Laboratories of The Rockefeller Institute for Medical Research.
J Gen Physiol. 1946 Jul 20;29(6):441-69.
Analytical methods which are accurate to about 1 per cent have been developed for the determination of small amounts (ca. 500 gamma) of bis(beta-chloroethyl)-sulfide (H), ethyl-bis(beta-chloroethyl)amine (EBA), tris(beta-chloroethyl)amine (TBA), beta-chloroethyl-benzylsulfide (benzyl-H), and beta-chloroethyl-ethylsulfide (ethyl-H). The determinations are made by micro titration of the HCl liberated upon complete hydrolysis of the vesicants. A description is given of an apparatus suitable for applying vapors of vesicants to unit areas of skin. A very precise and reproducible micropipetting technique is described for the introduction of the vesicants into the penetration apparatus. By means of this penetration apparatus studies have been made of several factors which may influence the rate at which vesicant vapors penetrate into skin. Model experiments have been performed in which H was allowed to vaporize and the vapor was absorbed on a surface such as that of diethylene glycol or vaseline. It has been found that if the surface of liquid H is increased by spreading the agent on filter paper, the rate of evaporation is markedly increased. Furthermore, if the vapor is agitated by means of a magnetically driven fan, the rate of absorption by diethylene glycol is greatly accelerated. With vaseline as the absorbing surface it has been found that the area of the absorbing surface has an effect on the rate of absorption of H vapor. More H is absorbed by vaseline spread on filter paper to give a rough surface than is absorbed by a smooth film of vaseline. Measurements of the rate of penetration into human skin of H, EBA, TBA, benzyl-H, and ethyl-H vapors have been performed at 21-23 degrees C. and 30-31 degrees C. by means of the penetration apparatus described in this paper. The measurements were carred out on human volunteers under conditions of controlled temperature and humidity. When human skin is exposed to air saturated with H vapor, the H penetrates the skin of the forearm at a rate of about 1.4 gamma per cm.(2) per minute (temperature 21-23 degrees C.; relative humidity 46 per cent). This value was found to hold in experiments in which H vapor was applied for 3 to 30 minute intervals, thus indicating that the permeability of the skin to H vapor is not altered during a 30 minute exposure. Agitation of the H vapor by fanning did not result in any measurable increase in the rate of penetration. Two of the volunteers were Negroes; the permeability of their skin to H vapor did not differ appreciably from that found for the other subjects. When human skin is exposed to air saturated with EBA vapor, the vesicant penetrates at the rate of 2.8 gamma per cm.(2) per minute (temperature 22 degrees C., relative humidity 50 to 52 per cent). The amount of EBA penetrated is linear with exposure time for exposure periods of 5 to 20 minutes. Under similar conditions, it was found that TBA penetrates at a rate of about 0.18 gamma per cm.(2) per minute (temperature 22-23 degrees C.; relative humidity 45 to 48 per cent). This value was found to hold in experiments in which TBA vapor was applied for 30 to 60 minute intervals. The amount of TBA penetrated is linear with exposure time. In the case of benzyl-H, a linear relationship between the amount lost from the penetration cup and exposure time was also observed but the plot did not pass through the origin. It is suggested that this anomaly is due to retention on the skin surface of an appreciable quantity of benzyl-H as a result of rapid physical adsorption or chemical combination with a constituent of the skin. The rate of penetration of benzyl-H may be calculated from the slope of the plot and is found to be 0.35 gamma per cm.(2) per minute (temperature 22 degrees C., relative humidity 55 to 60 per cent). The results with ethyl-H showed great variation among individual subjects and no satisfactory value for the rate of penetration can be given as yet. Measurements were also made of the rate of penetration of H, EBA, and TBA vapors at 30-31 degrees C. (relative humidity 47 to 49 per cent). At this temperature, a linear relationship was observed between the amount penetrated and the time of exposure. H vapor penetrated at a rate of 2.7 gamma per cm.(2) per minute, EBA vapor at 5.1 gamma per cm.(2) per minute, and TBA vapor at 0.29 gamma per cm.(2) per minute. Three of the subjects in the EBA measurements were Negroes. The permeability of their skin to EBA vapor did not differ from that found for the white subjects. Despite this fact, their skin failed to vesicate after an exposure period twice that which caused 50 per cent vesication in the white subjects. Calculation of the precision of the data showed that the average deviation, standard deviation, and standard error were not appreciably different for the data obtained with human subjects as compared with data for control experiments in which human skin was not involved. Consequently, no significant differences in the rate of penetration into the skin of individual subjects can be discerned from the data presented in this communication. The increase in the rate of penetration of H, EBA, and TBA vapors from 21-23 degrees C. to 30-31 degrees C. is approximately proportional to the increase in volatility of each agent. These results indicate that at the same gas concentration in milligrams per liter, H, EBA, and TBA vapors would all penetrate at about the same rate. The data presented above permit a determination of the approximate amount of each vesicant which must penetrate to cause vesication in about 50 per cent of the exposed sites. This amount has been designated by the symbol V(50). The V(50) for H and TBA at 21-23 degrees C. is the same, being about 6gamma; at 30-31 degrees C., the V(50) is 4 to 5 gamma. On the other hand, the V(50) for EBA at 22 degrees C. and 30-31 degrees C. is about 26 to 28 gamma. Thus, per gamma penetrated, H and TBA vapors are about equally effective in producing vesication while EBA vapor is only (1/5) to (1/8) as effective.
分析方法的精度约为 1%,已被开发用于测定少量(约 500 伽马)双(β-氯乙基)-硫化物(H),乙基-双(β-氯乙基)胺(EBA),三(β-氯乙基)胺(TBA),β-氯乙基-苄基硫醚(苄基-H)和β-氯乙基-乙基硫醚(乙基-H)。这些测定是通过完全水解水疱剂释放的 HCl 的微量滴定来完成的。本文介绍了一种适用于将水疱剂蒸气施加到皮肤单位面积的装置。本文还介绍了一种非常精确和可重复的微量移液技术,用于将水疱剂引入渗透装置中。通过该渗透装置,研究了可能影响水疱剂蒸气渗透到皮肤中的速率的几个因素。在模型实验中,允许 H 蒸发,并将蒸气吸收到二乙二醇或凡士林等表面上。结果发现,如果通过在滤纸上将试剂展开来增加 H 的表面,蒸发速率会明显增加。此外,如果通过磁性驱动的风扇使蒸气搅拌,则二乙二醇的吸收速率会大大加快。对于凡士林作为吸收表面,发现吸收表面的面积会影响 H 蒸气的吸收速率。用滤纸展开的 H 吸收的凡士林比光滑的凡士林膜吸收的 H 多。在 21-23°C 和 30-31°C 下,通过本文所述的渗透装置,对 H、EBA、TBA、苄基-H 和乙基-H 蒸气渗透到人体皮肤中的速率进行了测量。测量是在受控温度和湿度条件下对人体志愿者进行的。当人体皮肤暴露于充满 H 蒸气的空气中时,H 以约 1.4 伽马/平方厘米每分钟(温度 21-23°C;相对湿度 46%)的速率渗透前臂皮肤。在 H 蒸气应用 3 至 30 分钟的实验中发现了该值,这表明在 30 分钟暴露期间皮肤对 H 蒸气的渗透性不会改变。用风扇搅拌 H 蒸气不会导致渗透速率的任何可测量增加。两名志愿者是黑人;他们的皮肤对 H 蒸气的渗透性与其他受试者没有明显差异。当人体皮肤暴露于充满 EBA 蒸气的空气中时,水疱剂以 2.8 伽马/平方厘米每分钟的速率渗透(温度 22°C,相对湿度 50-52%)。暴露时间为 5 至 20 分钟时,EBA 的渗透量与暴露时间呈线性关系。在相似的条件下,发现 TBA 以约 0.18 伽马/平方厘米每分钟的速率渗透(温度 22-23°C;相对湿度 45-48%)。在 TBA 蒸气应用 30 至 60 分钟的实验中发现了该值。TBA 的渗透量与暴露时间呈线性关系。对于苄基-H,从渗透杯中损失的量与暴露时间之间也观察到线性关系,但该图未通过原点。建议这种异常是由于 H 迅速物理吸附或与皮肤成分发生化学结合而在皮肤表面保留相当数量的苄基-H 所致。苄基-H 的渗透速率可以从图的斜率计算得出,在 22°C 和相对湿度 55-60%时为 0.35 伽马/平方厘米每分钟。乙基-H 的结果在个体受试者之间差异很大,目前还不能给出渗透速率的令人满意的值。还测量了 H、EBA 和 TBA 蒸气在 30-31°C(相对湿度 47-49%)下的渗透速率。在该温度下,观察到渗透量与暴露时间之间存在线性关系。H 蒸气以 2.7 伽马/平方厘米每分钟的速率渗透,EBA 蒸气以 5.1 伽马/平方厘米每分钟的速率渗透,TBA 蒸气以 0.29 伽马/平方厘米每分钟的速率渗透。EBA 测量中的 3 名受试者是黑人。他们的皮肤对 EBA 蒸气的渗透性与白人受试者没有区别。尽管如此,他们的皮肤在暴露时间是引起白人受试者 50%水疱的两倍后仍未发生水疱。数据精度的计算表明,与涉及人体皮肤的对照实验相比,人体受试者获得的数据的平均偏差、标准偏差和标准误差没有明显差异。因此,从本通讯中提供的资料中,无法辨别个体受试者皮肤渗透速率的显著差异。H、EBA 和 TBA 蒸气从 21-23°C 增加到 30-31°C 的渗透速率的增加与每种试剂的挥发性增加大致成正比。这些结果表明,在相同的毫克/升气体浓度下,H、EBA 和 TBA 蒸气的渗透速率大致相同。上文提供的数据可确定引起约 50%暴露部位水疱所需的每种水疱剂的近似量。该量已被指定为符号 V(50)。在 21-23°C 时,H 和 TBA 的 V(50)相同,约为 6 伽马;在 30-31°C 时,V(50)为 4 至 5 伽马。另一方面,EBA 在 22°C 和 30-31°C 时的 V(50)约为 26 至 28 伽马。因此,每渗透伽马,H 和 TBA 蒸气在产生水疱方面的效果大致相同,而 EBA 蒸气的效果仅为(1/5)至(1/8)。