全氟辛烷磺酸(PFOS)在多胶束和单胶束囊泡中的相分离和被动扩散

Stephanie L., Wunder, Tutan Das, Aka, Thomas, Boller, Graham, Dobereiner
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引用次数: 0

摘要

全氟烷基物质(PFAS)是重要的环境危害物质,它们通过细胞膜进入微生物和动物组织,并与蛋白质和脂质结合1。研究人员研究了一种常见的全氟辛烷磺酸(PFOS)与由二棕榈酰基磷脂酰胆碱(DPPC)构成的模型细胞膜的相互作用,这种相互作用是多胶束小泡(MLVs)和大单胶束小泡(LUVs)中 DPPC/PFOS 摩尔比的函数。全氟辛烷磺酸既是制备出来的,也与囊泡一起孵育,并通过纳差扫描量热仪(用于测量相变温度,Tm)和动态光散射(DLS)或光学显微镜(用于测量粒度)监测其在 LUVs 和 MLVs 中的掺入情况。使用全氟辛烷磺酸制备的 MLV 和 LUV 没有观察到预转变。LUVs 和 MLVs 在长达 30 天的时间内保持完好,LUVs 的尺寸约为 100 纳米,MLVs 的尺寸约为 10-100 微米。当 DPPC/PFOS 的摩尔比为 75/1 ~ 7.5/1 时,出现了单一的 Tm,随着 DPPC/PFOS 摩尔比的降低,Tm 减小并变宽,这与之前观察到的情况相同。2 当 PFOS 浓度较高时(DPPC/PFOS < 5/1),观察到了两个或三个相变,其中一个 Tm 的温度接近纯净 MLVs/LUVs 的温度,另一个温度较低。这被解释为相分离为富含 PFOS 和贫含 PFOS 的区域。当 MLV 与 PFOS 共孵育时,可观察到纯 DPPC 所特有的主相位(Tm)和过渡相位(Tpre),这表明存在未掺入 PFOS 的双层膜。Tm 的强度随着时间、温度(即高于 Tm 的速度快于低于 Tm 的速度)和外部 PFAS 浓度的增加而降低,Tpre 则增加(T = Tm - Tpre 降低)。同时,还观察到 MLV 在较低温度下出现相变,并随着时间的推移而消失。这些结果表明,PFOS 逐渐从 MLV 的外层小叶(含有 PFOS)渗透到内层双分子层(未含有 PFOS),由此推断 PFOS 在 DPPC 双分子层之间(而不仅仅是在 DPPC 双分子层中)进行了被动扩散,这种扩散在 Tm 以上比在 Tm 以下发生得更快。虽然以前也观察到过全氟辛烷磺酸在细胞膜上的扩散,但这种效应被归因于与膜蛋白的结合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Phase Separation and Passive Diffusion of Perfluorooctane Sulfonic Acid (PFOS) in Multilamellar and Unilamellar Vesicles
Perfluorinated alkyl substances (PFAS) are important environmental hazards that enter microorganisms and animal tissues via their cellular membranes, where they bind to both proteins and lipids1. The interaction of a prevalent PFAS, perfluorooctane sulfonic acid (PFOS), with a model cell membrane composed of dipalmitoyl phosphatidylcholine (DPPC) was investigated as a function of molar ratio of DPPC/PFOS in both multilamellar vesicles (MLVs) and large unilamellar vesicles (LUVs). The PFOS was both prepared and incubated with the vesicles and its incorporation into the LUVs and MLVs was monitored by nano- differential scanning calorimetry (for phase transition temperatures, Tm) and by dynamic light scattering (DLS) or optical microscopy for size. For MLVs and LUVs prepared with PFOS, no pretransition was observed. The LUVs and MLVs remained intact for up to 30 days with sizes ~ 100nm for LUVs and ~ 10-100 μm for MLVs. At DPPC/PFOS ~ 75/1 to 7.5/1, there was a single Tm, that decreased and broadened as the DPPC/PFOS molar ratio decreased, as previously observed.2 At higher PFOS concentrations, DPPC/PFOS < 5/1, two or three phase transitions were observed, with one Tm at a temperature close to that of the neat MLVs/LUVs and one at lower temperature. This was interpreted as phase separation into PFOS rich and PFOS poor domains. When MLVs were incubated with PFOS, both the main (Tm) and pretransition (Tpre), characteristic of neat DPPC, were observed, indicating the presence of bilayers with no incorporated PFOS. The intensity of Tm decreased with increased time, temperature (i.e. faster above than below Tm) and the external PFAS concentration, and Tpre increased (T = Tm - Tpre decreased). Concurrently, a phase transition in the MLVs at lower temperature was observed and disappeared with time. These results indicate that there was progressive penetration of the PFOS from the outer leaflets (that had incorporated PFOS) to the interior bilayers (that had no incorporated PFOS) of the MLVs, and by implication that there was passive diffusion of PFOS across (not just into) the DPPC bilayers, which occurred more quickly above than below Tm. While diffusion of PFOS across cellular membranes has previously been observed, this effect has been attributed to association with membrane proteins.
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