首页> 美国卫生研究院文献>Biophysical Journal >X-ray diffraction structures of some phosphatidylethanolamine lamellar and inverted hexagonal phases.
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X-ray diffraction structures of some phosphatidylethanolamine lamellar and inverted hexagonal phases.

机译:某些磷脂酰乙醇胺的层状和倒六角相的X射线衍射结构。

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摘要

X-ray diffraction is used to solve the low-resolution structures of fully hydrated aqueous dispersions of seven different diacyl phosphatidylethanolamines (PEs) whose hydrocarbon chains have the same effective chain length but whose structures vary widely. Both the lower-temperature, liquid-crystalline lamellar (L(alpha)) and the higher-temperature, inverted hexagonal (H(II)) phase structures are solved, and the resultant internal dimensions (d-spacing, water layer thickness, average lipid length, and headgroup area at the lipid-water interface) of each phase are determined as a function of temperature. The magnitude of the L(alpha) and H(II) phase d-spacings on either side of the L(alpha)/H(II) phase transition temperature (T(h)) depends significantly on the structure of the PE hydrocarbon chains. The L(alpha) phase d-spacings range from 51.2 to 56.4 A, whereas those of the H(II) phase range from 74.9 to 82.7 A. These new results differ from our earlier measurements of these PEs (Lewis et al., Biochemistry, 28:541-548, 1989), which found near constant d-spacings of 52.5 and 77.0-78.0 A for the L(alpha) and H(II) phases, respectively. In both phases, the d-spacings decrease with increasing temperature independent of chain structure, but, in both phases, the rate of decrease in the L(alpha) phase is smaller than that in the H(II) phase. A detailed molecular description of the L(alpha)/H(II) phase transition in these PEs is also presented.
机译:X射线衍射用于解决七种不同的二酰基磷脂酰乙醇胺(PE)的完全水合水分散体的低分辨率结构,这些烃的烃链具有相同的有效链长,但结构差异很大。既解决了低温液晶层状(Lα)的问题,又解决了高温倒六角形(H(II))的相结构,并得出了内部尺寸(d间距,水层厚度,平均值确定每个相的脂质长度和脂质-水界面的头基面积)作为温度的函数。 L(alpha)/ H(II)相变温度(T(h))两侧的L(alpha)和H(II)相d间距的大小显着取决于PE烃链的结构。 L(α)相的d间隔范围为51.2至56.4 A,而H(II)相的d间隔范围为74.9至82.7 A.这些新结果与我们之前对这些PE的测量有所不同(Lewis等人,生物化学,28:541-548,1989),发现L(α)和H(II)相的d间距分别接近52.5和77.0-78.0A。在两个阶段中,d间距都随温度的升高而降低,与链结构无关,但是在两个阶段中,Lα相的下降速率均小于H(II)相的下降速率。还介绍了这些PE中Lα/ H(II)相变的详细分子描述。

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