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A. Rivera Defects in Materials, IRI, TUDelft

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Presentation on theme: "A. Rivera Defects in Materials, IRI, TUDelft"— Presentation transcript:

1 Metal hydride formation and hydrogen storage in Al-Li alloys IRI Symposium May 22, 2003
A. Rivera Defects in Materials, IRI, TUDelft Work supported by the Delft Institute for Sustainable Energy (DISE) Contributors at DM: A. van Veen (head), F. Labohm, J. de Roode, W.J. Legerstee, K.T. Westerduin, S.W.H. Eijt, H. Schut. External contributors (Materials Science Faculty, TUDelft): R. Delhez, N. van der Pers

2 World energy consumption
To reduce oil dependency  Hydrogen

3 How to store hydrogen? A 1000 kg car consumes
5-6 kg fuel/100 km The same car would consume 2 kg H2/100 km in combustion mode or 1 kg H2 /100 km in fuel cell mode However, at room temperature and atmospheric pressure 1 kg H2 occupies 11 m3 Storage: Pressurised vessels Liquified H2 Sorbed at surface or bulk materials

4 Contents Material requirements Non-transition light metal hydrides
Examples Non-transition light metal hydrides Experimental developments Al-Li materials Conclusions and further work

5 Material requirements
Storage capacity > 5 wt. % Fast reaction kinetics H2 release: 100 kPa at T < 200 ºC Reversibility in the range 0 – 200 ºC Resistance to degradation Cost Safety

6 Sources of inefficiencies
Hysteresis between absorption and desorption Hydride stability Limited kinetics Poor heat conduction Small diffusion constant Surface reactions Necessity for initial hydriding activation Sensitivity to air, impurities or other gases Volume expansion Decrepitation into fine powder

7 Storage and release Hydrogen in solution: α-phase
Hydrogen in hydride: β-phase Formation of hydride: α & β M + ½xH2  MHx + ΔQ Isotherm flat More plateaux can appear Desorption isotherm is lower due to stress This is undesired for hydrogen storage Formation enthalpy can be obtained

8 Kinetics E.g. MgH2 at 600 K Slow diffusion 1 μm / s

9 Hydrogen storage materials

10 Key properties

11 Non-transition light metal hydrides
LiAlH4, NaAlH4 (in water  irreversible full H2 release) High capacities (10 and 5 wt.%, respectively) No reversible due to decomposition 3 LiAlH4  Li3AlH6 + 2 Al + 3 H [ oC] Li3AlH6 + 2 Al  3 LiH + 3 Al H2 [ oC] 3 LiH + 3 Al  3 AlLi H2 [ oC] Slow kinetics Catalysts, as Fe, Ti and Zr Make some steps reversible Improve the kinetics

12 Our approach Objective: to develop nanostructured light weight alloys for hydrogen storage Choice: Al-Li compounds Preparation Sputtering of Al-Li alloy or LiAlH4 Laser ablation of Al-Li alloy or LiAlH4 Cathodic charge, ion implantation gas or plasma exposure + annealing Characterisation Volumetric analyses, Permeation, TDS, XRD, NDP, PBA Occasionally ERDA, SEM, TEM

13 Gas analysis techniques
Hydra Hydrogen absorption and desorption experiments Desorption detection limits H2 molecules Dynamic measurements give direct information on kinetics Appropriate for thin films Permeation of solved molecules or electrochemically introduced atoms in situ after sputtering will become available soon Sensitive thermal desorption spectrometry Detection limit as low as 1011 H2 molecules Significantly lower for D2

14 Hydra

15 Hydra Expansion volume M1 10-2-10 Pa M2 10-105 Pa M0 0.1-6 MPa
Mix volume Gas inlet To pumps Pd filter Mass analyser Cell ( K)

16 Hydra (static) M1 1015-1017 H2 M2 1017-1022 H2 Expansion volume M0
0.1-6 MPa Mix volume Gas inlet To pumps Pd filter Mass analyser Cell ( K)

17 Hydra (dynamic) Expansion volume M1 M2 M0 0.1-6 MPa Mix volume
Gas inlet To pumps Pd filter Mass analyser H2/s H2 Cell ( K)

18 Hydra software

19 Desorption of LiAlH4 0.4 mg LiAlH4, 0.1 K/s Total H2: 1.5x1022 g-1
Total gas: 3.9x1022 g-1 0: Hydroxide 1: LiAlH4 2: Li3AlH6 3: LiH

20 Sputter deposited Al-Li: SEM
SEM evidences the formation of columnar structures in the nm range, size increases with distance from substrate ~1 µm sputter deposited Pd layer Pd ~1 µm sputter deposited Al-Li at room temperature, the layer contains 5at.%Li (NDP) Al Li

21 Sputter deposited Al-Li: Hydrogen
Dynamic measurements: High sensitivity Easy background estimation Peaks indicate kinetics processes Around 0.5 at.H% Recharging results in low T peak of 0.3 at.H%

22 Conclusions and further work
Effort to fulfil material requirements Successful H2 detection techniques Successful creation of samples by Sputtering Laser ablation Currently: High Li content samples from LiAlH4 targets Study of samples with high porosity Fundamental study of Li nanocrystals in c-Al

23 Further information Contact A. Rivera: Rivera@iri.tudelft.nl
A. van Veen:


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