Leal Cecília, Rögnvaldsson Sibylla, Fossheim Sigrid, Nilssen Esben A, Topgaard Daniel
Radiation Biology, Norwegian Radium Hospital, Montebello N-0310 Oslo, Norway.
J Colloid Interface Sci. 2008 Sep 15;325(2):485-93. doi: 10.1016/j.jcis.2008.05.051. Epub 2008 Jun 3.
Proton-detected NMR diffusion and (31)P NMR chemical shifts/bandwidths measurements were used to investigate a series of liposomal formulations where size and PEGylation extent need to be controlled for ultrasound mediated drug release. The width of the (31)P line is sensitive to aggregate size and shape and self-diffusion (1)H NMR conveys information about diffusional motion, size, and PEGylation extent. Measurements were performed on the formulations at their original pH, osmolality, and lipid concentration. These contained variable amounts of PEGylated phospholipid (herein referred to as PEG-lipid) and cholesterol. At high levels of PEG-lipid (11.5 and 15 mol%) the self-diffusion (1)H NMR revealed the coexistence of two entities with distinct diffusion coefficients: micelles (1.3 to 3x10(-11) m(2)/s) and liposomes (approximately 5x10(-12) m(2)/s). The (31)P spectra showed a broad liposome signal and two distinct narrow lines that were unaffected by temperature. The narrow lines arise from mixed micelles comprising both PEG-lipids and phospholipids. The echo decay in the diffusion experiments could be described as a sum of exponentials revealing that the exchange of PEG-lipid between liposomes and micellar aggregates is slower than the experimental observation time. For low amounts of PEG-lipid (1 and 4.5 mol%) the (31)P spectra consisted of a broad signal typically obtained for liposomes and the diffusion data were best described by a single exponential decay attributed solely to liposomes. For intermediate amounts of PEG-lipid (8 mol%), micellization started to occur and the diffusion data could no longer be fitted to a single or bi-exponential decay. Instead, the data were best described by a log-normal distribution of diffusion coefficients. The most efficient PEG-lipid incorporation in liposomes (about 8 mol%) was achieved for lower molecular weight PEG (2000 Da vs 5000 Da) and when the PEG-lipid acyl chain length matched the acyl chain length of the liposomal core phospholipid. Simultaneously to the PEGylation extent, self-diffusion (1)H NMR provides information about the size of micelles and liposomes. The size of the micellar aggregates decreased as the PEG-lipid content was increased while the liposome size remained invariant.
质子检测核磁共振扩散以及(31)P核磁共振化学位移/带宽测量被用于研究一系列脂质体制剂,在超声介导的药物释放中,这些制剂的大小和聚乙二醇化程度需要得到控制。(31)P谱线的宽度对聚集体大小和形状敏感,而自扩散(1)H核磁共振传达了有关扩散运动、大小和聚乙二醇化程度的信息。在制剂的原始pH值、渗透压和脂质浓度下进行测量。这些制剂含有不同量的聚乙二醇化磷脂(在此称为聚乙二醇脂质)和胆固醇。在高含量的聚乙二醇脂质(11.5和15摩尔%)时,自扩散(1)H核磁共振显示存在两种具有不同扩散系数的实体共存:胶束(1.3至3×10(-11)平方米/秒)和脂质体(约5×10(-12)平方米/秒)。(31)P谱显示出一个宽的脂质体信号以及两条不受温度影响的明显窄线。窄线来自包含聚乙二醇脂质和磷脂的混合胶束。扩散实验中的回波衰减可以描述为指数之和,这表明脂质体和胶束聚集体之间聚乙二醇脂质的交换比实验观察时间慢。对于低含量的聚乙二醇脂质(1和4.5摩尔%),(31)P谱由通常在脂质体中获得的宽信号组成,扩散数据最好用仅归因于脂质体的单指数衰减来描述。对于中等含量的聚乙二醇脂质(8摩尔%),开始发生胶束化,扩散数据不再能拟合为单指数或双指数衰减。相反,数据最好用扩散系数的对数正态分布来描述。对于较低分子量的聚乙二醇(2000道尔顿对5000道尔顿)以及当聚乙二醇脂质酰基链长度与脂质体核心磷脂的酰基链长度匹配时,脂质体中实现了最有效的聚乙二醇脂质掺入。与聚乙二醇化程度同时,自扩散(1)H核磁共振提供了有关胶束和脂质体大小的信息。随着聚乙二醇脂质含量增加,胶束聚集体的大小减小,而脂质体大小保持不变。