ISSN : 0970 - 020X, ONLINE ISSN : 2231-5039
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Improved Hydrogen De/absorption Kinetics of Magnesium (Mg) via Addition of Catalyst Y2O3

Madhu Yadav1,2, Deepak Kumar Yadav1,3, Satya Narayan Dolia1,2 and Chhagan Lal1,2*

1Department of Physics, University of Rajasthan Jaipur, JLN Marg, Jaipur-302004 Rajasthan, India

2Centre for Non-Conventional Energy Resources, University of Rajasthan Jaipur, JLN Marg Jaipur, Rajasthan, India

3Department of Physics, Government GNA PG College, Bhatapara, Chhattisgarh, India.

Corresponding Author E-mail: clsaini52@uniraj.ac.in

DOI : http://dx.doi.org/10.13005/ojc/400530

Article Publishing History
Article Received on : 06 Jul 2024
Article Accepted on : 13 Sep 2024
Article Published : 07 Nov 2024
Article Metrics
Article Review Details
Reviewed by: Dr. Hemendra Bhandari
Second Review by: Dr. BK Sharma
Final Approval by: Dr. Charanjit Kaur
ABSTRACT:

MgH2 is attracting significant attention in the field of materials for storing hydrogen due to its mass-related hydrogen retention capacity, excellent reversibility, and cost-effectiveness making it a feasible option for fulfilling energy-sustaining needs. Despite its slow desorption and absorption limitation, the kinetics of MgH2 can be improved by the ball milling technique. In this work to synthesis nanocomposite, various wt% concentrations of Y2O3 (X = 5, 10) are introduced to MgH2. Thermodynamics of all prepared samples were measured by DSC, TGA, and PCT/PCI setups. The PCT investigation reveals that the Mg/MgH2-5 wt% Y2O3 nanocomposites store 4.7 wt% H2, where 100 h milled Mg/MgH2 store 5.2 wt% hydrogen. Adding Y2O3 with MgH2 reduces the dehydriding activation energy and onset temperature of Mg/MgH2.

KEYWORDS:

Activation energy; DSC; Hydrogen storage; MgH; PCT; TGA; Y2O3

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Yadav M, Yadav D. K, Dolia S. N, Lal C. Improved Hydrogen De/absorption Kinetics of Magnesium (Mg) via Addition of Catalyst Y2O3. Orient J Chem 2024;40(5).


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Yadav M, Yadav D. K, Dolia S. N, Lal C. Improved Hydrogen De/absorption Kinetics of Magnesium (Mg) via Addition of Catalyst Y2O3. Orient J Chem 2024;40(5). Available from: https://bit.ly/40Dv8Lz


Introduction

Hydrogen gets attenuation in the whole world due to its dense energy content of 142 MJ/kg, compact, ecofriendly nature, and can easily be produced from water 1. The main problem associates with its storage, which makes it not suitable for automobile as well as industrial applications. Its liquid and gas phase storage required cryogenic and high-pressure storage tanks. Both methods have a very high explosion risk and large energy lose due to boiling off 2. The main challenge of hydrogen storage is closely linked to the need for the development of reliable and efficient hydrogen compression methods. Solid-state hydrogen storage provides a much easier, safer, effective, and economical way to store hydrogen 3. Throughout recent decades ammonia borane 4,5 lithium compounds6,7, lightweight metal hydrides (for example MgH2, NaAlH4, LiAlH4, LiH, LaNi5H5, TiFeH2, PdH2) have been considered for their role as solid state materials used for storing hydrogen8.

In all above MgH2 hasshown great potential as a solid-state hydrogen storage media because of its large hydrogen storage capacity (theoretical ~7.6 wt%), compact, most abounded element, low cost, and high reversibility9,10. Due to high thermal stability and poor ab/desorption kinetics, it is not widely used in both automotive and industrial applications 11. In later times, several attempts have been made to enhance sorption kinetics and heat dynamics of Mg/MgH2, such as ball milling, catalysts, and alloys as dopants. For example, materials such as metals 12-15, alloys 16-21, oxide 11,22-24, and halides 25-28, have been doped with Mg/MgH2.  Extensive research efforts have been dedicated to transitional metal oxides serving as efficient catalysts to store hydrogen in MgH2. Oelerich et al. reported that the catalysing impact of TiO2, V2O5, Cr2O3, Mn2O3, Fe3O4, and CuO on the hydrogenation properties of Mg are comparable29. Fe3O4 demonstrated superior catalytic activity in the dehydrogenation reaction, which was succeeded by V2O5, Mn2O3, Cr2O3, and TiO2. Remarkably, Barkhordarian et al. recorded the exceptional catalytic activity of Nb2O5 and the rapid hydrogen sorption kinetics of 0.2 mol.% Nb2O5-doped Mg with nanosized crystal lattice30.

Xueping et al.31 examine the catalytic role of Y2O3 in promoting the dehydrogenation of NaAlH4.  It was observed that hydrogen storage capacity rises with Y2O3 concentration. Where desorption rate firstly increases and then decreases with Y2O3 concentration. Furthermore, Liu et al.32 examined the hydrogenation properties of MgH2-Y2O3/NiO hybrid. Their study revealed that the dehydrogenation temperature of MgH2 reduces with an enhancement of Y2O3/NiO hybrid. They found that Y2O3 plays a superior role in enhancing hydrogen storage capacity, improving cycle life kinetics, and sorption kinetics of MgH2.  Surface reactivity of Y2O3 powder toward hydrogen has been studied by Kogler et al. [33] and they found that due to the specific hydrophilicity of the oxide, sorption of water eventually takes place. The evidence supporting this surface-restricted mechanism is further strengthened by the absence of bulk structure and even at the highest reduction temperature (1173 K) morphological changes were observed upon reduction. To the authors’ knowledge, the catalytic effect of Y2O3 on MgH2 has not been widely studied so far. In the present study, we conducted a comprehensive study of catalytic role of Y2O3 on the hydrogen storage properties and sorption kinetics of Mg/MgH2.

Experimental Preparation

Nano-Composite Preparation

Mg and Y2O3 powder of purity 99.98% were used during the synthesis procedure. Mg-x wt% Y2O3 (x = 0, 5, 10) powder was loaded into a ball milling jar and then sealed with an O ring. Whole process is carried into a glove box filled with pure argon gas. Then sealed jar was transferred to ball milling machine (Model: Retsch PM 100 type).  Ball-Milling process was performed for 100 h at a speed of 150 rpm. To synthesis Mg-x wt %Y2O3 nanocomposites, ball to charge ratio of roughly 5:1 was used. Ball-Milling procedure was performed at room temperature under atmospheric condition.

Structural and Morphological Characterization

Catalytic role on crystal structure and crystalline dimension were examined by using cu-kα radiation (λ=1.54 Å). XRD data was collected across the 20-80̊ range. The surface morphology of the synthesized samples was measured by Scanning electron microscope (SEM, Model Nova-Nano FE-SEM 450) at 15 kV. Chemical elemental composition was recorded by an EDX detector, which is inbuilt in SEM instrument.

Thermodynamics of Dehydrogenation

Thermodynamics of the hydrogen-depleting reaction of Mg and Mg-5 wt% Y2O3 nano-composites were measured via a Differential Scanning Calorimeter (DSC Model No. 7020). All DSC measurements were carried out at diverse heating rates of 5, 10, 15, and 20 0C/min in scale of thermal conditions 300C – 5500C. Roughly 5-6 mg sample was used for each DSC measurement. A constant nitrogen flow of 60 ml/min was maintained during the whole measurement.

Catalytic effect on dehydrogenation properties was carried out with Thermal Gravimetric Analyzer (TGA) measurement (STA Model Hitachi TGA-7300). Other Conditions are the same as of DSC measurement.

Pressure-Composition-Temperature (PCT) analysis

A sievert-type Homemade PCI/PCT setup was employed to measure the hydrogen storage attributes of MgH2 – x wt% (x = 0, 5, 10). Roughly 1 gm sample was used for each PCT measurement. Before every measurement, a leakage test was performed for 24 h at 350 0C. After that activation process was executed at 3500C and 2 Mpa H2 pressure for 6 h followed by 6 cycles of activation. After each sample loading the same process was repeated. Then PCT   measurement was taken. Notably, Van’t Hoff equation was used to measure the enthalpy and entropy of re-hydrogenation reaction. Generally, enthalpy and entropy of most metal hydride are negative, except in certain instances.

Result and discussion

Figure 1 represents the XRD spectrum of Mg/MgH2 and Mg- 5 wt% Y2O3 nanocomposites. XRD investigation reveals that the phase identity of Mg/MgH2 and Mg- 5 wt% Y2O3 is maintained during ball milling. XRD spectrum indicates the existence of diverse phases within the nanocomposites, which possibly occur during ball-milling. The presence of these phases provides extra catalytic effects on the hydrogenation properties of Mg- 5 wt% Y2O3 nanocomposites. XRD data revealed diminished peak intensities and stretching of the Full width at half maxima (FWHM), value MgH2 is 0.17, and for Mg+5 wt%Mg+Y2O3 is 0.2 signifying the presence of physical stress accumulation and reduction in particle dimension during ball milling. Ball-milling creates new active surfaces, resulting in enhanced hydrogenation properties of the nanocomposite. Analysing, the X-ray diffraction (XRD) spectra focus on the full width at half maxima (FWHM) and peak intensity, which are essential parameters for assessing crystallinity and grain size. A narrower FWHM signifies larger crystallite sizes and improved crystallinity, as broader peaks usually indicate smaller crystallites or greater structural disorder. Higher peak intensity reflects better crystallinity and larger grain sizes, indicating well-aligned and abundant crystalline planes. The lattice parameters for MgH2 and Mg+5 wt%Mg+Y2O3 are as for MgH2 a=b=4.49 Å &C=2.0 Å and for Mg+5 wt%Mg+Y2O3 are a = b = c= 10.606 Å as verified from JCPDS file no.- 01-079-6694 and JCPDS file no.- 01-089-5592

These values align well with previously reported data. The ratio c/2a lattice parameter for MgH2 is 0.22 and for Mg+5 wt%Mg+Y2O3 is 0.5.

The crystallite size D was determined using Scherrer’s formula:

Where D is the average crystallite size, k is the shape factor, λ is the wavelength of Cu-Kα X-rays, β is the full width at half maxima (FWHM), θ is the Bragg angle. The value of D for MgH2 is 79 nm and for Mg+5 wt%Mg+Y2O3 is 71.5 nm.

By calculating, the dimensions of dislocation lines per unit volume, the dislocation density(𝞭) is calculated using Williamson and Smallman’s formula is

The value for MgH2 is 0.00016 nm-2 and for Mg+5 wt%Mg+Y2O3 is 0.00019 nm-2.

Unit Cell Volume (V)

The unit cell volume V for MgH2 was calculated using the relation V = a2 c and Mg+5 wt%Mg+Y2O3 is calculated by V=a3, where a and c are the lattice parameters values are 40.3202 Å3 and 1193.03 Å3.

Microstrain (𝞊)

Stress is an important factor influencing the structural features of crystalline lattices when there is a geometric mismatch between their boundaries. The relationship illustrated below can be utilized to compute microstrain (𝞊).

The value for MgH2 is 0.043855nm and for Mg+5 wt%Mg+Y2O3 is 0.04845 nm.

Then, it is summarised as MgH2 has a slightly larger crystallite size, lower dislocation density, and larger unit cell volume than MgH2– 5 wt% Y2O3. A slight peak shift for (110) was measured for MgH2 with the addition of Y2O3. And two peaks of Y2O3 for the plane (222) and (431) was noted.

Figure 1: XRD spectrum of 100 h milled MgH2 and Mg-5 wt% Y2O3 nanocomposites.

Click here to View Figure

SEM (Scanning electron Microscopy)

Surface morphology of all synthesis samples is shown in Figure 2.  Figure 2(a) represents the SEM micrograph of 100 h milled MgH2 and 2(b) represents MgH2– 5 wt%Y2O3 nanocomposites. The average crystalline size for MgH2 was recorded at ~ 79 nm and for MgH2– 5 wt% Y2O3 nanocomposites was in the range of ~71.5 nm. SEM imaging indicates a decrease in the particle size after ball milling, generating a refreshed surface area conducive to hydrogen absorption and release within the composites. Examination of SEM images shows that ball milling yields a nonuniform particle size distribution. Analysis of SEM images emphasize the dense aggregation of small particles in the vicinity of large particles and some clusters are present in the prepared samples. This property plays an important role in improving the kinetics of hydrogenation. Figure 2(c) and 2(d) represents the EDX mapping of 100 h milled MgH2 and MgH2– 5 wt%Y2O3 nanocomposites. The EDX analysis provides information on both elemental identification and quantitative composition. Hight of the peaks represents the chemical quantitive information of the nanocomposites.

Figure 2: FE-SEM for 100h milled (a) MgH2 (b) for Mg-5 wt%Y2O3 nanocomposites, EDX graphing for 100h milled (c) MgH2 (d) for Mg-5 wt%Y2O3 nanocomposites.

Click here to View Figure

Figure 3 represent particle size distribution of MgH2 and MgH2– 5 wt% Y2O3 nanocomposites. For each plot about 200 data points have been recorded. The average particle size found for MgH2 is 81.963 ± 32.045 nm and for MgH2– 5 wt% Y2O3 is 81.021 ± 21.273 nm.

Figure 3: particle size distribution plots of 100 h milled (a) MgH2 and (b) MgH2– 5 wt% Y2O3

Click here to View Figure

Pressure-Composition-Temperature (PCT)

Pressure-composition-temperature (PCT) is carried out at diverse temperatures for 100 h milled Mg and Mg-5 wt%Y2O3. The maximum hydrogen absorption achieved for Mg is 5.2 wt% at 320 ̊ C as shown in Fig.4(a). The results indicate that as temperature increases, the plateau pressure shifts towards the higher end, correlating with a decrease in absorption capacity, and notably the plateau pressure does not persist unchanged with the temperature.

Fig4(b) represents the maximum absorption capacity achieved for Mg-5 wt% Y2O3 nanocomposites is 4.7 wt% at 280 ̊ C. The PCT plot recorded in the temperature range 280-340 ̊ C. PCT investigation indicate that with the increase of temperature absorption capacity reduces.  But the plateau pressure didn’t persist unchanged with the temperature.

Fig.4 (c) shows comparative study at temperature 280 ̊ C at different weight percentage. So, it shows that Mg- 5 wt%Y2O3 have higher hydrogen absorption capacity as compare to different weight percentage. From the PCT analysis it is clear that as we increase Y2O3 concentration absorption capacity of Mg/MgH2 reduces.

Figure 4: shows PCT profile of (a) 100 h milled Mg/MgH2, (b)Mg-5wt%Y2O3 nanocomposites, and (c) Comparative study at different wt%.

Click here to View  Figure

Enthalpy and entropy for hydrogenation reaction were determined applying the Van’t Hoff equation to PCT measurements and analyzing by Van’t Hoff plots. Fig. 5 represents the Van’t Hoff plot of 100 h milled (a) Mg/MgH2 (b) Mg- 5 wt% Y2O3, and the calculated enthalpy and entropy for MgH2 is 52.502 kJ/mol and 104.25 J/mol-k, for Mg-5 wt% Y2O3 is 76.995 kJ/mol and 149.236 J/mol-K, and for Mg-10 wt%Y2O3 is 55.156 kJ/mol and 108.976 J/mol-K respectively. So, from the results we conclude that the lowest enthalpy was obtained for Mg-5 wt% Y2O3 nanocomposites.  Entropy calculations are conducted to understand the transition from gaseous molecular hydrogen to dissolved atomic hydrogen. Enthalpy governs the heat released or absorbed during hydrogen uptake or release reaction.

Figure 5: Van’t Hoff Plot of 100 h milled (a) Mg/MgH2, (b) Mg- 5 wt%Y2O3 nanocomposites,

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Thermodynamics and Kinetics of the dehydrogenation process

TGA and DSC analysis of MgH2 and Mg-5 wt% Y2O3 nanocomposites at different heating rates are shown in fig. 6 (a, b). Thermogravimetric analysis (TGA) of MgH2 shows that the maximum weight loss is observed at 15 ̊ C/min and loss is reached up to 3.1 % at 460 ̊ C and Mg-5 wt% Y2O3 shows that the maximum weight loss is 1.6% up to 477 ̊ C at the heating scale of 20 ̊ C/min

Thermodynamics analysis of Mg and Mg-5 wt%Y2O3 nanocomposites were examined through Differential Scanning Calorimetry (DSC) as shown in fig 6 (c, d). The decomposition of metal hydride often leads to an exothermic reaction. The exothermic reaction represents the hydrogen is liberated through the decomposition of MgH2 at 449 0C at the heating scale of 15 0C. As, the heating rate decreases the peak shifted towards lower side. Heat flow profile obtained by the Mg-5 wt%Y2O3 show decomposition at 447 0C at the heating scale of 20 0C.  With decreasing heating rate, the peak tends to move towards lower end. DSC and TGA analysis indicate that on set temperature of Mg/MgH2 shifted toward lower end with increasing Y2O3 concentration.

Figure 6: (a, b) shows TGA for 100 h milled MgH2 and Mg-5 wt% Y2O3 nanocomposites (c) shows comparative study at the rate of 10 ̊ C/min

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Figure 6: (c, d) shows DSC for 100 h milled MgH2 and Mg-5 wt% Y2O3 nanocomposites.

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The activation energy (Ea) for dehydrogenation reaction of the synthesized nanocomposites has been derived. By performing TGA measurements at varying heating rates under the correspondent experimental setup, the activation energy can be determined using Kissinger equation

Where k= β/ Tp2 , β represents the heating rate, TP represents the peak temperature, R represents the gas constant and Ea represents the activation energy. When plotting a graph of ln(k) contrary to 1/T, slope corresponds to -Ea/R. The activation energy value is accumulated from the slope.  Fig.7 shows activation energy for (a) MgH2 and (b) Mg-5 wt% Y2O3. The calculated activation energy for MgH2 is 218.57 kJ/mol and for Mg-5 wt% Y2O3 is 203.03 kJ/mol. The activation energy acts as threshold that must be surpassed to initiate the liberation of hydrogen and its nanocomposites. Figure 7 illustrates decrease of activation energy with catalyst concentration. The behavior affected by factors such as catalytic impact, particle dimension, surface area, and catalytic properties affects the desorption rates. Sample with higher activation energy are indicative of heightened thermal stability.

Figure 7: Kissinger plot of 100 h milled (a) MgH2, and (b) for Mg-5 wt% Y2O3 nanocomposites.

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Conclusion

The study focused on examination how catalysts Y2O3 influence structural, morphological, and ab/desorption kinetics of Mg/MgH2 by utilizing XRD, FE-SEM with EDX and simultaneous TGA-DSC techniques. XRD and SEM investigation shows that ball-milling provides non-uniform mixing and creates new active fresh surface, which leads to increase hydrogen ab/desorption kinetics as well as capacity of Mg/MgH2. PCT analysis revels that the highest absorption achieved for Mg/MgH2 is at 5.2 wt% at 320 ̊ C and for Mg-5 wt% Y2O3 nanocomposites is 4.04 wt% at 280 0C. From PCT analysis it is clear that that the hydrogen absorption capacity of Mg/MgH2 reduces with increasing Y2O3 concentration. The DSC analysis indicates that that the decomposition of metal hydride often leads to an exothermic reaction. Through the decomposition of MgH2 hydrogen is liberated at 449 0C and Mg-5 wt%Y2O3 shows decomposition at 447 0C. DSC analysis revels that the onset hydrogenation temperature of Mg/MgH2 shifted towards lower end with addition of Y2O3 catalyst. TGA analysis shows that activation energy for MgH2 is 218.57 kJ/mol and for Mg-5 wt% Y2O3 is 203.03 kJ/mol. So, by the addition of catalysts activation energy decreases.

Acknowledgment

The authors would like to acknowledge the Department of Physics, University of Rajasthan, Jaipur for their assistance with TGA and DSC facilities respectively. Also thankful to MNIT Jaipur for Characterization XRD and FE-SEM with EDX facility.

Conflict of Interest

The authors have no relevant financial or non-financial interest to disclose.

Funding Sources

There is no funding Sources

Ethical Approval

All the ethical Standard maintain during the research. On the behalf of all authors Corresponding Authors (Dr. Chhagan Lal) demonstrate that we have followed the accepted ethical standard of genuine research study in the research article.

Data Availability Statement

On the behalf all authors Dr. Chhagan Lal declare that all authors have freely (Voluntarily) entered the research with full information and that consent has been taken from all authors before entering the research.

Authors Contribution

Madhu Yadav, Prof. S.N. Dolia involved in formal Investigation, Methodology and writing, Deepak Kumar Yadav helped in formal analysis of measurements and the entire work was done in the supervision of Dr. Chhagan Lal. 

Future Directions

Future directions may involve further optimization of nanocomposite synthesis parameters, exploration of alternative additives, and investigation of the performance of MgH2 nanocomposites under realistic operating condition. Additionally, studies focusing on scale-up and commercial viability of the developed materials warranted to facilitate their practical application in hydrogen storage system.

References

  1. Chawla, K; Yadav, DK; Sharda, P; Lal, N; Sharma, S; Lal, C. International Journal of Hydrogen Energy 2020; 45(44):23971-23976.
    CrossRef
  2. Chawla, K; Yadav, DK; Bajpai, A; Kumar, S; Lal, C. Environmental Science and Pollution Research 2021; 28:3872-3879.
    CrossRef
  3. Sakintuna,B; Lamari-Darkrim,F; Hirscher,M. International journal of hydrogen energy 2007; 32(9):1121-1140.
    CrossRef
  4. Hu, MG; Geanangel, RA; Wendlandt, WW. Acta, 1997,23,249-255.
    CrossRef
  5. Stephens, FH; Pons, V; Baker, RT; Dalton Trans.2007, doi:10.1039/B7030532C.
  6. Chen, P; Xiong, Z; Luo, J; Lin, J;Tan ,KL. Nature,2002,420: 302–304.
    CrossRef
  7. Chen, P; Xiong, Z; Luo, J; Lin, J; Tan, KL.J. Phys. Chem. B,2003,107,10967–10970.
    CrossRef
  8. Jain, I; Jain, P; Jain, A. J Alloy Compd 2010,503(2),303-39.
    CrossRef
  9. Schlapbach, L; Zuttel, A. Nature,2001, 414:353-358.
    CrossRef
  10. Jain, IP; Lal, C; Jain, A. Int. J. Hydrogen Energy, 2010,35,5133-5144
    CrossRef
  11. Yadav, DK; Chawla, K; Jain, IP; Lal, C. Environmental Science and Pollution Research 2021,28,3866-3871.
    CrossRef
  12. Ouyang, LZ; Cao, ZJ; Wang, H; Liu, JW; Sun, DL; Zhang, QA; Zhu, M. Int. J. Hydrogen Energy 2013,38,8881-8887.
    CrossRef
  13. Hanad, N.; Ichikawa, T.; Fujii, H., J. Phys. Chem. B,2005,109,7188-7194.
    CrossRef
  14. Dai, J.H.; Song, Y.; Yang, R. J. Phys. Chem. C,2010,114,11328-11334.
    CrossRef
  15. Mahmoudi, N; Kaflou A.; A. Simchi A. J. Power Sources,2011, 196,4604-4608.
    CrossRef
  16. Zhong, H.C.; Wang, H.; Ouyang, L.Z. Int. J. Hydrogen Energy,2014,39,3320-3326.
    CrossRef
  17. Yu, X.B.; Yang, Z.X.; Liu, H.K.; Grant, D.M.; Walker, G.S. Int. J. Hydrogen Energy,2010,35,6338-6344.
    CrossRef
  18. Janot, R.; Darok, X.; Rougier, A., Aymard, L., Nazri, G.A.; Tarascon, J.M., J. Alloys Compd.,2005,404-406 ,293-296.
    CrossRef
  19. Chawla, K., Sharma, G.; Bajpai, A.; Roy, P.K.; Jain, I.P.; Lal C. International Journal of Hydrogen Energy,2024, 57,1253-1262.
    CrossRef
  20. Chawla, K., Yadav, D.K., Bajpai, A., Jain, I.P. and Lal, C. Sustainable Energy Technologies and Assessments,2022,51,101981.
    CrossRef
  21. Friedrichs, O.; Aguey -Zinsou F.; Ares Fernandez J.R.; Sanchez-Lopez J.C.; Justo A.; Klassen T.; Bormann R.; Fernandez A. Acta Materialia,2006,54 ,105-110.
    CrossRef
  22. Révész, A.; Fátay, D.; Zander, D.; Spassov, T., Journal of Metastable & Nanocrystalline Materials,2015,24-25,447-450.
    CrossRef
  23. Cabo, M.; Garroni, S.; Pellicer, E.; Milanese, C.; Giella, A.; Marini, A.; Rossinyol, E.; Surinach, S.; Baro, M.D., Int. J. Hydrogen Energy;2011;36; 5400-5410.
    CrossRef
  24. Yadav,D.K.;Chawla,K.;Lal,N.;Choudhary,B.L.;Lal,C. MaterialsToday:Proceedings, 2021;46;2326-2329.
    CrossRef
  25. Yavari, A.R.; Le Moulec, A.; Castro F.R.D.; Deledda, S.; Friedrichs, O.; Botta, W.J.; Vaughan, G.; Klassen, T.; Fernandez, A.; Kvick, A. Scripta Materialia,2005,52,719-724.
    CrossRef
  26. Jin, S.A.; Shim, J.H.; Cho, Y.W.; Yi, K.W.; J. Power Sources,2007, 172, 859-862.
    CrossRef
  27. S. Kumar, A. Jain, S. Yamaguchi, H. Miyaoka, T. Ichikawa, A. Mukherjee, G.K. Dey, Y. Kojima, Int. J. Hydrogen Energy,2017,42,6152-6159.
    CrossRef
  28. Ismail, M.; Energy,2015, 79,177-182.
    CrossRef
  29. Oelerich, W.; Klassen, T.; Bormann, R. J Alloys Compd, 2001,315,37-42.
    CrossRef
  30. Barkhordarian, G.; Klassen, T.; Bormann, R. Scr Mater,2003,49,213-217.
    CrossRef
  31. Xueping, Z., Guo, X., Shenglin, L., Xin, F. and Jiaojiao, Z., 2013. Effect of CeO2 and Y2O3 as Catalysts on Hydrogen Desorption Properties of NaAlH4. Rare Metal Materials and Engineering42(7),1321-1324.
    CrossRef
  32. Liu, Y.; Wang, S.; Li, Z.; Gao, M.; Liu, Y.; Sun, W.; Pan, H.Processes, 2021, 9(5), 892.
    CrossRef
  33. Kogler, M.; Köck, E.M.; Bielz, T.; Pfaller, K.; Klötzer, B.; Schmidmair, D.; Perfler L.; Penner S.; The Journal of Physical Chemistry C, 2014,118(16), 8435-8444.
    CrossRef


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