are well investigated [12][13][14][15][16][17][18][19][20][21][22][23][24]. In this work, the influence of different ratios of CO, CO 2 , N 2 on the hydrogen storage performance of the complex metal hydride Na 3 AlH 6 with 4 mol% TiCl 3 , 8 mol% aluminum and 8 mol% activated carbon is explored.
Cycling tests of the composite were carried out in a fully automated Sieverts instrument PCTPro 2000 (SETARAM Inc., Caluire, France). Then, 2.0 g of material was used for each test. Hydrogenations were done at 2.5 MPa hydrogen pressure at 170 • C and dehydrogenations at 0.1 MPa at 170 • C. The XRD measurement was performed on the STOE STADI P (Cu-Kα radiation, 1.541 Å) in a 0.5 mm diameter capillary filled with purified argon (both H 2 O and O 2 < 1 ppm). The IR-Spectrum measurements of the gaseous products were performed with a NICOLET MAGNA 560 FTIR spectrometer using Smart OMNI-Transmission cell with KBr windows. The gas sample was taken directly from the autoclave to the gas bag, being subsequently transferred into the Smart OMNI-Transmission cell. The gas phase spectra were taken at room temperature. Handling of the material was done in the MBraun glove box, in Argon atmosphere where oxygen and water levels always kept below 1 ppm.
The solid-state 13 C NMR spectra were recorded on a Bruker Avance III HD 500WB spectrometer using a double-bearing magic angle spinning (MAS) probe (DVT BL4) at a resonance frequency of 125.8 MHz. The experimental conditions for 13 C CP MAS NMR were as follows: 10-12 kHz spinning rate, 3 s recycle delay, 20,000-52,000 scans, 2 ms contact time, 3.3 µs 1 H π/2 pulse, and high-power proton decoupling (spinal64). The 13 C chemical shift was referenced with respect to neat TMS in a separate rotor.
The hydrogenation and dehydrogenation cycles with gas mixtures were performed on a test rig shown in Figure 1. The autoclave was charged with a total pressure of 3.0 MPa of pure hydrogen or gas mixtures (Table 2) except of 11.0 MPa for the gas mixture in 7 (Table 2). Gas mixture 7 was used as an example for autothermal syngas production from propane/butane mixtures of a commercial system. All gas mixtures were prepared in house. The autoclave was heated using a JUMO controller. The pressure inside the autoclave was monitored by JUMO pressure sensor and the temperature by a type K thermocouple. After the hydrogenation test, the hydrogen or gas mixture overpressure was released through the overpressure release valve. Immediately after releasing the gas pressure, desorbed hydrogen was collected and measured using a calibrated gas burette.

Hydrogen Storage Performance of the Na3AlH6 Composite Material in Pure Hydrogen
Activated carbon (8 mol%) and aluminum (8 mol%) were added to Na3AlH6 and TiCl3 (4 mol%) to enhance heat transfer of the composite material, which could improve the hydrogenation and dehydrogenation kinetic as well as dispersion, which can prevent the material from sintering during long time cycling. The other reason for addition of aluminum is that the forming of Ti-Al alloy during doping processes would consume part of Al from Na3AlH6. To replace this consumed Al metal and as the result to maintain the reversibility of the system, the amount of 8 mol% Al is added [25].
Here, we define that one "cycle" includes one hydrogenation and one dehydrogena-  Activated carbon (8 mol%) and aluminum (8 mol%) were added to Na 3 AlH 6 and TiCl 3 (4 mol%) to enhance heat transfer of the composite material, which could improve the hydrogenation and dehydrogenation kinetic as well as dispersion, which can prevent the material from sintering during long time cycling. The other reason for addition of aluminum is that the forming of Ti-Al alloy during doping processes would consume part of Al from Na 3 AlH 6 . To replace this consumed Al metal and as the result to maintain the reversibility of the system, the amount of 8 mol% Al is added [25].
Here, we define that one "cycle" includes one hydrogenation and one dehydrogenation process. A complete cycle takes 4 h, including 2 h of hydrogenation and 2 h of dehydrogenation. As shown in Figure 2, 187 cycles were achieved without notable degradation. Every hydrogenation cycle was performed at 2.5 MPa hydrogen pressure and 170 • C, while every dehydrogenation cycle was performed at 0.1 MPa pressure and 170 • C. Then, 2.15 ± 0.02 wt % of hydrogen was evolved and absorbed during hydrogenation or dehydrogenation. This value will be used as hydrogen normalized capacity in cycling experiments. In our prior research, the hydrogen capacity of the composite without additives of Al and activated carbon was less than 1.7 wt % [26]. Addition of activated carbon and Al has improved stability and hydrogen storage capacity of the composite by more than 30% and therefore confirmed the benefits of these additives. In general, the addition of carbon materials to metal hydride compounds results in improved kinetics of dehydrogenation and hydrogenation and the ability to transport and to release the produced heat during the reaction with hydrogen [27]. Table 3 shows the dehydrogenation H 2 capacity (0.1 MPa dehydrogenation pressure) of samples hydrogenated for 0.5, 1, and 2 h. The dehydrogenation time was varied between 1, 2, and 3 h. The hydrogenation and dehydrogenation temperatures were changed between 180 and 150 • C. It can be observed, that when temperature is higher than or equal to 160 • C, only 1 h is needed to fully hydrogenate the material at 3.0 MPa or dehydrogenate the material at 0.1 MPa. Increasing hydrogenation or dehydrogenation time to 2 or 3 h does not improve or only slightly improves the hydrogen capacity. At 150 • C, extending of hydrogenation and dehydrogenation time is necessary to obtain higher H 2 capacity. As result of these investigations, it was concluded to perform the cycling experiments with synthesis gas components at 170 • C and use 1 h for hydrogenation and 1 h for dehydrogenation processes.  Table 3 shows the dehydrogenation H2 capacity (0.1 MPa dehydrogenation pressure) of samples hydrogenated for 0.5, 1, and 2 h. The dehydrogenation time was varied between 1, 2, and 3 h. The hydrogenation and dehydrogenation temperatures were changed between 180 and 150 °C. It can be observed, that when temperature is higher than or equal to 160 °C, only 1 h is needed to fully hydrogenate the material at 3.0 MPa or dehydrogenate the material at 0.1 MPa. Increasing hydrogenation or dehydrogenation time to 2 or 3 h does not improve or only slightly improves the hydrogen capacity. At 150 °C, extending of hydrogenation and dehydrogenation time is necessary to obtain higher H2 capacity. As result of these investigations, it was concluded to perform the cycling experiments with synthesis gas components at 170 °C and use 1 h for hydrogenation and 1 h for dehydrogenation processes.    Figure 3 shows the hydrogen storage performance of the composite material in different ratios of CO and H 2 gas mixture. After 10 cycles with 0.1 vol % CO + 99.9 vol %H 2 and 1 vol % CO + 99 vol %H 2 , the dehydrogenation storage capacity of the composite material decreased by 17.2% and 57.3%, respectively. The sample cycled with 10 vol % Hydrogen 2021, 2 152 CO + 90 vol % H 2 gas mixture shows the most severe degradation. There was almost no hydrogen released after only 2 cycles after hydrogenation with 10 vol % CO + 90 vol % H 2 gas mixture. Attempts to recharge the sample with 5 MPa of pure hydrogen failed, which means that the changes during the cycling with the gas contained 10 vol % CO seem to be irreversible. Figure 4 shows the X-ray diffraction pattern of the doped Na 3 AH 6 material after treatment with different amounts of CO in H 2 . It can be seen that Na oxides were formed after 10 cycles with 0.1 vol % CO + 99.9 vol % H 2 and 1 vol % CO + 99 vol % H 2 . In case of 10 vol % CO + 90 vol % H 2 mixture, the formation of NaOH can be observed just after 2 cycles. The peak intensity ratio of Al:NaCl at around 45 • (2θ) becomes smaller when the concentration of CO increases in the gas mixture. The Al peak with 10 vol % CO + 90 vol % H 2 sample almost disappears after 2 cycles. As shown in the embedded enlarged Figure 4, a new weak reflection at round 37.4 • (2θ) appeared. This peak may belong to some kind of Al oxygenates.
In order to get more information about the weak reflection at round 37.4 • (2θ) observed in the X-ray diffraction pattern of Figure 4, we measured a carbon solid state NMRspectrum. Figure 5 shows the 13 C CP/MAS NMR spectrum of Ti-doped Na 3 AlH 6 after the second hydrogenation with 10 vol % CO + 90 vol % H 2 gas mixture. The most intense and asymmetric line at about 51 ppm in the 13 C NMR spectrum in Figure 5 can be assigned to methoxy groups (O-CH 3 ) [28]. These methoxy groups can be connected to Al-and/or Naatoms. The observation of O-CH 3 -groups also confirms the detection of Al-O-compounds in the X-ray diffraction pattern in Figure 4. The high-field line at about −8 ppm stems most likely from methyl groups directly bound to aluminum atoms [29]. The spectral intensity between 10 and 40 ppm is partly due to a small background signal of the probe.  Figure 3 shows the hydrogen storage performance of the composite material in different ratios of CO and H2 gas mixture. After 10 cycles with 0.1 vol % CO + 99.9 vol %H2 and 1 vol % CO + 99 vol %H2, the dehydrogenation storage capacity of the composite material decreased by 17.2% and 57.3%, respectively. The sample cycled with 10 vol % CO + 90 vol % H2 gas mixture shows the most severe degradation. There was almost no hydrogen released after only 2 cycles after hydrogenation with 10 vol % CO + 90 vol % H2 gas mixture. Attempts to recharge the sample with 5 MPa of pure hydrogen failed, which means that the changes during the cycling with the gas contained 10 vol % CO seem to be irreversible. Figure 4 shows the X-ray diffraction pattern of the doped Na3AH6 material after treatment with different amounts of CO in H2. It can be seen that Na oxides were formed after 10 cycles with 0.1 vol % CO + 99.9 vol % H2 and 1 vol % CO + 99 vol % H2. In case of 10 vol % CO + 90 vol % H2 mixture, the formation of NaOH can be observed just after 2 cycles. The peak intensity ratio of Al:NaCl at around 45°(2θ) becomes smaller when the concentration of CO increases in the gas mixture. The Al peak with 10 vol % CO + 90 vol % H2 sample almost disappears after 2 cycles. As shown in the embedded enlarged Figure 4, a new weak reflection at round 37.4° (2θ) appeared. This peak may belong to some kind of Al oxygenates. with different CO + H2 ratios. All samples were hydrogenated and dehydrogenated in pure hydrogen twice ("activation 1 (act 1) and activation 2 (act 2)) before cycling in the gas mixture.

The Influence of CO Gas on the Cycling Behavior of the Ti-Doped Na3AlH6
Pure H2, 0.1 vol % CO + 99.9 vol % H2, 1 vol % CO + 99 vol % H2, 10 vol % CO + 90 vol % H2. All samples were hydrogenated and dehydrogenated in pure hydrogen twice ("activation 1 (act 1) and activation 2 (act 2)) before cycling in the gas mixture.  Figure 3 shows the hydrogen storage performance of the composite material in different ratios of CO and H2 gas mixture. After 10 cycles with 0.1 vol % CO + 99.9 vol %H2 and 1 vol % CO + 99 vol %H2, the dehydrogenation storage capacity of the composite material decreased by 17.2% and 57.3%, respectively. The sample cycled with 10 vol % CO + 90 vol % H2 gas mixture shows the most severe degradation. There was almost no hydrogen released after only 2 cycles after hydrogenation with 10 vol % CO + 90 vol % H2 gas mixture. Attempts to recharge the sample with 5 MPa of pure hydrogen failed, which means that the changes during the cycling with the gas contained 10 vol % CO seem to be irreversible. Figure 4 shows the X-ray diffraction pattern of the doped Na3AH6 material after treatment with different amounts of CO in H2. It can be seen that Na oxides were formed after 10 cycles with 0.1 vol % CO + 99.9 vol % H2 and 1 vol % CO + 99 vol % H2. In case of 10 vol % CO + 90 vol % H2 mixture, the formation of NaOH can be observed just after 2 cycles. The peak intensity ratio of Al:NaCl at around 45°(2θ) becomes smaller when the concentration of CO increases in the gas mixture. The Al peak with 10 vol % CO + 90 vol % H2 sample almost disappears after 2 cycles. As shown in the embedded enlarged Figure 4, a new weak reflection at round 37.4° (2θ) appeared. This peak may belong to some kind of Al oxygenates. with different CO + H2 ratios. All samples were hydrogenated and dehydrogenated in pure hydrogen twice ("activation 1 (act 1) and activation 2 (act 2)) before cycling in the gas mixture.
Pure  Figure 3 shows the hydrogen storage performance of the composite material in different ratios of CO and H2 gas mixture. After 10 cycles with 0.1 vol % CO + 99.9 vol %H2 and 1 vol % CO + 99 vol %H2, the dehydrogenation storage capacity of the composite material decreased by 17.2% and 57.3%, respectively. The sample cycled with 10 vol % CO + 90 vol % H2 gas mixture shows the most severe degradation. There was almost no hydrogen released after only 2 cycles after hydrogenation with 10 vol % CO + 90 vol % H2 gas mixture. Attempts to recharge the sample with 5 MPa of pure hydrogen failed, which means that the changes during the cycling with the gas contained 10 vol % CO seem to be irreversible. Figure 4 shows the X-ray diffraction pattern of the doped Na3AH6 material after treatment with different amounts of CO in H2. It can be seen that Na oxides were formed after 10 cycles with 0.1 vol % CO + 99.9 vol % H2 and 1 vol % CO + 99 vol % H2. In case of 10 vol % CO + 90 vol % H2 mixture, the formation of NaOH can be observed just after 2 cycles. The peak intensity ratio of Al:NaCl at around 45°(2θ) becomes smaller when the concentration of CO increases in the gas mixture. The Al peak with 10 vol % CO + 90 vol % H2 sample almost disappears after 2 cycles. As shown in the embedded enlarged Figure 4, a new weak reflection at round 37.4° (2θ) appeared. This peak may belong to some kind of Al oxygenates. with different CO + H2 ratios. All samples were hydrogenated and dehydrogenated in pure hydrogen twice ("activation 1 (act 1) and activation 2 (act 2)) before cycling in the gas mixture.
Pure  Figure 3 shows the hydrogen storage performance of the composite material in different ratios of CO and H2 gas mixture. After 10 cycles with 0.1 vol % CO + 99.9 vol %H2 and 1 vol % CO + 99 vol %H2, the dehydrogenation storage capacity of the composite material decreased by 17.2% and 57.3%, respectively. The sample cycled with 10 vol % CO + 90 vol % H2 gas mixture shows the most severe degradation. There was almost no hydrogen released after only 2 cycles after hydrogenation with 10 vol % CO + 90 vol % H2 gas mixture. Attempts to recharge the sample with 5 MPa of pure hydrogen failed, which means that the changes during the cycling with the gas contained 10 vol % CO seem to be irreversible. Figure 4 shows the X-ray diffraction pattern of the doped Na3AH6 material after treatment with different amounts of CO in H2. It can be seen that Na oxides were formed after 10 cycles with 0.1 vol % CO + 99.9 vol % H2 and 1 vol % CO + 99 vol % H2. In case of 10 vol % CO + 90 vol % H2 mixture, the formation of NaOH can be observed just after 2 cycles. The peak intensity ratio of Al:NaCl at around 45°(2θ) becomes smaller when the concentration of CO increases in the gas mixture. The Al peak with 10 vol % CO + 90 vol % H2 sample almost disappears after 2 cycles. As shown in the embedded enlarged Figure 4, a new weak reflection at round 37.4° (2θ) appeared. This peak may belong to some kind of Al oxygenates. with different CO + H2 ratios. All samples were hydrogenated and dehydrogenated in pure hydrogen twice ("activation 1 (act 1) and activation 2 (act 2)) before cycling in the gas mixture.
Pure  Figure 3 shows the hydrogen storage performance of the composite material in different ratios of CO and H2 gas mixture. After 10 cycles with 0.1 vol % CO + 99.9 vol %H2 and 1 vol % CO + 99 vol %H2, the dehydrogenation storage capacity of the composite material decreased by 17.2% and 57.3%, respectively. The sample cycled with 10 vol % CO + 90 vol % H2 gas mixture shows the most severe degradation. There was almost no hydrogen released after only 2 cycles after hydrogenation with 10 vol % CO + 90 vol % H2 gas mixture. Attempts to recharge the sample with 5 MPa of pure hydrogen failed, which means that the changes during the cycling with the gas contained 10 vol % CO seem to be irreversible. Figure 4 shows the X-ray diffraction pattern of the doped Na3AH6 material after treatment with different amounts of CO in H2. It can be seen that Na oxides were formed after 10 cycles with 0.1 vol % CO + 99.9 vol % H2 and 1 vol % CO + 99 vol % H2. In case of 10 vol % CO + 90 vol % H2 mixture, the formation of NaOH can be observed just after 2 cycles. The peak intensity ratio of Al:NaCl at around 45°(2θ) becomes smaller when the concentration of CO increases in the gas mixture. The Al peak with 10 vol % CO + 90 vol % H2 sample almost disappears after 2 cycles. As shown in the embedded enlarged Figure 4, a new weak reflection at round 37.4° (2θ) appeared. This peak may belong to some kind of Al oxygenates.  In order to get more information about the weak reflection at round 37.4° (2θ served in the X-ray diffraction pattern of Figure 4, we measured a carbon solid state N spectrum. Figure 5 shows the 13 C CP/MAS NMR spectrum of Ti-doped Na3AlH6 afte second hydrogenation with 10 vol % CO + 90 vol % H2 gas mixture. The most intense asymmetric line at about 51 ppm in the 13 C NMR spectrum in Figure 5 can be assign methoxy groups (O-CH3) [28]. These methoxy groups can be connected to Al-and/or atoms. The observation of O-CH3-groups also confirms the detection of Al-O-compo in the X-ray diffraction pattern in Figure 4. The high-field line at about −8 ppm stems likely from methyl groups directly bound to aluminum atoms [29]. The spectral inte between 10 and 40 ppm is partly due to a small background signal of the probe.
To gain a better understanding of the influences of CO on the molecular proc during the hydrogenation, the gas-phase FTIR spectra was measured and shown in Fi 6. During the hydrogenation, part of the CO (νC=O = 2350 cm −1 ) reacts with the com hydride and produces CH4 (νC-H = 3016 cm −1 , δC-H = 1305 cm −1 ). No other gases can b tected in the IR-spectra.  To gain a better understanding of the influences of CO on the molecular processes during the hydrogenation, the gas-phase FTIR spectra was measured and shown in Figure 6. During the hydrogenation, part of the CO (ν C=O = 2350 cm −1 ) reacts with the complex hydride and produces CH 4 (ν C-H = 3016 cm −1 , δ C-H = 1305 cm −1 ). No other gases can be detected in the IR-spectra.

The Influence of CO2 Gas on Cycling Behavior of the Complex Hydride Ti-Doped Na3AlH6
The hydrogen storage performance with different CO2 + H2 gas ratios were measured and are shown in Figure 7. The influence of 1 vol % CO2 on the storage capacity is comparable to a mixture with 1 vol % CO. After 10 cycles, the capacity degradation was 53.5% in the 1 vol % CO2 + 99 vol % H2 gas mixture and 57.3% in 1 vol % CO + 99 vol % H2. After increasing the concentration of CO2 up to 10 vol %, the capacity degradation becomes

The Influence of CO 2 Gas on Cycling Behavior of the Complex Hydride Ti-Doped Na 3 AlH 6
The hydrogen storage performance with different CO 2 + H 2 gas ratios were measured and are shown in Figure 7. The influence of 1 vol % CO 2 on the storage capacity is comparable to a mixture with 1 vol % CO. After 10 cycles, the capacity degradation was 53.5% in the 1 vol % CO 2 + 99 vol % H 2 gas mixture and 57.3% in 1 vol % CO + 99 vol % H 2 . After increasing the concentration of CO 2 up to 10 vol %, the capacity degradation becomes larger and reaches 86.8% after 6 cycles. The performance of hydride with 10 vol % CO 2 + 90 vol % H 2 is better than the one with 10 vol % CO + 90 vol % H 2 . Several new compounds can be identified by X-ray powder diffractometry after cycling with different CO 2 /H 2 gas mixtures as shown in Figure 8. The diffraction pattern of dehydrogenated hydride (Al, NaH, NaCl) which was cycled in pure hydrogen, was used as a reference. The Al, NaH, NaCl peaks can be found in all these samples. The small amounts of Na 3 AlH 6 in the composite in 10 vol % CO 2 + 90 vol % H 2 is due to the sluggish kinetics that is getting worse during cycling. The NaH phase is partly consumed during cycling to produce Na carbon oxides such as Na 2 CO 3 and Na 2 C 2 O 4 . The ratio of Al:NaH:NaCl becomes smaller that implies that the consumption of Al and NaH during cycling with 10 vol % CO 2 + 90 vol % H 2 gas mixture took place. The loss of Al and NaH leads to a reduction of the storage capacity of the material. posite in 10 vol % CO2 + 90 vol % H2 is due to the sluggish kinetics that is getting worse during cycling. The NaH phase is partly consumed during cycling to produce Na carbon oxides such as Na2CO3 and Na2C2O4. The ratio of Al:NaH:NaCl becomes smaller that implies that the consumption of Al and NaH during cycling with 10 vol % CO2 + 90 vol % H2 gas mixture took place. The loss of Al and NaH leads to a reduction of the storage capacity of the material.  All samples were hydrogenated and dehydrogenated two times in pure hydrogen (act 1 and act 2) before the cycling with the gas mixture. after 2 cycles. The peak intensity ratio of Al:NaCl at around 45°(2θ) becomes smaller when the concentration of CO increases in the gas mixture. The Al peak with 10 vol % CO + 90 vol % H2 sample almost disappears after 2 cycles. As shown in the embedded enlarged Figure 4, a new weak reflection at round 37.4° (2θ) appeared. This peak may belong to some kind of Al oxygenates. with different CO + H2 ratios. All samples were hydrogenated and dehydrogenated in pure hydrogen twice ("activation 1 (act 1) and activation 2 (act 2)) before cycling in the gas mixture.
Pure H 2 , posite in 10 vol % CO2 + 90 vol % H2 is due to the sluggish kinetics that is getting worse during cycling. The NaH phase is partly consumed during cycling to produce Na carbon oxides such as Na2CO3 and Na2C2O4. The ratio of Al:NaH:NaCl becomes smaller that implies that the consumption of Al and NaH during cycling with 10 vol % CO2 + 90 vol % H2 gas mixture took place. The loss of Al and NaH leads to a reduction of the storage capacity of the material. during cycling. The NaH phase is partly consumed during cycling to produce Na carbon oxides such as Na2CO3 and Na2C2O4. The ratio of Al:NaH:NaCl becomes smaller that implies that the consumption of Al and NaH during cycling with 10 vol % CO2 + 90 vol % H2 gas mixture took place. The loss of Al and NaH leads to a reduction of the storage capacity of the material.

Collective Influence of CO, CO2, and N2 Gas Components on the Cycling Behavior of Ti-Doped Complex Hydride Na3AlH6
As mentioned in the introduction, the auto-thermal production of syngas with air contains in addition to H2, CO, CO2, H2O also high amounts of N2 gas. The high amount of neutral N2 reduces the partial pressure of H2 in the gas mixtures and changes the hydrogenation behavior of the complex hydride. Our experiments with 62 vol % N2 + 38 vol % H2 gas mixture shows that 3.0 MPa total pressure which corresponds to only 1.1 MPa of hydrogen partial pressure is not high enough to recharge the sample at 170 °C, see Figure 9. This pressure of 1.1 MPa is below the equilibrium pressure at 170 °C, which is equal to 1.5 MPa. In order to reach partial H2 pressure of 3 MPa in a gas mixture of 1.5 vol

Collective Influence of CO, CO 2 , and N 2 Gas Components on the Cycling Behavior of Ti-Doped Complex Hydride Na 3 AlH 6
As mentioned in the introduction, the auto-thermal production of syngas with air contains in addition to H 2 , CO, CO 2 , H 2 O also high amounts of N 2 gas. The high amount of neutral N 2 reduces the partial pressure of H 2 in the gas mixtures and changes the hydrogenation behavior of the complex hydride. Our experiments with 62 vol % N 2 + 38 vol % H 2 gas mixture shows that 3.0 MPa total pressure which corresponds to only 1.1 MPa of hydrogen partial pressure is not high enough to recharge the sample at 170 • C, see Figure 9. This pressure of 1.1 MPa is below the equilibrium pressure at 170 • C, which is equal to 1.5 MPa. In order to reach partial H 2 pressure of 3 MPa in a gas mixture of 1.5 vol % CO + 10 vol % CO 2 + 27 vol % H 2 + 61.5 vol % N 2 , the overall gas pressure must be increased to 11 MPa. As shown in Figure 8, the degradation reaches 94% after 6 cycles with this gas mixture. The fast degradation process seems to be due to combined influence of the different gas impurities during cycling. Each kind of gas impurity affects the complex hydride in a different way. Figure 10 shows the X-ray diffraction pattern of the complex hydride after 6 cycles with the 1.5 vol % CO + 10 vol % CO 2 + 27 vol % H 2 + 61.5 vol % N 2 gas mixture, and for comparison, the pattern of the decomposed complex hydride after cycling in pure H 2 as a reference. Only very small diffraction peaks of Na 3 AlH 6 are observed after the cycling and decomposition. The main reflections belong to Al-metal, NaH, and NaCl from the doping process. No or very small reflections of Al-metal and NaH or Na 3 AlH 6 can be observed in the diffraction pattern after only 6 cycles. Na 2 CO 3 can be detected as newly formed compound, which can easily be explained by a reaction of NaO(H) with CO 2 . No additional Al-O-compounds are detected.  s the hydrogen storage performance of the composite material in difand H2 gas mixture. After 10 cycles with 0.1 vol % CO + 99.9 vol %H2 99 vol %H2, the dehydrogenation storage capacity of the composite by 17.2% and 57.3%, respectively. The sample cycled with 10 vol % CO mixture shows the most severe degradation. There was almost no hyter only 2 cycles after hydrogenation with 10 vol % CO + 90 vol % H2 pts to recharge the sample with 5 MPa of pure hydrogen failed, which nges during the cycling with the gas contained 10 vol % CO seem to be e 4 shows the X-ray diffraction pattern of the doped Na3AH6 material th different amounts of CO in H2. It can be seen that Na oxides were cles with 0.1 vol % CO + 99.9 vol % H2 and 1 vol % CO + 99 vol % H2. In O + 90 vol % H2 mixture, the formation of NaOH can be observed just eak intensity ratio of Al:NaCl at around 45°(2θ) becomes smaller when of CO increases in the gas mixture. The Al peak with 10 vol % CO + 90 lmost disappears after 2 cycles. As shown in the embedded enlarged eak reflection at round 37.4° (2θ) appeared. This peak may belong to ygenates.  Hydrogen 2021, 2, FOR PEER REVIEW 9 larger and reaches 86.8% after 6 cycles. The performance of hydride with 10 vol % CO2 + 90 vol % H2 is better than the one with 10 vol % CO + 90 vol % H2. Several new compounds can be identified by X-ray powder diffractometry after cycling with different CO2/H2 gas mixtures as shown in Figure 8. The diffraction pattern of dehydrogenated hydride (Al, NaH, NaCl) which was cycled in pure hydrogen, was used as a reference. The Al, NaH, NaCl peaks can be found in all these samples. The small amounts of Na3AlH6 in the composite in 10 vol % CO2 + 90 vol % H2 is due to the sluggish kinetics that is getting worse during cycling. The NaH phase is partly consumed during cycling to produce Na carbon oxides such as Na2CO3 and Na2C2O4. The ratio of Al:NaH:NaCl becomes smaller that implies that the consumption of Al and NaH during cycling with 10 vol % CO2 + 90 vol % H2 gas mixture took place. The loss of Al and NaH leads to a reduction of the storage capacity of the material.    Figure 9. Cyclic performance of the composite at 170 °C under 11 MPa hydrogenation in 1.5 v CO + 10 vol % CO2 + 2 7 vol % H2 + 61.5 vol % N2 gas mixture in comparison to cycling pure H2 , with 1 vol % CO + 99 vol % H2 , with 10 vol % CO2 + 90 vol % H2 a with 62 vol % N2 + 38 vol % H2 at 3 MPa total pressure hydrogenation.

Discussions
In this paper, we reported about the cycling performance of Ti-doped Na 3 AlH 6 + Al + activated carbon composite in pure hydrogen and studied the influence of different ratios of CO, CO 2 , N 2 gas components on the hydrogen storage properties of this complex hydride. By addition of activated carbon and aluminum to TiCl 3 -activated Na 3 AlH 6 , the cycling stability and hydrogen storage capacity could be successfully enhanced in comparison to undoped material in pure hydrogen. Both CO, CO 2 gas components react with the hydride mixture and cause a serious decline in hydrogen storage capacity to form Al-O-and/or carboxyl compounds and Na-O-and/or carbonates, and CH 4 .
Several reaction pathways exist, which can explain the conversion of CO/CO 2 to methane and water.
reduction of CO/CO 2 with Na 3 AlH 6 . -reduction of CO/CO 2 with NaH. -reduction of CO/CO 2 with H 2 under the influence of TiAl x as catalyst.
Hugelshofer et al. [11] described the reaction of LiAlH 4 with CO 2 and postulated the formation of various amorphous metal oxides, which cannot be identified by XRD. The similar reactivity of the complex aluminum hydrides LiAlH 4 and Na 3 AlH 6 could explain the formation of some amorphous metal oxides compounds with the general formula Na x Al Y O z . The structure and the amount of formed oxide-compounds strongly depends on the amount of CO or CO 2 in the gas mixture, while CH 4 and H 2 O are produced. Water seems to be the main reason for the production of metal oxide compounds and subsequently, reduced reversibility of the storage material.
The reduction of CO 2 to methane in the presence of mechanochemically activated alkali metal hydrides were discovered by Zhao et al. [23]. They observed elemental carbon, hydrogen, alkali metal oxides, and carbonates as final products from the reaction of the oxides with CO 2 . Similar reaction pathways can be expected in our case with the exception that in the presence of TiAl x -catalyst hydrogenated gaseous compounds (CH 4 ) can be observed.
The in situ formed Al-Ti active species [30], which are acting as a catalyst for the hydrogenation of NaH/Al to Na 3 AlH 6 , can also act as catalyst in a hydrogen atmosphere for the reduction of CO to produce CH 4 [11].
In comparison to these three examples, our system is more complicated, since all three different reaction pathways can take place at the same time. During these reduction processes, stoichiometric amounts of H 2 O are produced which consequently react with hydride species to produce Na-and/or Al-oxide compounds. In a following process, these oxide compounds can react with CO 2 producing carbonates and in case of CO producing formic acid compounds. A loss of catalytic activity of Al-Ti species and the oxidation of Naand Al-hydride species lower the reversibility of the composite system and hence degrade the hydrogen storage capacity.

Conclusions
Ti-doped Na 3 AlH 6 is a medium temperature hydrogen storage material with a theoretical hydrogen storage capacity of 3 wt % H 2 and an impressive stable capacity over several hundreds of de-and re-hydrogenation cycles in pure hydrogen. Nowadays, most of the worldwide used hydrogen is produced from natural gas. This means that significant amounts of CO and CO 2 could be present in the produced hydrogen gas. Therefore, we have tested the reactivity of CO and CO 2 against Ti-doped N 3 AlH 6 . Both gases, CO and CO 2 , show a high affinity to the complex hydrides and just after few hydrogenation/dehydrogenation cycles, cause irreversible damage. The complex hydride could not be regenerated with pure hydrogen under current experimental conditions. The N 2 gas impurity does not react with the hydride, but it greatly reduces the partial pressure of H 2 and therefore cause difficulties for the hydrogenation reaction. The experimental data show that syngas cannot be used for the recharging of these complex hydrides, therefore prior to the hydrogenation process, a thorough purification of hydrogen from CO, CO 2 , and of N 2 is necessary. This purification process can be realized using well-known separation methods such as PSA (pressure swing adsorption), membrane techniques (Pd-based membranes, ceramic membranes, electrochemical membranes), and cryogenic separation. On the other hand, due to the high reactivity of Ti-doped Na 3 AlH 6 towards CO and CO 2 , the material can be used for the absorption of small amounts of these gases and the production of high purity hydrogen for PEM-fuel cell applications.