Bagatolli L A, Gratton E
Laboratory for Fluorescence Dynamics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801-3080, USA.
Biophys J. 2000 Jul;79(1):434-47. doi: 10.1016/S0006-3495(00)76305-3.
Giant unilamellar vesicles (GUVs) composed of different phospholipid binary mixtures were studied at different temperatures, by a method combining the sectioning capability of the two-photon excitation fluorescence microscope and the partition and spectral properties of 6-dodecanoyl-2-dimethylamino-naphthalene (Laurdan) and Lissamine rhodamine B 1,2-dihexadecanoyl-sn-glycero-3-phosphoethanolamine (N-Rh-DPPE). We analyzed and compared fluorescence images of GUVs composed of 1,2-dilauroyl-sn-glycero-3-phosphocholine/1, 2-dipalmitoyl-sn-glycero-3-phosphocholine (DLPC/DPPC), 1, 2-dilauroyl-sn-glycero-3-phosphocholine/1, 2-distearoyl-sn-glycero-3-phosphocholine (DLPC/DSPC), 1, 2-dilauroyl-sn-glycero-3-phosphocholine/1, 2-diarachidoyl-sn-glycero-3-phosphocholine (DLPC/DAPC), 1, 2-dimyristoyl-sn-glycero-3-phosphocholine/1, 2-distearoyl-sn-glycero-3-phosphocholine (DMPC/DSPC) (1:1 mol/mol in all cases), and 1,2-dimyristoyl-sn-glycero-3-phosphoethanolamine/1, 2-dimyristoyl-sn-glycero-3-phosphocholine (DMPE/DMPC) (7:3 mol/mol) at temperatures corresponding to the fluid phase and the fluid-solid phase coexistence. In addition, we studied the solid-solid temperature regime for the DMPC/DSPC and DMPE/DMPC mixtures. From the Laurdan intensity images the generalized polarization function (GP) was calculated at different temperatures to characterize the phase state of the lipid domains. We found a homogeneous fluorescence distribution in the GUV images at temperatures corresponding to the fluid region for all of the lipid mixtures. At temperatures corresponding to phase coexistence we observed concurrent fluid and solid domains in the GUVs independent of the lipid mixture. In all cases the lipid solid domains expanded and migrated around the vesicle surface as we decreased the temperature. The migration of the solid domains decreased dramatically at temperatures close to the solid-fluid-->solid phase transition. For the DLPC-containing mixtures, the solid domains showed line, quasicircular, and dendritic shapes as the difference in the hydrophobic chain length between the components of the binary mixture increases. In addition, for the saturated PC-containing mixtures, we found a linear relationship between the GP values for the fluid and solid domains and the difference between the hydrophobic chain length of the binary mixture components. Specifically, at the phase coexistence temperature region the difference in the GP values, associated with the fluid and solid domains, increases as the difference in the chain length of the binary mixture component increases. This last finding suggests that in the solid-phase domains, the local concentration of the low melting temperature phospholipid component increases as the hydrophobic mismatch decreases. At the phase coexistence temperature regime and based on the Laurdan GP data, we observe that when the hydrophobic mismatch is 8 (DLPC/DAPC), the concentration of the low melting temperature phospholipid component in the solid domains is negligible. This last observation extends to the saturated PE/PC mixtures at the phase coexistence temperature range. For the DMPC/DSPC we found that the nonfluorescent solid regions gradually disappear in the solid temperature regime of the phase diagram, suggesting lipid miscibility. This last result is in contrast with that found for DMPE/DMPC mixtures, where the solid domains remain on the GUV surface at temperatures corresponding to that of the solid region. In all cases the solid domains span the inner and outer leaflets of the membrane, suggesting a strong coupling between the inner and outer monolayers of the lipid membrane. This last finding extends previous observations of GUVs composed of DPPE/DPPC and DLPC/DPPC mixtures (, Biophys. J. 78:290-305).
采用双光子激发荧光显微镜的切片能力与6 - 十二烷酰基 - 2 - 二甲基氨基萘(Laurdan)以及丽丝胺罗丹明B 1,2 - 二己酰基 - sn - 甘油 - 3 - 磷酸乙醇胺(N - Rh - DPPE)的分配和光谱特性相结合的方法,研究了由不同磷脂二元混合物组成的巨型单层囊泡(GUVs)在不同温度下的情况。我们分析并比较了由1,2 - 二月桂酰 - sn - 甘油 - 3 - 磷酸胆碱/1,2 - 二棕榈酰 - sn - 甘油 - 3 - 磷酸胆碱(DLPC/DPPC)、1,2 - 二月桂酰 - sn - 甘油 - 3 - 磷酸胆碱/1,2 - 二硬脂酰 - sn - 甘油 - 3 - 磷酸胆碱(DLPC/DSPC)、1,2 - 二月桂酰 - sn - 甘油 - 3 - 磷酸胆碱/1,2 - 二花生四烯酰 - sn - 甘油 - 3 - 磷酸胆碱(DLPC/DAPC)、1,2 - 二肉豆蔻酰 - sn - 甘油 - 3 - 磷酸胆碱/1,2 - 二硬脂酰 - sn - 甘油 - 3 - 磷酸胆碱(DMPC/DSPC)(所有情况下均为1:1摩尔/摩尔)以及1,2 - 二肉豆蔻酰 - sn - 甘油 - 3 - 磷酸乙醇胺/1,2 - 二肉豆蔻酰 - sn - 甘油 - 3 - 磷酸胆碱(DMPE/DMPC)(7:3摩尔/摩尔)组成的GUVs在对应于流体相和流体 - 固相共存的温度下的荧光图像。此外,我们研究了DMPC/DSPC和DMPE/DMPC混合物的固 - 固温度范围。从Laurdan强度图像计算出不同温度下的广义极化函数(GP),以表征脂质域的相态。我们发现,在对应于所有脂质混合物流体区域的温度下,GUV图像中荧光分布均匀。在对应于相共存的温度下,我们在GUVs中观察到同时存在的流体和固体域,且与脂质混合物无关。在所有情况下,随着温度降低,脂质固体域在囊泡表面扩展并迁移。在接近固 - 液→固相转变的温度下,固体域的迁移显著降低。对于含DLPC的混合物,随着二元混合物组分疏水链长度差异的增加,固体域呈现出线状、准圆形和树枝状形状。此外,对于含饱和PC的混合物,我们发现流体和固体域的GP值与二元混合物组分疏水链长度差异之间存在线性关系。具体而言,在相共存温度区域,与流体和固体域相关的GP值差异随着二元混合物组分链长度差异的增加而增加。这一最新发现表明,在固相域中,低熔点温度磷脂组分的局部浓度随着疏水错配的减小而增加。在相共存温度范围并基于Laurdan GP数据时,我们观察到当疏水错配为8(DLPC/DAPC)时,固相域中低熔点温度磷脂组分的浓度可忽略不计。这一最新观察结果扩展到相共存温度范围内的饱和PE/PC混合物。对于DMPC/DSPC,我们发现在相图的固体温度范围内,非荧光固体区域逐渐消失,表明脂质互溶性。这一最新结果与DMPE/DMPC混合物的情况形成对比,在对应于固体区域温度的情况下,DMPE/DMPC混合物的固体域保留在GUV表面。在所有情况下,固体域跨越膜的内叶和外叶,表明脂质膜的内单层和外单层之间存在强耦合。这一最新发现扩展了先前对由DPPE/DPPC和DLPC/DPPC混合物组成的GUVs的观察结果(《生物物理学杂志》78:290 - 305)。