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气体中离子迁移的分子动力学模拟。

Molecular dynamics simulation of ion mobility in gases.

机构信息

Department of Chemistry, Nebraska Center for Materials and Nanoscience, and Center for Integrated Biomolecular Communication, University of Nebraska-Lincoln, Lincoln, Nebraska 68588, USA.

Department of Chemistry and Center for Integrated Biomolecular Communication, University of Nebraska-Lincoln, Lincoln, Nebraska 68588, USA.

出版信息

J Chem Phys. 2018 Feb 14;148(6):064109. doi: 10.1063/1.4998955.

Abstract

A force field molecular dynamics method is developed to directly simulate ion drift in buffer gases driven by an electric field. The ion mobility and collision cross sections (CCSs) with relevance to ion mobility spectrometry can be obtained from the simulated drift velocity in high-density buffer gases (pressure ∼50 bars) and high electric fields (∼10 V/m). Compared to trajectory methods, the advantage of the molecular dynamics method is that it can simultaneously sample the internal dynamic motions of the ion and the ion-gas collisions. For ions with less than 100 atoms, the simulated collision cross section values can be converged to within ±1%-2% by running a 100 ns simulation for 5-19 h using one computer core. By using a set of element-based Lennard-Jones parameters that are not tuned for different atomic types in different molecules, the simulated collision cross sections for 15 small molecular ions (number of atoms ranging from 17 to 85, mass ranging from 74.1 to 609.4 g/mol) are consistent with experimental values: the mean unsigned error is 2.6 Å for He buffer gas and 4.4 Å for N buffer gas. The sensitivity of the simulated CCS values to random diffusion, drift velocity, electric field strength, temperature, and buffer gas density is examined.

摘要

一种力场分子动力学方法被开发出来,用于直接模拟电场驱动下的缓冲气体中的离子漂移。通过在高密度缓冲气体(压力约为 50 巴)和高电场(约 10 V/m)中模拟的漂移速度,可以获得与离子迁移谱相关的离子迁移率和碰撞截面(CCS)。与轨迹方法相比,分子动力学方法的优势在于它可以同时采样离子的内部动态运动和离子-气体碰撞。对于原子数小于 100 的离子,通过在一个计算机核心上运行 5-19 小时的 100 ns 模拟,可以将模拟的碰撞截面值收敛到±1%-2%以内。通过使用一组不针对不同分子中不同原子类型进行调整的基于元素的 Lennard-Jones 参数,我们模拟的 15 种小分子离子(原子数从 17 到 85 不等,质量从 74.1 到 609.4 g/mol)的碰撞截面与实验值一致:氦缓冲气体的平均无符号误差为 2.6 Å,氮缓冲气体的平均无符号误差为 4.4 Å。模拟的 CCS 值对随机扩散、漂移速度、电场强度、温度和缓冲气体密度的灵敏度进行了检验。

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