Blume A, Griffin R G
Biochemistry. 1982 Nov 23;21(24):6230-42. doi: 10.1021/bi00267a031.
Mixtures of dipalmitoylphosphatidylethanolamine (DPPE) and cholesterol (CHOL) have been studied with solid-state 13C and 2H nuclear magnetic resonance (NMR) techniques. DPPE was 13C labeled at the carbonyl group of the sn-2 chain, and 2H was introduced at the 4 position of the sn-2 chain and the 1 position of the ethanolamine head group. The 13C and 2H spectra of each labeled lipid were studied as a function of temperature and CHOL concentration, and the results indicate three distinguishable temperature-composition regions. In region I, which occurs at low temperatures and CHOL concentrations, the 13C and 2H spectra are similar to those observed for pure DPPE in its gel phase. In region II, which occurs at higher temperatures or CHOL concentrations, the sn-2 13C = O spectra of DPPE/CHOL mixtures display two components, indicating the coexistence of two conformationally and dynamically inequivalent DPPE molecules. One of these is similar to gel-state DPPE, while the second "fluid" fraction displays some liquid-crystalline character. The two-component 13C spectra can be simulated quantitatively with a two-parameter chemical exchange model that permits the fraction of each form and the exchange rate to be determined as a function of temperature and composition. The 2H spectra observed in region II do not exhibit two components in an obvious way. Nevertheless, with some reasonable assumptions, the 2H spectra obtained from chain-labeled DPPE can also be simulated with a two-component model with the exchange rates and fractional populations obtained from the 13C results. The calculations predict not only the line shapes but also the losses in spectral intensity arising from use of the quadrupole echo technique. Furthermore, the 2H spectra show that with increasing temperature the fluid fraction observed in region II undergoes a transition to a higher degree of disorder, and should therefore not be labeled "liquid crystalline". In region III, which occurs at high temperatures and CHOL concentrations, both the 13C and 2H spectra are those expected of liquid-crystalline lipid. The NMR results are compared to, and found to be different from, those obtained with calorimetric investigations. It is suggested that these differences are due to the small domains present in DPPE/CHOL mixtures that lead to phase transitions of low cooperativity. Some metastability of the DPPE/CHOL system was observed at high CHOL concentrations and low temperatures.
已使用固态碳-13和氢-2核磁共振(NMR)技术研究了二棕榈酰磷脂酰乙醇胺(DPPE)与胆固醇(CHOL)的混合物。DPPE在sn-2链的羰基处进行了碳-13标记,氢-2被引入到sn-2链的4位和乙醇胺头部基团的1位。研究了每种标记脂质的碳-13和氢-2光谱随温度和CHOL浓度的变化,结果表明存在三个可区分的温度-组成区域。在区域I中,该区域出现在低温和低CHOL浓度下,碳-13和氢-2光谱与在凝胶相中的纯DPPE所观察到的光谱相似。在区域II中,该区域出现在较高温度或较高CHOL浓度下,DPPE/CHOL混合物的sn-2碳-13=O光谱显示出两个成分,表明存在两种构象和动力学上不等价的DPPE分子。其中一种类似于凝胶态DPPE,而第二种“流体”部分表现出一些液晶特性。双成分碳-13光谱可以用一个双参数化学交换模型进行定量模拟,该模型允许确定每种形式的比例和交换率随温度和组成的变化。在区域II中观察到的氢-2光谱并没有明显地表现出两个成分。然而,在一些合理的假设下,从链标记的DPPE获得的氢-2光谱也可以用一个双成分模型进行模拟,其交换率和分数丰度从碳-13结果中获得。这些计算不仅预测了线形,还预测了由于使用四极回波技术而导致的光谱强度损失。此外,氢-2光谱表明,随着温度升高,在区域II中观察到的流体部分会转变为更高程度的无序状态,因此不应被标记为“液晶”。在区域III中,该区域出现在高温和高CHOL浓度下,碳-13和氢-2光谱都是液晶脂质所预期的光谱。将NMR结果与量热研究结果进行了比较,发现两者不同。有人认为,这些差异是由于DPPE/CHOL混合物中存在的小区域导致低协同性的相变。在高CHOL浓度和低温下观察到了DPPE/CHOL系统的一些亚稳性。