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| NIOSH Home > Safety and Health Topics >Skin Exposures and Effects >Occupational & Environmental Exposures of Skin to Chemicals- 2005> Abstracts |
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Absorption from contaminated soil into skin and silicone rubber membranes
S.E. Deglin, D.L. Macalady, A.L. Bunge* Background
The potential health risk from dermal exposure to contaminated soils depends on the amount absorbed and the toxicological potency. Dermal absorption measurements from soils usually are reported as the percent of the amount of chemical applied (i.e., the % absorption), which is the product of the contaminant concentration on the soil (Csoil) and the amount of soil on the skin (Msoil /A). In actual exposures the amount of soil on skin is less than required to completely cover the exposed area. Despite this, absorption experiments are almost always conducted with enough soil to cover the skin surface with several layers. If chemical from the extra soil layers does not migrate to the skin, then the % absorption in an actual exposure could be much larger than observed in these multi-layer experiments. Thus, the goal of this study is to better understand the effect of Msoil /A on the % absorption. Method
The permeation of 4-cyanophenol (4CP, molecular weight = 119, octanol-water partition coefficient = 40) from soil was measured through human skin or silicone rubber membranes (SRM) used as a surrogate for skin. The SRM from Samco Silicone Products ( The soil in this study was the < 250 mm fraction of a clay loam collected from Ft. Collins, CO. which contained approximately 1 weight percent organic carbon. This soil was contaminated with 4CP to a concentration (Csoil) of 300 mg g-1 by mixing Experiments were conducted with the whole contaminated soil (i.e., all particles < 250 mm) or with the 38 to 63 mm fraction of the whole contaminated soil. Soil was applied in an amount (40 mg cm-2) that produced multiple layers or in smaller amounts between 0.2 and 8 mg cm-2. In a few experiments, 40 mg cm-2 of soil was applied and then dumped off leaving a thin layer of particles that adhered to the skin or SRM. The mass loading of this adhering layer was approximately 1 to 2 mg cm-2. Often, after a specified exposure time, the soil was removed, the membrane was rinsed with de-ionized water and then covered with a saturated aqueous solution of 4CP. After this, the experiment was continued for another 6 or 8 h. For each diffusion cell, the flux of chemical through the skin or SRM was monitored by HPLC analysis of the receptor solution collected over time. Results
Silicone Rubber Membrane (SRM) Early in the SRM experiments, the fluxes from the saturated solution and from supersaturated soil are similar, as we might expect since the thermodynamic driving force for transfer through the SRM are the same. However, the flux from soil decreased in time, unlike the saturated solution, for which flux was constant. This decrease was even larger for the adhering layer (Fig. 1).
After 12 h, about 67% of the 4CP from the adhering layer had penetrated the SRM. In the experiment with 40 mg cm-2 of applied soil, there was a 5 to 10-fold decrease over the 12 h exposure even though only about 6% of the chemical had penetrated the SRM. This suggests that there was limited transfer of chemical from soil particles that do not have direct contact with SRM. In a similar experiment, 40 mg cm-2 of soil was added to the adhering layer after 15 h and the diffusion cells that originally had 40 mg cm-2 of soil were shaken at 7, 10 and 15 h (Fig 2). The addition of soil to the adhering layer increased the flux almost to the value early in the experiment. A similar, but less dramatic response occurred when the multiple layers of the 40 mg cm-2 application was redistributed by shaking. Fig. 3 shows the cumulative mass of 4CP that permeated through SRM in 8 hours plotted as a function of the mass of whole soil on the skin. Chemical penetration through the SRM increased with soil loading until the loading was ~8 mg cm-2, after which further increases in soil loading had no effect. This is consistent with the idea that increasing the soil loading above the amount required to completely cover the surface does not increase dermal absorption. For the sieved soil, loading had no affect when it was larger than ~2 m cm-2 (data not shown).
Figure 4 shows the cumulative mass of 4CP that penetrated through the SRM from the sieved soil (38-63 mm) and whole soil (< 250 mm) as a function of time and soil loading in experiments conducted on two different days. The results for experiments repeated on both days were similar (Fig. 4a), indicating reasonable day-to-day reproducibility. As shown in Fig. 4b, the penetration rate through SRM was greater from the sieved soil fraction than from the whole soil. Penetration through SRM from the sieved soil applied with a loading of 0.8 mg cm-2 was similar to that obtained for 3.1 mg cm-2 of the whole soil and was nearly twice as much as from 1.6 mg cm-2 of the whole soil. This suggests that the adhering layer consists mostly of small particles. Independent determination of 4CP concentration on the whole and sieved soil fraction showed no significant difference. This would indicate that increased 4CP penetration from the sieved soil was not due to an increased amount of 4CP on the smaller particles.
Skin Figure 5 shows the results form an experiment, similar to that shown in Fig. 1, in which the contaminated soil was replaced after 12 h by saturated aqueous solution. From saturated water, the flux after 8 h was approximately 50% larger through skin than through the SRM. However, much different than SRM, flux through skin from the contaminated soil was less than 10% of that from saturated water. Because absorption into skin from the contaminated soil was small, contaminant concentration on the soil changed only a little and consequently, the flux did not decrease in time as was observed in the SRM experiments. The reason for the much smaller flux from the contaminated soil compared to the saturated aqueous solution is unknown, although one possibility is that skin is heterogeneous while SRM is not. Interestingly, the flux from saturated water reached steady state in 6 h in the SRM experiments, but continued to increase over 8 h in the skin experiments. By contrast, steady state was easily established in 4 h in experiments of flux through skin from saturated water applied after a previous application of 38-63 mm sieved pure 4CP powder (Fig. 6). It seems that the cleaning procedure leaves soil particles that are released slowly from the skin surface.
Comparing Figs. 5 and 6, it is evident that the flux through skin from the contaminated soil is almost the same as from the pure powder, perhaps because this heavily contaminated soil is similar to pure powder sieved to the same particle size. It is important to stress that flux through skin from the contaminated soil has a much greater variability than was observed in the SRM experiments. A 12-replicate experiment with 1.5 mg cm-2 of the sieved soil had a coefficient of variation of 50% in the cumulative amount of 4CP that penetrated the skin in 8 h. As a result, a plot like Fig. 4 prepared for skin showed no apparent correlation between flux and soil loading. Conclusions
Based on the observations described above, there appears to be little transfer of chemical from soil particles that do not have direct contact with the membrane or skin. Although SRM is commonly used as a surrogate for skin, absorption through skin shows some important differences compared to SRM. For SRM, the flux from contaminated soil is almost the same as from the saturated aqueous solution and pure powder, until absorption into the SRM reduces the concentration of chemical in the soil layer that is in contact with the SRM. Bringing fresh soil into contact the SRM surface increases the flux to its earlier value. For skin, the flux from contaminated soil is only about 10% of that from saturated solution, which is too small to cause the flux to decrease during the experimental times studied. For whole soil on the SRM studied, absorption increased to a maximum value at a soil loading of about 6 mg cm-2, above which absorption did not increase further. A similar relationship between soil loading and absorption could not be established because of the large variability in the skin experiments. We acknowledge support from the
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