Meirovitch E, Meirovitch H
Supercomputer Computations Research Institute, Florida State University, Tallahassee 32306-4052, USA.
Biopolymers. 1996 Jan;38(1):69-88. doi: 10.1002/(sici)1097-0282(199601)38:1<69::aid-bip6>3.0.co;2-u.
A small linear peptide in solution may populate several stable states (called here microstates) in thermodynamic equilibrium; elucidating its dynamic three dimensional structure by multi- dimensional nmr is complex since the experimentally measured nuclear Overhauser effect intensities (NOEs) represent averages over the individual contributions. We propose a new methodology based on statistical mechanical considerations for analyzing nmr data of such peptides. In a previous paper (called paper I, H. Meirovitch et al. (1995) Journal of Physical Chemistry, 99, 4847-4854] we have developed theoretical methods for determining the contribution to the partition function Z of the most stable microstates, i.e. those that pertain to a given energy range above the global energy minimum (GEM). This relatively small set of dominant microstates provides the main contribution to medium- and long-range NOE intensities. In this work the individual populations and NOEs of the dominant microstates are determined, and then weighted averages are calculated and compared with experiment. Our methodology is applied to the pentapeptide Leu-enkephalin H-Tyr-Gly-Gly-Phe-Leu-OH, described by the potential energy function ECEPP. Twenty one significantly different energy minimized structures are first identified within the range of 2 kcal/mol above the GEM by an extensive conformational search; this range has been found in paper I to contribute 0.6 of Z. These structures then become "seeds" for Monte Carlo (MC) simulations designed to keep the molecule relatively close to its seed. Indeed, the MC samples (called MC microstates) illustrate what we define as intermediate chain flexibility; some dihedral angles remain in the vicinity of their seed value, while others visit the full range of [-180 degrees, 180 degrees]. The free energies of the MC microstates (which lead to the populations) are calculated by the local states method, which (unlike other techniques) can handle any chain flexibility. The NOE of MC microstate i is calculated as the average <1/r(3)>i(2), and an effective interatomic distance ri(eff) is defined as ri(eff) = <l/r(3)>i(-1/3), where r is the distance between two protons. Under "initial rate approximation," and neglecting angular modulations, the overall I is the average over ri(eff-6), weighted by the populations of the MC microstates. This treatment is justified under the assumption that the rates at which conformations interconvert within, and among, microstates are faster and slower, respectively, than the rotational reorientation of the molecule. I(-6) leads to the virtual theoretical distances, compared to the corresponding virtual experimental distances, which were obtained previously from a cryoprotective solution of Leu-enkephalin at 280 K. A reasonable fit is found between theory and experiment. Future research directions are outlined.
溶液中的小线性肽在热力学平衡状态下可能存在几种稳定状态(这里称为微状态);通过多维核磁共振阐明其动态三维结构很复杂,因为实验测量的核Overhauser效应强度(NOE)代表了各个贡献的平均值。我们提出了一种基于统计力学考虑的新方法来分析此类肽的核磁共振数据。在之前的一篇论文(称为论文I,H. Meirovitch等人(1995年)《物理化学杂志》,99卷,4847 - 4854页)中,我们已经开发了理论方法来确定对最稳定微状态的配分函数Z的贡献,即那些与全局能量最小值(GEM)之上给定能量范围相关的微状态。这一相对较小的一组主导微状态对中程和远程NOE强度提供了主要贡献。在这项工作中,确定了主导微状态的各个布居和NOE,然后计算加权平均值并与实验进行比较。我们的方法应用于由势能函数ECEPP描述的五肽亮氨酸脑啡肽H - Tyr - Gly - Gly - Phe - Leu - OH。首先通过广泛的构象搜索在高于GEM 2千卡/摩尔的范围内识别出21种显著不同的能量最小化结构;在论文I中发现这个范围对Z的贡献为0.6。这些结构随后成为蒙特卡罗(MC)模拟的“种子”,旨在使分子相对接近其种子结构。实际上,MC样本(称为MC微状态)说明了我们所定义的中间链柔性;一些二面角保持在其种子值附近,而其他二面角则遍历[-180度,180度]的整个范围。MC微状态的自由能(导致布居)通过局部状态方法计算,该方法(与其他技术不同)可以处理任何链柔性。MC微状态i的NOE计算为平均<1/r(3)>i(2),并且有效原子间距离ri(eff)定义为ri(eff) = <l/r(3)>i(-1/3),其中r是两个质子之间的距离。在“初始速率近似”下,忽略角度调制,总体I是ri(eff - 6)的平均值,由MC微状态的布居加权。在构象在微状态内和微状态间相互转换的速率分别比分子的旋转重取向快和慢的假设下,这种处理是合理的。I(-6)导致虚拟理论距离,与之前从280 K下亮氨酸脑啡肽的冷冻保护溶液中获得的相应虚拟实验距离进行比较。在理论和实验之间发现了合理的拟合。概述了未来的研究方向。