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