A. Chlorides in natural hailstones

Chloride filter replica experiments were performed on hailstones from different precipitations in the Colorado-Nebraska region. The results on a hailstone collected at Niwot, Colorado, 10 June 1969 and another at Chadron, Nebraska, 7 June 1967 are shown in Figures 1 and 2, respectively.

Figure 1 is a crossed polar polarized light photograph of a slice that is close to that analyzed for chlorides, in which the structure of crystals is evidenced, and the zones of the enlargements of the chloride analysis are indicated. A thin layer having been shaved away by the microtome, the correspondence between crystals and chloride pattern is not exact. In Figures 1a, 1b, and 1c, enlarged details of the replica on a millipore filter (0.22 μm pore size) are shown. The sensitivity of the filter technique makes chloride detection possible (Fig. 5) in hailstones of low NaCl content such as those from the precipitation in the Colorado-Nebraska region.

The first result is confirmation of Reference Mizuno and KuroiwaMizuno and Kuroiwa’s (1970) conclusion that solute molecules are not incorporated within the ice lattice but are mainly segregated along grain boundaries; in fact, a perfect correspondence between chloride patterns and grain boundaries was observed.

By comparing Figure 1b with Figure 1a or Figure 1c, it can be seen that small crystals produce strong patterns, while larger crystals show faint patterns. This behavior may be explained by variations in the rate of crystallization; when the rate is low large crystals are produced and the crystallization front rejects a larger amount of solute. Nevertheless. fluctuations in the chloride content of accreted droplets of a cloud may also affect the chloride distribution, as can be seen from Figures 2b and QC, where enlarged details in a transition region of crystals are shown. In this situation, a sharp decrease is seen in chloride content going from larger radial crystals to smaller ones. This behavior contrasting with that of the former hailstone may be explained by the inner layer (the small crystals) being completely frozen in a “non-porous" structure, and the outer layer superimposed, no longer permitting the liquid penetration of high chloride content from the outside during final freezing. It should also be noted in this hailstone (Fig. 2a) as well as in all those examined (Fig. 1e, Fig. 6) that the periphery of the slice was always characterized by a high quantity of chloride from both solute material (reactions along grain boundaries) and undissolved material (reactions corresponding with contaminating particles; see Figure 6). Penetrating channels of reactions due to particles were also frequently observed from the periphery toward the center (Fig. 6).

Fig.1 .

Crossed polarized light picture of a hailstone slice (Niwot, Colorado, 10 June 1969, with chloride reaction replicas on filter at the area near the corresponding zones shown by the arrows and near the strip marked.

Fig.2 .

Crossed polarized light picture of a section of a hailstone slice (Chadron, Nebraska, 7 June,1967), with chloride reaction replicas on the filter at the area near the corresponding zone shown by the arrows.

Fig.3 .

Chloride reaction patterns of grain boundaries on 0.8 μm pore filter.

Fig.4 .

Chloride reaction patterns of air bubbles (shown by arrows) in a hailstone (on 0.22 μm pore filter).

Intense spots of solute were always noticed along boundaries of individual air bubbles in any examined hailstone; an example is shown in Figure 4 where the bubbles are contrasting with a faint background of grain boundaries.

Figures 3 and 6 show replicas made an 0.8 μm pore-size filters. By using a larger pore-size filter a heavier or darker reaction pattern resulted due to deeper penetration of the ice surface into the pores. In this experiment a more quantitative evaluation could be made of the total chloride content at different zones in the hailstones, but the finer details of the ice-bubble structure and of the crystal grain boundaries were much more prominent in the replicas made on 0.22 μm pore size filters as seen in Figures 4. 5, and 7.

Fig.5 .

Faint patterns of chloride reactions along the grain boundaries in a hailstone (on 0.22 μm pore filter).

Fig.6 .

Chloride reactions from contaminating particles near the periphery of a hailstone (on 0.8 μm pore filter).

Fig.7 .

Chloride reaction pattern showing a loop resembling a dislocation of Frank-Read type (on 0.22 μm pore filter).

Although weak in intensity, solute reaction patterns seem to be observable by this technique along sub-grain boundaries and dislocation lines in accordance with the theory of dislocations in metals. In fact, Reference CottrellCottrell (1953) has demonstrated that the solubility of a solute atom is higher in a dislocation than elsewhere, and the solute atoms will be located preferentially in the expanded region near a dislocation. Each dislocation will collect more solute atoms during solidification when the mobility of solute atoms is high. Therefore, it would be expected that those types of volume sources called Frank-Read sources which can reach maximum dimensions of a few hundred micrometers, could be readily observed by the reaction pattern produced at such dislocation regions. This dislocation shape emerges when a step begins on the surfaces fixed in the ends by a right-handed and a left-handed screw dislocation, and this step being anchored grows only by bulging.

Fig.8 .

Chloride reaction patterns showing the undissolved particles, the tiny bubbles, and grain boundaries of different intensities within a hailstone (on 0.22 μm pore filter).

A feature resembling such a dislocation was apparent in the hailstones examined; an example is given in Figure 7 together with grain and subgrain boundary patterns. The size is in accordance with observations of Reference DashDash (1956) on dislocation loops in silicon.

A remarkable difference was noticed in the chloride content of embryos from one hailstone to another. Sometimes a very high content was found due to the presence of giant particles; in other embryos the region was almost chloride-free.

It is probable that this technique of observing the chloride distribution within a hailstone could be used to determine the hailstone’s internal features. As seen in one small section of a chloride reaction replica (Fig. 8), the grain size and its boundaries, the many tiny bubbles (in this relatively clear ice zone), and the chloride particulates, all can be exactly located within this hailstone. Conclusions seem premature relating the environmental growth conditions of hailstones to the chloride distributions, since the filter technique should also be applied to contaminated ice artificially grown by accretion. Further investigation is needed of the way in which the solute is segregated during freezing of individual droplets in different growth conditions as well as studies of varying ice densities of the resulting dry accretion. It is expected that a distribution of chlorides on the filter in the dry growth will have different patterns from those in the wet or spongy accreted ice. This could give a criterion for distinguishing the different types of growth, which eliminates the effects of migration using the evaporation technique. Moreover, the effect on chloride distribution of the final freezing of liquid water seeping into a low density, porous structure should be investigated by this technique. In fact, the frequent penetrating channels of reactions, the high chloride content of the peripheral layer, and the above-mentioned correlation between pattern intensity and crystal sizes seem to add evidence for a model which implies a final wetting and freezing of a previously formed porous structure.

B. Solute segregation in ice from a low concentration NaCl solution

A NaCl solution (0.3 g/1) was radially frozen at —25°C in a plastic cylinder (4.5 cm diameter) insulated on top and bottom. Chloride filter replicas were taken on sections normal to the cylinder axis, the plane having been shaved flat by using the microtome. Results are shown in Figure 9 which gives from left to right the chloride distribution from the periphery toward the center. As we observed in hailstones, complete solute segregation exists along grain boundaries. There is evidence of a surface layer of high chloride concentration followed by a region of poor concentration gradually increasing toward the center. Similar behavior was found by Reference Smith and PounderSmith and Pounder (1960) through chemical analysis of melted slices cut at different distances from the surface. Apparently they were unable to demonstrate the existence of a surface layer of concentrated chlorides and could not correlate the distribution with internal features.

Fig.9 .

Reaction patterns obtained form bulk ice frozen a low concentration NaCl solution.

C. Solute segregation in ice from NaCl solution of sea-water concentration

A 30 g/1 NaCl solution was radially frozen in the same conditions as the former solution. As mentioned before, with ice at high NaCl content, a modification was introduced in the technique, since the filler could be wetted and a reaction shown to be taking place at very low temperatures. The ice surface and the filler were placed on a cold plate whose temperature was finely regulated, In a sequence of pictures from Figures ma to 10f results are shown on filter patterns corresponding to gradually warmer temperatures from — 21.2°C (eutcctic) to — 18°C. The pressure exerted on the ice rod was also critical, and was kept constant for all the experiments.

Fig.10 .

Reaction patterns obtained from bulk ice frozen from a 30 g per liter. NaCl solution. Reaction obtained at various temperatures. From top left to bottom right successive photographs show the results of reactions at — 2I.2°C, — 2C.5°C, — 20.o°C, —19.5°C, —19.0°C, and 18.0°C.

In Figure 10a the chlorides are concentrated in brine droplets; they are segregated successively between platelets of relatively pure ice (Fig. 10b). As the temperature increases, they expand until they completely cover the filter (Fig. 10f).