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Water Cluster History


The anomalous properties of water have excited chemists to attempt explanation for many years. These hypotheses have mainly involved consideration of the existence of different water clusters within liquid water. Such clusters are either low density (similar in density to that of hexagonal ice) or of higher density; their changing relative concentrations determining the changes in physical properties.


Ice Ih cell cluster

Low-density ice-like particles

Dense liquid water

Higher-density liquid matrix

 

The first reported suggestion for clusters being responsible for water's anomalous density maximum was by Whiting in 1884 [764]. Melting ice was proposed to release solid low-density ice crystals (left) which remained within the higher density matrix (right). Whiting proposed that the concentrations of these solid particles changed with temperature and pressure.

 

Chadwell [765] reviewed the first 40 years in the development of this idea.


Ice Ih cell cluster

Low-density ice-like clusters

 

 

 

 

 

=

Walrafen pentamer;  'quartz-like' cluster

Higher-density clusters

 

 

In 1933, Bernal and Fowler developed this model in two important respects [1177]. Firstly the denser matrix was proposed to be made up of 'quartz-like' clusters (right) that may pack closer together. Secondly, and significantly, they introduced the idea of equilibration of water molecules interconverting between the clusters [766].


Ice Ih cell cluster

Low-density ice-like clusters

Ice Ih cell cluster, with an interstitial water molecule

Cluster plus an interstitial molecule

 

 

An interesting idea, based on interstitial water molecules within the ice hexagonal box (right) was put forward in 1946 [767]. Such clusters are not now thought to be present in significant quantities.


Dodecahedral water cluster

Low-density clathrate clusters

Dodecahedral water cluster, with an interstitial water molecule

Cluster plus an interstitial molecule

 

 

Pauling suggested another interstitial arrangement in 1959, making use of his interest in clathrate structures [8b]. These clusters were quickly dismissed, however, for being unable to explain the available diffraction data if the main constituents in liquid water.


   4-membered cyclic water cluster     5-membered cyclic water cluster    6-membered cyclic water cluster      7-membered cyclic water cluster  8-membered cyclic water cluster

 

 

A random network model of water, also introduced by Bernal [1177] and published in 1975 [19], contained a mixture of water clusters including 4-, 5-, 6-, 7- and 8-membered rings. Some success has been had using this model but its homogeneous nature is not universally applicable or productive.


Ice Ih cell cluster

An ice Ih cluster

 

 

Wilse Robinson's research group introduced the outer structure two-state mixture model in 1987, which involved a mixture of water clusters related to ices 1h, II and III. The group went on to produce a number of papers using the model to successfully and quantitatively explain many of water's anomalies (for example, [23, 56, 57, 60, 69, 73, 148]).


 

 

A cluster from ice-two < p> 

An ice II cluster

A cluster from ice-three

An ice III cluster

 

 

The only difficulty with this model concerns whether the clusters can exist in liquid water and so the clusters should perhaps be more realistically considered as 'indicative' structures.


Dodecahedral water cluster

 

 

 

 

 

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5-membered cyclic water cluster6-membered cyclic water cluster

 

 

In 1998 Dougherty and Howard proposed an equilibrium model for water [15] involving dodecahedra, 5- and 6-membered clusters based on several of water's anomalous properties.


Dense water shown as 2 water tetramers

Dense cluster

 

 

 

=
8-molecule open water cluster

Low-density cluster

 

These water cluster models lead logically on to the icosahedral water cluster model , published in 2000 [55] and described at this site. This model is based on dense and less dense clusters equivalent to an equilibrium opposite (see animated gif, 129 kB). The less-dense bicyclo(2,2,2) structures (right) occur when the hydrogen bonding is strongest and the dense structures occur when the weaker but more numerous van der Waals interactions predominate.


 

 

 

 

 

  8-molecule open water cluster

 

Low-density cluster

 

 

 

 

 

 

 

=

280-molecule icosahedral open water cluster

Icosahedral cluster

 

 

When conditions arise (such as on supercooling at low temperatures) when there is a high concentration of the expanded 8-membered bicyclo clusters, partial to complete icosahedral clusters (right) may arise. A full description of this is given elsewhere on this site. This cluster contains the dodecahedral, ice Ih cell, 5-, 6-membered and 8-membered bicyclo(2,2,2) subclusters included in the historical survey of models, above.

 

The meaning of the term 'cluster' has evolved during this time as well. In the beginning, water clusters were thought of as discrete entities, like crystals, with long (e.g. > seconds) individual lifetimes where the same molecules were involved throughout. Nowadays, we know that molecules may leave or add to clustersa with frequencies that depend on their situation and obey statistical laws with clusters appearing, evolving and disappearing with involvement of physically different molecular constituents. The aqueous environment is heterogeneous with more than one type of environment present and with the relative preponderance of these environments changing with temperature, pressure, solutes and surfaces. Clusters are now thought of as dynamic entities offering a simplified view into a complex, broken and rapidly shifting environment. As such they reveal water's underlying nature.


Footnotes

a   Some authors prefer the term 'dynamic heterogeneities' to 'clusters', but this site does not. The same type of structuring is meant in both cases. [Back]

 

 

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This page was last updated by Martin Chaplin on 22 June, 2008


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