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Third Day Poster Session, 17 June 2010 - NanoTR-VI

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<strong>Poster</strong> <strong>Session</strong>, Thursday, <strong>June</strong> <strong>17</strong><br />

Theme F686 - N1123<br />

Hydrogen Storage and Release Mechanisms in MOF-5<br />

M. MANI-BISWAS 1 , T. CAGIN 1,2<br />

1 Materials Science and Engineering, Texas A&M University, College Station, TX 77843, USA<br />

2 Department of Chemical Engineering, Texas A&M University, Texas, TX 77843-3122, USA<br />

Abstract- Metal organic framework MOF-5 is a hybrid porous crystalline material. It has high porosity and large<br />

surface area and hence potential application in gas storage, catalysis, drug delivery, etc. For applications as a gas<br />

storage material, it is important to find out a suitable gas delivery mechanism. Here we propose such a<br />

mechanism by taking advantage of near shear instability of MOF-5. Using molecular simulation we show that at<br />

high pressure MOF-5 gets deformed to 55% of its original volume. We also show that during this deformation<br />

process; MOF-5 passes through certain stages from where, by decreasing the pressure, 100% reversibility can be<br />

achieved. Based on this behavior, a purely mechanical process is proposed for gas (H 2 ) storage and release.<br />

Keywords: Hydrogen storage, Metal organic frameworks, Molecular Dynamics, sorption simulation, mechanical instability.<br />

Metal organic frameworks (MOF) are hybrid<br />

porous crystalline materials. They have the highest<br />

pore size, low density and large surface area of any<br />

crystalline material 1-4 . In general, MOFs are made<br />

up of metal oxide clusters positioned at the vertices<br />

and connected by organic linkers. For example, the<br />

simplest structure MOF-5 (IRMOF-1) is made up<br />

of Zn 4 O clusters are positioned at the corners of the<br />

cubic cell and connected by benzene dicarboxylate<br />

(BDC) linkers. The framework molecules take up<br />

only a small fraction of the available space in the<br />

crystal and about 80 % of the volume is free to<br />

accommodate any guest molecule 1 . MOFs can be<br />

easily prepared in the laboratory and have good<br />

thermal stability (till 300-400 0 C) 3 . All these<br />

properties make MOFs suitable for applications<br />

such as gas storage/separation, catalysis, molecular<br />

recognition, etc. 5, 6 MOFs have potential to adsorb<br />

gases like H 2 , CH 4 , CO 2 , N 2 , Ar, etc. and the<br />

adsorption capacity may be improved by changing<br />

the functionality of the linker and thus increasing<br />

MOF-guest interaction energy, incorporating open<br />

metal sites, catenation of framework, etc 4 . MOF<br />

filled containers have demonstrated enhanced<br />

storage capacity (44% more hydrogen, 4 times<br />

more Xenon and 3 times more propane) compared<br />

to empty containers 5 , further strengthening the<br />

potential of MOFs as gas storage medium.<br />

Studies on the mechanical property have revealed<br />

that MOF-5 is a soft material and it is nearly<br />

unstable 7-8 , implying that the crystal is flexible<br />

enough to transform to a new structure in the<br />

presence of an external stimulus. Single-crystal-tosingle-crystal<br />

transformations by exchange of guest<br />

molecule or by varying temperature condition have<br />

been reported for some MOFs 9 and these<br />

transformations have been implicated in controlled<br />

delivery of the guest molecules. Here we show by<br />

theoretical methods, that at high pressure MOF-5<br />

undergoes reversible structural transformation i,e<br />

volume compression/decompression stages which<br />

may be continued for number of cycles. Taking<br />

advantage of the cyclic nature of MOF-5<br />

deformation under pressure, a purely mechanical<br />

gas storage and delivery system has been proposed.<br />

We considered hydrogen as a representative gas<br />

and performed simulations with hydrogen filled<br />

MOF-5. Given the pore size of MOF-5 (available<br />

volume ~ 11267 Å 3 ), at 100 MPa and at room<br />

temperature, ~167 molecules of hydrogen can be<br />

entrapped inside the crystal (considering density of<br />

hydrogen at this condition is 49.25 kg/m 3 ). This<br />

amounts to 7wt % H 2 per gm of MOF-5. Under<br />

pressure as the crystal deforms the entrapped gas<br />

will be released, which may be used further. In the<br />

proposed process, using pressure induced<br />

mechanical gas delivery system, efficiency as high<br />

as 90% may be achieved.<br />

*Corresponding author: cagin@che.tamu.edu<br />

REFERENCES<br />

[1] Li, H.; Eddaoudi, M.; O.Keeffe, M.; Yaghi, O.<br />

M. Nature, 1999, 402, 276-279.<br />

[2] Eddaoudi, M.; Kim, J.; Rosi, N.; Vodak, D.;<br />

O'Keeffe, M.; Yaghi, O. M. Science, 2002, 295,<br />

469-472.<br />

[3] Rosi, N.; Eckert J., Eddaoudi M.; Vodat D.T.;<br />

Kim J.; O'Keeffe, M.; Yaghi, O. M Science, 2003,<br />

300, 1127-1129.<br />

[4] Rowsell, J. L.C. Yaghi, O. M. Angew. Chem<br />

Int. Ed. 2005, 44, 4670-4679.<br />

[5] Mueller, U. Schubert M.; Teich F.; Puetter H.;<br />

Schierle-Arndt K.; Pastre J. J. Mater. Chem., 2006,<br />

16, 626-636.<br />

[6] Ferey, G. Chem. Soc. Rev. 2007, 37, 191-214.<br />

[7] Han, S. S. and Goddard III, W. A. J. Phys.<br />

Chem. C, 2007, 111 (42), 15185 -15191.<br />

[8] Mattesini, M.; Soler, J. M.; Yndurain, F. Phys.<br />

Rev. B 2006, 73, 094111 1-8.<br />

[9] Wu, C-D.; Lin, W. Angew. Chem. Int. Ed.<br />

2005, 44, 1958-1961.<br />

6th Nanoscience and Nanotechnology Conference, zmir, <strong>2010</strong> 765

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