Water Chains in Hydrophobic Crystal Channels: Nanoporous Materials as Supramolecular Analogues of Carbon Nanotubes
Water Chains in Hydrophobic Crystal Channels: Nanoporous Materials as Supramolecular Analogues of Carbon Nanotubes
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DOI:
10.1002/anie.201002418
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发表时间:
2010-01-01
影响因子:
16.6
通讯作者:
Davis, Anthony P.
中科院分区:
文献类型:
--
作者:
Natarajan, Ramalingam;Charmant, Jonathan P. H.;Davis, Anthony P.
The behavior of water in narrow apolar pores has attracted much recent interest. Although it might seem that such channels should repel water,[1] it transpires that they can be hydrated and moreover that their “hydrophobic” nature promotes rapid water flow. The phenomenon is observed in biology, where the pores of aquaporins (water-transporting proteins) are composed largely of hydrophobic amino acids.[2] It is also seen for carbon nanotubes (CNTs) which, according to both theoretical [3] and experimental [4] studies, allow rapid passage of water molecules. Water flow through CNTs can be selective [5] and controllable,[6] suggesting applications in water-purification [7] and nanofluidic devices. To understand these systems, it is important to gather structural information on water in hydrophobic environments. Especially relevant is the “water wire”, a one-dimensional hydrogen-bonded chain of water molecules. The water in aquaporin channels adopts this motif,[2] as does the water in the narrowest and best-understood CNTs.[3a, b, e] However, while there are many crystal structures which show water molecules in single file,[8] there is limited information on water wires in purely hydrophobic environments.[9] In particular there seem to be no structures in which water wires are surrounded exclusively by π systems. We now report the crystal engineering of channels bounded by nonpolar aromatic units, and the structural characterization of linear chains of water molecules within these pores.We have previously shown that steroidal bisphenylureas 1 (Figure 1 a) crystallize as monohydrates to form structures with hexagonal P61 symmetry, containing one-dimensional channels of unusually large diameter (Figure1b, c).[10] Groups R1 and R2 are directed into the channels, so that in principle they can be varied substantially without disrupting the crystal packing. Potentially, this should allow a broad scope for tuning of channel size and properties. Indeed, our original report [10] described three structures 1a–c, in which group R1 was altered to give pore diameters of 14.3, 12.3, and 11.6, respectively.