- 输入参数：一个典型的mdp文件
1 ; 2 ; STANDARD MD INPUT OPTIONS FOR MARTINI 2.x 3 ; Updated 02 feb 2013 by DdJ 4 ; 5 ; for use with GROMACS 4.5/4.6 6 ; 7 8 title = Martini 9 10 ; TIMESTEP IN MARTINI 11 ; Most simulations are numerically stable 12 ; with dt=40 fs, some (especially rings and polarizable water) require 20-30 fs. 13 ; Note that time steps of 40 fs and larger may create local heating or 14 ; cooling in your system. Although the use of a heat bath will globally 15 ; remove this effect, it is advised to check consistency of 16 ; your results for somewhat smaller time steps in the range 20-30 fs. 17 ; Time steps exceeding 40 fs should not be used; time steps smaller 18 ; than 20 fs are also not required unless specifically stated in the itp file. 19 ; 时间步长：不要大于40，不要小于20.20-30fs是一个很好的选择。 20 21 integrator = md 22 dt = 0.04 23 nsteps = 50000 24 nstcomm = 10 ;质心移动的频率 25 comm-grps = ;对质心的分组，默认为整个系统 26 27 nstxout = 0 28 nstvout = 0 29 nstfout = 0 30 nstlog = 1000 31 nstenergy = 100 32 nstxtcout = 1000 ;number of steps that elapse between writing position coordinates using lossy compression 每隔几步输出一次低精度坐标值 33 xtc_precision = 100 ;轨迹压缩文件的精度 34 xtc-grps = ;轨迹压缩文件内部的分组 35 energygrps = DPPC W 36 37 ; NEIGHBOURLIST and MARTINI 38 ; Due to the use of shifted potentials, the noise generated 39 ; from particles leaving/entering the neighbour list is not so large, 40 ; even when large time steps are being used. In practice, once every 41 ; ten steps works fine with a neighborlist cutoff that is equal to the 42 ; non-bonded cutoff (1.2 nm). However, to improve energy conservation 43 ; or to avoid local heating/cooling, you may increase the update frequency 44 ; and/or enlarge the neighbourlist cut-off (to 1.4 nm). The latter option 45 ; is computationally less expensive and leads to improved energy conservation 46 ;由于使用了漂移势，临近列表的噪声较大。一般将刷新频率设为10，截断距离设为1.2nm，不过为了更好地精度，截断距离也可设为1.4nm，这样既可以获得更高精度， 47 ;也不会带来过多的计算量。 48 49 nstlist = 10 50 ns_type = grid 51 pbc = xyz 52 rlist = 1.4 ; 截断距离，1.4nm以外的不再视为键合和近邻作用 53 54 ; MARTINI and NONBONDED 55 ; Standard cut-off schemes are used for the non-bonded interactions 56 ; in the Martini model: LJ interactions are shifted to zero in the 57 ; range 0.9-1.2 nm, and electrostatic interactions in the range 0.0-1.2 nm. 58 ; The treatment of the non-bonded cut-offs is considered to be part of 59 ; the force field parameterization, so we recommend not to touch these 60 ; values as they will alter the overall balance of the force field. 61 ; In principle you can include long range electrostatics through the use 62 ; of PME, which could be more realistic in certain applications 63 ; Please realize that electrostatic interactions in the Martini model are 64 ; not considered to be very accurate to begin with, especially as the 65 ; screening in the system is set to be uniform across the system with 66 ; a screening constant of 15. When using PME, please make sure your 67 ; system properties are still reasonable. 68 ; 标准截断被用于Martini模型中的非键合作用：LJ作用在0.9-1.2nm之间变为0，并且静电作用发生在0-1.2nm之内。 69 ; 对非键合力的处理是经过仔细考虑了买我们建议你不要乱动。原则上，你可以将长程静电力也纳入考虑，通过使用PME方法，这在一些情况下会更精确。 70 ; 请注意，在Martini模型中，静电作用从一开始就是不精确的，当使用PME时，请确认你的系统性质仍然是合理的 71 ; With the polarizable water model, the relative electrostatic screening 72 ; (epsilon_r) should have a value of 2.5, representative of a low-dielectric 73 ; apolar solvent. The polarizable water itself will perform the explicit screening 74 ; in aqueous environment. In this case, the use of PME is more realistic. 75 ; 在可极化水模型中，相关的静电筛选（epsilon-r）应该取2.5，代表一个低的无极化溶液。 76 ; For use in combination with the Verlet-pairlist algorithm implemented 77 ; in Gromacs 4.6 a straight cutoff in combination with the potential 78 ; modifiers can be used. Although this will change the potential shape, 79 ; preliminary results indicate that forcefield properties do not change a lot 80 ; when the LJ cutoff is reduced to 1.1 nm. Be sure to test the effects for 81 ; your particular system. The advantage is a gain of speed of 50-100%. 82 ; 83 84 coulombtype = Shift ; 在某个位置将势能设为常数（0） 85 ;Reaction_field (for use with Verlet-pairlist) ;PME (especially with polarizable water) 86 rcoulomb_switch = 0.0 ;where to start switching the Coulomb potential, only relevant when force or potential switching is used 87 ; 在何处开启库仑势 88 rcoulomb = 1.2 89 ;distance for the Coulomb cut-off 截断距离 90 epsilon_r = 15 ;The relative dielectric constant. A value of 0 means infinity. 91 ; 2.5 (with polarizable water) 92 vdw_type = Shift ;cutoff (for use with Verlet-pairlist) 93 rvdw_switch = 0.9 94 rvdw = 1.2 ;1.1 (for use with Verlet-pairlist) 95 96 ;cutoff-scheme = verlet 97 ;coulomb-modifier = Potential-shift 98 ;vdw-modifier = Potential-shift 99 ;epsilon_rf = 0 ; epsilon_rf = 0 really means epsilon_rf = infinity,即截断距离之外的静电常数为无穷大 100 ;verlet-buffer-drift = 0.005 101 102 ; MARTINI and TEMPERATURE/PRESSURE 103 ; normal temperature and pressure coupling schemes can be used. 正常的温度和压力耦合就可以 104 ; It is recommended to couple individual groups in your system separately. 建议分组耦合 105 ; Good temperature control can be achieved with the velocity rescale (V-rescale) 使用速度重整化恒温器，耦合时间常数设为1ps。 106 ; thermostat using a coupling constant of the order of 1 ps. Even better 当然使用0.1ps效果就更好了，但这样的耦合就不能称之为弱耦合了 107 ; temperature control can be achieved by reducing the temperature coupling 108 ; constant to 0.1 ps, although with such tight coupling (approaching 109 ; the time step) one can no longer speak of a weak-coupling scheme. 110 ; We therefore recommend a coupling time constant of at least 0.5 ps. 我们推荐耦合时间常数最少为0.5ps 111 ; The Berendsen thermostat is less suited since it does not give Berendsen恒温器不太适用，因为他不能给出一个良好的系综 112 ; a well described thermodynamic ensemble. 113 ; 114 ; Pressure can be controlled with the Parrinello-Rahman barostat, 压力可用P-R恒压。耦合时间常数在4-8ps之间。 115 ; with a coupling constant in the range 4-8 ps and typical compressibility 注意到，为了平衡，Berendsen恒温器可能产生更好的效果，因为P-R易于被扰动。 116 ; in the order of 10-4 - 10-5 bar-1. Note that, for equilibration purposes, 117 ; the Berendsen thermostat probably gives better results, as the Parrinello- 118 ; Rahman is prone to oscillating behaviour. For bilayer systems the pressure 对于双层膜系统，压力耦合应该是半各向异性。 119 ; coupling should be done semiisotropic. 120 121 tcoupl = v-rescale 122 tc-grps = DPPC W 123 tau_t = 1.0 1.0 124 ref_t = 320 320 125 Pcoupl = parrinello-rahman 126 Pcoupltype = semiisotropic 127 tau_p = 12.0 12.0 ;parrinello-rahman is more stable with larger tau-p, DdJ, 20130422 128 compressibility = 3e-4 3e-4 129 ref_p = 1.0 1.0 130 131 gen_vel = no 132 gen_temp = 320 133 gen_seed = 473529 134 135 ; MARTINI and CONSTRAINTS 136 ; for ring systems and stiff bonds constraints are defined 137 ; which are best handled using Lincs. 138 139 constraints = none 140 constraint_algorithm = Lincs 141 unconstrained_start = no; 启动时不做限制：no（对初始构象做限制，重构壳层），yes（不对初始构象做限制） 142 lincs_order = 4 143 lincs_warnangle = 30
时间步长：推荐将时间步长设为20-30 fs, 同时使用更大的邻区列表截断(到1.4 nm).
温度与压力耦合时间常数：好的温度控制可以使用Berendsen方法, 耦合常数的数量级为τ= 1 ps.压力可采用Berendsen方法进行控制, 耦合常数的范围在1-5 ps之间, 典型的压缩系数为10-4-10-3 bar-1. 需要注意的是, 为了估算CG模拟的压缩系数, 你应该使用Parrinello-Rahman耦合方法.
配对列表(pairlist)以及配对列表截断(pairlist cutoff)：10步一次，1.4或1.2nm
截断(cutoffs)的选择：对于非键作用, 使用标准的截断(cutoff)方案: LJ相互作用在0.9-1.2 nm的范围内被调整为0, 静电相互作用的调整范围为0.0-1.2 nm. 对非键截断的处理是力场参数化的一部分, 最好不要去碰这些值, 因为这可能会改变力场的整体平衡.
PME与反应力场：原则上是可以用的, 尽管Martini力场参数化时使用短程移位静电相互作用. 使用反应力场(也可等效为移位势能)可能不会对模拟有太大影响. 另一方面, PME可能导致模拟行为显著不同, 在某些应用中可能更真实(如在枝状聚合物和抑菌多肽攻击脂质双层膜的模拟中可以看到真实的膜孔). 需要注意的是, Matini模型中的静电相互作用并不是很精确, 尤其整个系统的屏蔽被设为均匀的, 具有相同的屏蔽常数15. 当使用PME时, 请确保体系的性质仍然是合理的.PME可以与极化Martini水模型结合使用, 并且是合理的, 因为静电相互作用更真实.