Venable Richard M, Sodt Alexander J, Rogaski Brent, Rui Huan, Hatcher Elizabeth, MacKerell Alexander D, Pastor Richard W, Klauda Jeffery B
Laboratory of Computational Biology, National Heart, Lung, and Blood Institute, National Institutes of Health, Bethesda, Maryland.
Department of Chemical and Biomolecular Engineering, University of Maryland, College Park, Maryland.
Biophys J. 2014 Jul 1;107(1):134-45. doi: 10.1016/j.bpj.2014.05.034.
The C36 CHARMM lipid force field has been extended to include sphingolipids, via a combination of high-level quantum mechanical calculations on small molecule fragments, and validation by extensive molecular dynamics simulations on N-palmitoyl and N-stearoyl sphingomyelin. NMR data on these two molecules from several studies in bilayers and micelles played a strong role in the development and testing of the force field parameters. Most previous force fields for sphingomyelins were developed before the availability of the detailed NMR data and relied on x-ray diffraction of bilayers alone for the validation; these are shown to be too dense in the bilayer plane based on published chain order parameter data from simulations and experiments. The present simulations reveal O-H:::O-P intralipid hydrogen bonding occurs 99% of the time, and interlipid N-H:::O=C (26-29%, depending on the lipid) and N-H:::O-H (17-19%). The interlipid hydrogen bonds are long lived, showing decay times of 50 ns, and forming strings of lipids, and leading to reorientational correlation time of nearly 100 ns. The spontaneous radius of curvature for pure N-palmitoyl sphingomyelin bilayers is estimated to be 43-100 Å, depending on the assumptions made in assigning a bending constant; this unusual positive curvature for a two-tailed neutral lipid is likely associated with hydrogen bond networks involving the NH of the sphingosine group.
C36 CHARMM脂质力场已通过对小分子片段进行高水平量子力学计算,并结合对N-棕榈酰鞘磷脂和N-硬脂酰鞘磷脂进行广泛的分子动力学模拟进行验证,从而扩展到包括鞘脂。来自双层和胶束中多项研究的这两种分子的核磁共振数据在力场参数的开发和测试中发挥了重要作用。以前大多数针对鞘磷脂的力场是在详细的核磁共振数据可用之前开发的,仅依靠双层的X射线衍射进行验证;根据已发表的模拟和实验中的链序参数数据,这些力场在双层平面中显示过于密集。目前的模拟显示,脂质内的O-H:::O-P氢键在99%的时间内发生,脂质间的N-H:::O=C(26-29%,取决于脂质)和N-H:::O-H(17-19%)。脂质间的氢键寿命很长,衰减时间为50纳秒,并形成脂质链,导致重排相关时间接近100纳秒。根据在指定弯曲常数时所做的假设,纯N-棕榈酰鞘磷脂双层的自发曲率半径估计为43-100埃;这种两亲性中性脂质不寻常的正曲率可能与涉及鞘氨醇基团NH的氢键网络有关。