In considering the microscopic structure of ice, it is important to distinguish between 'single' crystals and 'polycrystals'. A single crystal is one in which the strict periodic arrangement of the molecules continues in all directions throughout the material with no large-angle boundaries. By contrast, a polycrystal is essentially a composite of many, more-or-less randomly-oriented single crystals such that large-angle crystal boundaries arise where the individual single crystals meet.
Natural ice found on Earth in glaciers and ice sheets is polycrystalline. The image to the right shows a thin section of polycrystalline ice from Dome C, Antarctica (ex: Barnes, PhD thesis, 2002) viewed between crossed polarisers that shows the individual crystals very clearly. The crystals are a few millimetres across.

The vein system has been observed by numerous workers and indeed it can be readily seen with the naked eye - if you allow an ice cube from your fridge to warm up a bit, the veins look like tiny silvery lines. The geometry of the vein system has been determined (see e.g. Mader 1992a) and is controlled by the 'dihedral angle', which is the angle subtended at a crystal boundary in contact with water.
The composite figure to the left shows the dihedral angle in figure (a) and the cross-section of a vein at a 'triple-junction' (i.e. the line where three crystals meet) in figure (b). Four veins meet in a 'node' at the points where four crystals meet. The images in figures (c) and (d) are photographs of the vein system in laboratory-grown ice using transmitted white light (ex: Mader 1992a. The veins can be seen because water has a different refractive index from ice. The optics of the system is described in detail in Mader 1992a. In (c), a vein cross-section is clearly visible. The vein cross-section is not strictly uniform. This is primarily because the vein is not exactly perpendicular to the angle-of-view, but may also be due to slightly different values of interfacial energy for the three crystal-crystal boundaries associated with the cross-section. The photograph in (d) shows a node where four veins meet. All the veins in these images are approximately 100mm across. The diagram in figure (e) illustrates the vein network around a crystal (redrawn after Price 2000).A paper on the implications of the liquid water content for radar measurements has recently been published (West et al 2007) and several other manuscripts are currently in preparation.
Those involved in this work include Dr. Heidy Mader, Dr David Chandler (NERC PDRA 2004-2007), Dr Bryn Hubbard (Institute of Geography and Earth Sciences, Aberystwyth), Dr David Rippin (NERC PDRA 2004-2006), Dr Jared West (School of Earth and Environment, Leeds), Professor Tavi Murray (Department of Geography, Swansea).
Funded by the Natural Environment Research Council (UK)
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