液晶态磷脂酰乙醇胺脂质体和LB膜结构的研究

用原子力显微镜、小角X射线散射和³¹PNMR分别对液晶态磷脂酰乙醇胺脂质体和LB膜结构进行了研究.用原子力显微镜观察到了液晶态脂质体的立方相和双层膜共存的结构图像.研究结果表明,两相共存的状态与双亲性分子的结构、浓度以及介质的组分和pH等因素有关.用小角X射线散射和³¹PNMR研究发现,在DEPE液晶态中,钠盐诱导形成Q²²⁹(Im3m)立方相.DEPE液晶态分别在37.5℃出现L_β→L_α可逆相变,在63.5℃出现L_α→H_Ⅱ可逆相变.     

鞘磷脂和神经节苷脂对磷脂酰乙醇胺混合脂超分子体系液晶态立方相Im3m和Pn3m结构影响的研究

用磷脂酰乙醇胺(DEPE)、鞘磷脂(Sphingomyeline, Sph)、神经节苷脂(Gm1)和胆固醇(Chol)模拟了生物膜超分子体系液晶态结构, 通过用小角X射线衍射(SAXD)对混合脂体系液晶态结构进行了研究, 鉴定出了两种立方相: 即Im3m(Q²²⁹)和Pn3m(Q²²⁴)结构. 实验发现, 鞘磷脂的含量对DEPE膜的结构有一定的影响, 随着鞘磷脂浓度的增加, 混合脂体系的液晶态结构发生了由Im3m(Q²²⁹)到Pn3m(Q²²⁴)的变化. 神经节苷脂(Gm1)的含量对混合脂体系的液晶态结构也有一定的影响, 当神经节苷脂(Gm1)含量达到某一临界值时, 混合脂体系的液晶态结构发生了从Im3m(Q²²⁹)到Pn3m(Q²²⁴) 的变化. 当DEPE-Shp-Gm1超分子聚集体中含有胆固醇时, 胆固醇的极性头部(—OH)与磷脂酰乙醇胺(DEPE)、鞘磷脂(Shp)、神经节苷脂(Gm1)的极性头部通过氢键相互作用形成液晶态立方相Im3m(Q²²⁹)结构, 再通过疏水/亲水相互作用形成稳定的Pn3m (Q²²⁴)结构.     

脂双层膜表面结构与稳定性的原子力显微镜研究

用原子力显微镜研究了1,2－二油酸甘油－3－磷酸－1甘油（DOPG）脂双层膜 的表面结构与稳定性。实验结果表明,原子力显微镜的探针与脂双层膜的相互作用 导致脂双层膜表面产生一个永久的损伤。静电相互作用对脂双层膜结构和稳定性的 影响表明,在NaCl溶液中制成的脂质体,随着NaCl浓度的增加,它们的双层膜更稳 定。在低的NaCl浓度则经常被损伤,在1 mol/L NaCl溶液中制备的指双层变得更稳 定。在KCl溶液中结果恰好相反。在高的KCl浓度中经常被损伤,随着KCl浓度的降 低,它们的双层膜更稳定。葡萄糖和蔗糖对脂双层膜结构有稳定作用。     

改性中孔分子筛SBA-16薄膜的合成及表征

在酸性条件下, 以导电玻璃(ITO)为基底合成了SBA-16分子筛膜. 所制备的SBA-16膜孔径均匀, 具有体心立方结构(属于Im3m空间群), SBA-16膜的晶胞参数为18.6 nm. TEM, SEM和XRD等技术研究表明, 加入少量的AlCl₃盐于形成膜的母液并且采用RSiX₃对导电玻璃基底进行处理, 能够明显改善SBA-16膜的连续性而不影响孔结构. 红外(FTIR)研究结果表明, SBA-16膜的表面硅羟基和结晶水很少, 膜很稳定. XPS研究表明, 加入少量MnCl₂对SBA-16膜进行改性, 可以提高膜的导电性.     

DOPC,DOPE和神经酰胺对鞘磷脂/胆固醇双层膜结构的影响

用LB技术和原子力显微镜(AFM)研究了1,2-二油酸甘油-3-磷脂酰胆碱(DOPC)、1,2-二油酸甘油-3-磷脂酰乙醇胺(DOPE)和神经酰胺(Ceramide)对鞘磷脂(SM)/胆固醇(Chol)结构的影响. 实验结果表明, 在表面压力较低时, 每种混合脂双层膜都呈现均匀分布的脂双层结构. 随着表面压力的增加, 形态发生了明显的变化: (1) SM/Chol二元组分双层膜形成均一的液态有序相微区结构, 衬底覆盖率达到80%; (2) DOPC的加入促使SM/Chol双层膜出现相分离现象, SM/Chol形成的液态有序相 “岛状” 微区结构漂浮在液态无序相的DOPC上部, 约占总面积的30%; (3) DOPE与SM/Chol形成的双层膜明显不同于DOPC/SM/Chol, 呈现出液态无序相、液态有序相及凝胶相3相共存的结构; (4) Ceramide诱导了SM/Chol双层膜结构发生重排, 两层脂分子间发生翻转形成囊泡结构, 部分神经酰胺从液态有序相中分离形成小颗粒结构. 在较高膜压下, 各系统都呈现出具有特定形态的双层膜结构. 分子官能团的成键能力决定了双层膜形态结构.     

利用X射线衍射和拉曼光谱法对KCl和NaCl混合溶液微观结构的研究

利用X射线衍射法和拉曼光谱法系统研究了25 ℃下, 0-26%质量分数浓度范围内KCl和NaCl混合溶液的结构。通过分析X射线衍射法所得的混合溶液的差值结构函数F(Q)以及差值对分布函数G(r)发现,混合溶液组分中的K⁺的水化层半径及其水化数均大于Na⁺,从而揭示出常温下NaCl在水中的溶解度大于KCl的原因。在拉曼光谱的研究中,观察到溶液中水分子的四面体氢键受破坏程度随KCl浓度的增加和NaCl浓度的减少,先增大后减小,并结合X射线衍射法的结果,推断混合溶液中Na⁺对水溶液中氢键结构的破坏程度比K⁺严重,且加入适量的K⁺会使Na⁺由结构缔造者转变为打破结构者,对水溶液结构的破坏增强。     

巴比妥酸楔形棒状液晶分子的合成、性质及与三嗪衍生物的氢键识别组装体

合成了一端含巴比妥酸, 另一端含带三条烷基链苯甲酸酯楔形单元, 中间为苯乙烯共轭单元的棒状分子5-{4-[3,4,5-三(十二烷氧基)苯甲酸酯]苯乙烯}-(1H,3H)-2,4,6嘧啶三酮(BA³/12); 采用偏光显微镜(POM)、 示差扫描量热法(DSC)、 X射线衍射(XRD)、 扫描电子显微镜(SEM)、 红外光谱(IR)、 核磁共振波谱(NMR)和荧光光谱等对其进行了表征. 结果表明, BA³/12能自组装形成晶格结构为c2mm的长方柱相液晶; 红外光谱及核磁共振氢谱表征数据初步证实了BA³/12与三嗪化合物6-(5-{4-[3,4-双(十二烷氧基)]苄氧基}苯基)噻吩-2,4-二氨基-1,3,5三嗪(1T²/12)形成的等摩尔氢键复合物BA/T的结构; BA/T不仅具有液晶性质且能形成具有三维网络状结构的超分子凝胶.     

Cs(ATZ)的制备、晶体结构与热力学性质

以5-氨基四唑(ATZ)和氢氧化铯溶液为原料, 制备了配合物Cs(ATZ)并培养出单晶, 结构由X-ray单晶衍射测定. 晶体属正交晶系, 空间群Pnma, 晶体学参数: a＝0.8114(4) nm, b＝0.6907(4) nm, c＝0.9122(5) nm, V＝0.5113(5) nm³, D_c＝2.819 g/cm³, Z＝4, F(000)＝392, m＝7.112 mm^－1, R＝0.0485. 其中Cs^＋与9个氮原子配位, 分子间通过氢键、金属离子与N原子的桥连接及分子间作用力, 形成三维结构, 增加了晶体结构的稳定性. 同时, 用红外、拉曼光谱对配合物进行了表征. 根据测得的ATZ及Cs(ATZ)在氢氧化铯溶液中的反应焓和溶解焓, 算得配合物Cs(ATZ)标准摩尔生成焓为 (－430.56±0.43) kJ•mol^－1.     

AlmN和AlmN+(m=2～9)团簇结构与稳定性的量子化学研究

用密度泛函理论(DFT)的B3LYP方法,在6-311G^*水平上对Al_mN和Al_mN⁺(m=2～9)团簇的几何构型、电子结构、振动频率等性质进行了理论研究,给出了以Al_m团簇作为设计Al_mN类结构的母体,考虑在不同位置上结合N原子的结构,可以较快找到Al_mN类团簇基态结构的一种方法.通过对基态结构的离解能和能量二次差分讨论,得到m为奇数的Al_mN团簇比m为偶数的稳定.对基态结构的绝热电离能讨论结果表明,只存在Al-N键的Al2N和Al3N团簇较稳定.     

脂筏微区超分子聚集体结构的稳定性

生物膜中脂筏微区结构的动态特征与稳定性决定着生物膜的功能。通过从动物细胞提取脂筏,实验不但观测到质膜微囊烧瓶状凹陷结构,而且还观测到大量的球状和椭球状结构.通过模拟脂筏微区结构,重点对二元体系和三元体系的超分子聚集体结构的多形性进行了研究和探索。研究发现随着表面压力的增加,鞘磷脂和胆固醇双层膜出现了紧密聚集不规则的微区结构,在 SM/Chol/DOPC双层膜中,SM/Chol形成的微区结构漂浮在液态DOPC小颗粒上部。当 DOPE加入到SM/Chol中,三种成份形成不稳定的双层膜结构.Ceramide促进了SM/Chol结构发生重排,微区形状从原来的不规则向着紧密聚集的圆形结构演变;混合单层膜的分子面积与表面吉布斯自由能决定了分子间的相互作用, 当过量分子面积与过量吉布斯自由能为负值时,分子间相互作用表现为吸引力, 出现凝聚现象; 为正值时,分子间相互作用表现为排斥力, 促使单层膜出现相分离现象. 过量吉布斯自由能值越小, 单层膜的热稳定性越高.通过动物细胞提取脂筏与体外模拟脂筏相结合的方法,从超分子水平阐述了脂筏微区结构与功能的生物学意义,为生物膜的研究提供了理论依据和实验支持。     

Study of liquid crystal space groups using controlled tilting with cryogenic transmission electron microscopy

We developed a method that enables differentiation between liquid crystalline-phase particles corresponding to different space groups. It consists of controlled tilting of the specimen to observe different orientations of the same particle using cryogenic transmission electron microscopy. This leads to the visualization of lattice planes (or reflections) that are present for a given structure and absent for the other one(s) and that give information on liquid crystalline structures and their space groups. In particular, we show that we can unambiguously distinguish among particles having the inverted micellar cubic (space group Fd(3)m, 227), the inverted bicontinuous gyroid (space group Ia(3)d, 230), the inverted bicontinuous diamond (space group Pn(3)m, 224), and the inverted bicontinuous primitive cubic structure (space group Im(3)m, 229).     

Formation of cubic phases from large unilamellar vesicles of dioleoylphosphatidylglycerol/monoolein membranes induced by low concentrations of Ca2+

We developed a new method for the transformation of large unilamellar vesicles (LUVs) into the cubic phase. We found that the addition of low concentrations of Ca(2+) to suspensions of multilamellar vesicles (MLVs) of membranes of monoolein (MO) and dioleoylphosphatidylglycerol (DOPG) mixtures (DOPG/MO) changed their L(alpha) phase to the cubic phases. For instance, the addition of 15-25 mM Ca(2+) to 30%-DOPG/70%-MO-MLVs induced the Q(229) phase, whereas the addition of > or =28 mM Ca(2+) induced the Q(224) phase. LUVs of DOPG/MO membranes containing > or =25 mol % DOPG were prepared easily. Low concentrations of Ca(2+) transformed these LUVs in excess buffer into the Q(224) or the Q(229) phase, depending on the Ca(2+) concentration. For example, 15 and 50 mM Ca(2+) induced the Q(224) and Q(229) phase in the 30%-DOPG/70%-MO-LUVs at 25 degrees C, respectively. This finding is the first demonstration of transformation of LUVs of lipid membranes into the cubic phase under excess water condition.     

Bulk and dispersed aqueous phase behavior of phytantriol: effect of vitamin E acetate and F127 polymer on liquid crystal nanostructure

Phytantriol (3,7,11,15-tetramethylhexadecane-1,2,3-triol, PHYT) is a cosmetic ingredient that exhibits similar lyotropic phase behavior to monoolein (GMO), forming bicontinuous cubic liquid crystalline structures (Q(II)) at low temperatures and reversed hexagonal phase (H(II)) at higher temperatures in excess water. Despite these similarities, phytantriol has received little attention in the scientific community. In this study, the thermal phase behavior of the binary PHYT-water and ternary PHYT-vitamin E acetate (VitEA)-water systems have been studied and compared with the behavior of the dispersed cubosomes and hexosomes formed with the aid of a stabilizer (Pluronic F127). The phase behavior and nanostructure were studied using crossed polarized light microscopy (CPLM), differential scanning calorimetry (DSC), and small-angle X-ray scattering (SAXS) techniques. The presence of lipophilic VitEA in the PHYT-water system suppressed the temperature of the Q(II)-to-H(II)-to-L2 transitions, indicating that lipophilic compounds, in relatively small amounts, may have a significant impact on the phase behavior. Increasing the F127 concentration in the phytantriol-based cubosome system did not induce the Q(II)(Pn3m) to Q(II)(Im3m) transition known for the GMO-water system. This indicates a different mode of interaction between F127 and the lipid domains of phytantriol-water systems. Taken together, these results indicate that phytantriol may not only provide an alternative lipid for preparation of liquid crystalline systems in excess water but may also provide access to properties not available when using GMO.     

Metal cation induced cubic phase in poly(ethylene glycol)-functionalized dioleoylphosphatidylethanolamine aqueous dispersions

Metal cations (Mn(2+) or Ca(2+)) in aqueous dispersions of mixtures of dioleoylphosphatidylethanolamine (DOPE) and poly(ethylene glycol)-functionalized DOPE (DOPE-PEG(350)) induce, above a certain amount of the PEG lipid component, a phase transition from the inverted hexagonal phase H(II) to the bicontinuous inverted cubic phase Q(224) with space group Pn3m. The process is driven by the decrease of free elastic energy due to the Gaussian curvature of the cubic phase. The structural characterization of the phase behavior over the whole explored range of DOPE-PEG/DOPE weight ratio (3-25%) is reported, focusing on the role of the metal cation in the formation of the 3D cubic lattice. This result may represent a significant progress toward a design-based approach to drug delivery.     

Control of the internal structure of MLO-based isasomes by the addition of diglycerol monooleate and soybean phosphatidylcholine

This work describes the effect of two different surfactants on the internal nanostructure of the kinetically stabilized isasomes (internally self-assembled particles or "somes"), which are a new family of colloidal particles (cubosomes, hexosomes, micellar cubosomes, and emulsified microemulsions, EME). The stabilization of these systems is performed by using the polymeric stabilizer F127. We demonstrate that the internal structure of these oil-free and oil-loaded dispersed particles can be modulated by varying the lipid composition. To achieve this goal, we replaced part of our primary lipid monolinolein (MLO) with diglycerol monooleate (DGMO) or soybean phosphatidylcholine (PC). We found that DGMO has a counter effect to that of tetradecane (TC) and allows us to tune back the self-assembled nanostructure in the TC-loaded dispersions from H2 (hexosomes) to Im3m (cubosomes). Although TC has a higher impact on confined structures than does DGMO, we demonstrate that the addition of DGMO significantly affects the internal structure of the TC-solubilized dispersions and favors the formation of large water channels. PC can also be used to modify the internal structure for MLO-based systems. It is somehow different from DGMO due to the fact that the fully hydrated Pn3m cubic structure in the presence of PC for the TC-free dispersion is preserved after dispersing. The results also indicate that PC is less effective than DGMO for tuning back the TC-loaded internal structure from H2 to cubic phase, in which it makes the confined structure less ordered. In addition, we found that DGMO has a significant effect on the internal structure of isasomes. It increases the water solubilization capacity for dispersed and nondispersed bulk phases. In contrast to the MLO-based dispersions, the present results indicate that F127 plays an important role in the internal structure of these dispersions due to its penetration into the oil-free cubic phase changing the symmetry from Pn3m to Im3m.     

Horse heart cytochrome c entrapped into the hydrated liquid-crystalline phases of phytantriol: X-ray diffraction and Raman spectroscopic characterization

Small angle X-ray diffraction (SAXD), resonance Raman (RR) spectroscopy with 413 nm excitation, and non-resonance Raman technique with 785 nm excitation were used to probe the influence of entrapped cytochrome c (Cyt c) on the structure of hydrated phytantriol (Phyt) liquid-crystalline phases as well as conformational changes of heme group and secondary structure of the protein. SAXD measurements indicated that incorporation of Cyt c affects both nanostructure dimensions and type of liquid-crystalline phases of hydrated Phyt. The unit cell dimensions decrease with increasing Cyt c concentration for all phases. In addition, protein perturbs the nanostructure of Q(230) and Q(224) liquid-crystalline phases of hydrated Phyt to such an extent that they transform into the Q(229) phase with the Im3m space group. RR data revealed that entrapment of oxidized Cyt c into the Q(230) phase at 1 wt.% content results in near complete reduction of central iron ion of the heme group, while its low-spin state and six-ligand coordination configuration are preserved. Based on the analysis of heme out-of-plane folding vibration near 568 cm(-1) (γ(21)) and ν(48) mode at 633 cm(-1), it was demonstrated that the protein matrix tension on the heme group is relaxed upon incorporation of protein into Q(230) phase. Non-resonant Raman bands of difference spectra showed the preservation of α-helix secondary structure of Cyt c in the liquid-crystalline phase at relatively high (5 wt.%) content. The Cyt c induced spectroscopic changes of Phyt bands were found to be similar as decrease in temperature.