By Hesse J.
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Extra info for A p-extremal length and p-capacity equality
15 (2003) 257  A. Alberti, S. Quartieri, G. Vezzalini, Eur. J. , 8 (1996) 1273.  G. Artioli, K. Stahl, G. Cruciani, A. C. Hanson, Am. Mineral, 86 (2001) 185.  K. Stahl, G. C. Hanson, Phys. Chem. Minerals, 23 (1996) 328.  A. Sani, G. Cruciani, A. Gualtieri, Phys. Chem. Minerals, 29 (2002) 351. 40  M. Johnoson, D. O'Connor, P. A. Catlow, SL. Owens, G. Sankar, R. J. Teat, R. Stephenson, J. Phys. Chem. B, 107 (2003) 942.  E. Galli, G. Gottardi, H. Mayer, A. Preisinger, E. Passaglia, Acta Cryst.
Its structure is constructed exclusively by two fused four rings forming triple cranckshaft chains which circumscribe a 1D 10-ring channel system, in the same way as the same cranckshaft chains circumscribe the 18-membered rings of VPI-5. , as occurs in VPI-5. A1PO-H2 is not thermally stable; upon heating to 100°C, it transforms into AlPO-tridymite. It is however possible to dehydrate A1PO-H2 under vacuum at room temperature without topological changes even if strong distortion of the framework occurs.
We know that UiO-26 can loose its unshared water molecules reversibly, but if calcined and dehydrated at 400°C and 600°C, it transforms irreversibly into two new phases, the structures of which are unknown . A1PO-14  and A1PO-JDF , microporous materials of this group, can loose the additional bonding, by calcinations and dehydration, without topological changes (Table 5). Table 5 AIPO4 materials that contain Al polyhedra that share edges. Al atoms can be 4-, 5- or 6coordinated. Al/P= 1 Fig.