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各位老师,最近我发了一篇有关结合Gromacs研究液体结构的文章,审稿人对gromacs模拟部分提的意见很尖锐,但由于这是我的第一篇有关Gromacs的文章,有些意见我真不知道怎么改进,请各位老师指导改进谢谢。
审稿人给的意见如下:
I am unable to recommend the present work on"***" due to inconsistencyand inaccuracy. My major objections are : the DFT method with such a smallbasis set is not reliable at all and leads to erroneous claim(本工作中用的方法基组为ωB97XD functional[28] and the 6−311++G(d, p)), similarly MDsimulation with such a small box is also not reliable (这个问题我可以解决), the adopted method ispoor to describe the charge systems, the authors didn't analyze the energyoutput of MD simulations to understand the forces responsible for stability....
本工作中的计算模拟部分的计算方法叙述如下:
AllMD simulations were carried out using GROMACS-5.1.5 software package[27].The initial structure of NO3- was optimized at ωB97XD functional[28] and the 6−311++G(d, p) basis set level[29] in Gaussian16 package[30].The partial charges on each atom of NO3- were obtained from Ref. 31.The parameters of NO3- initially parametrized using AMBERwere converted to GROMACS format using the ACPYPE script[32]. Thewater molecules were modeled using the SPC/E model[33]. All bondsand angles of the water molecules were constrained using the SHAKE algorithm[34].Initially, energy minimization corrected atomic overlaps to ensure that themaximum force on any atom was below 100 kJ mol-1 nm-1 maintaininga pressure of 1 atm and a temperature of 300 K.
Allsystems were relaxed by an energy minimization step using the steepest descentmethod with a time step of 100 fs. Then, the equilibration in the isobaric-isothermal(NPT) ensemble was carried out for a 20 ns simulation length while maintainingthe pressure at 1 atm and temperature at 300 K using a velocity-rescalethermostat[35] and the Parrinello-Rahman scheme[36] witha time step of 1 fs. The production runs were carried out in the NPT ensemblefor 50 ns with a time step of 1 fs. The temperature was maintained using the V-rescalethermostat, while the pressure was controlled using the Parrinello-Rahmanbarostat. Long-range electrostatic interactions were guided by particle meshEwald (PME)[37-39] with a cut-off distance of4.7Å with a PME order of 6 and an Ewald tolerance of 10−6. Thetrajectory data were collected every 0.5 ps for analysis. Molecule visualizationwas displayed by the Visual Molecular Dynamics (VMD) program[40].The partial electric charge sets, Lennard-Jones parameters for the systems, andthe details of the simulation box are shown in the Supporting Information inTable S1 and S2.
恳请各位老师提供些改进的意见和方法,非常感谢
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