{ "cells": [ { "attachments": {}, "cell_type": "markdown", "metadata": {}, "source": [ "### Temporally Correlated Active Noise Simulation Tutorial\n", "\n", "Temporally Correlated Active Noise Simulation is available in OpenMichroM versions >= 1.0.7 \n", "\n", "#### Introduction\n", "\n", "This tutorial is aimed at introducing nonequilibrium activity to OpenMiChroM simulations. First, we will go through a very brief introduction of the theoretical idea, then, the simulation procedures are discussed.\n", "\n", "##### Theory\n", "\n", "Activity, such as originating from molecular motors applying forces on the polymer, is modeled as \n", "an athermal drive experienced by each coarse-grained monomer. Since motors typically exhibit on/off dynamics, the athermal force is expected to be correlated in time, as opposed to the thermal noise\n", "that is temporally uncorrelated. To model activity, we add a novel noise-like term to the forces associated with a monomer, such that the equation of motion of the $n$-th monomer reads as follows:\n", "\n", "$$\n", "\\gamma \\frac{dr_n}{dt} = -\\nabla_n U + \\xi^{\\rm therm}_n + f^{\\rm act}_n\n", "$$\n", "\n", "where $\\gamma$ is the damping coefficient and $U$ is the passive potential, like the harmonic bonds joining neighboring monomers in a polymer. \n", "$\\xi^{\\rm therm}_n$ is the the thermal noise that is uncorrelated over time as well as across the chain:\n", "\n", "$$\n", "\\langle \\xi^{\\rm therm}_n(t)\\rangle=0\\quad \\text{and} \\quad \\langle \\xi^{\\rm therm}_n(t)\\xi^{\\rm therm}_m(t^\\prime)\\rangle = 2\\gamma T\\delta_{mn}\\delta(t-t^\\prime).\n", "$$\n", "\n", "The active noise kicks are given by $f^{\\rm act}(t)$, which are correlated over time and their correlation decays over a characteristic time scale $\\tau$:\n", "\n", "$$\n", "\\langle f^{\\rm act}_n \\rangle=0 \\quad \\text{and} \\quad \\langle f^{\\rm act}_n(t)f^{\\rm act}_m(t^\\prime) \\rangle=F^2e^{-|t-t^\\prime|/\\tau}\\delta_{mn}\n", "$$\n", "\n", "The dynamics of the active force of the $n$-th monomer is governed by the following equation:\n", "\n", "$$\n", "\\tau \\frac{df^{\\rm act}_n}{dt} = -f^{\\rm act}_n + \\sqrt{2\\gamma \\theta_a}\\eta(t)\n", "$$\n", "\n", "where $\\theta_a\\equiv F^2\\tau/\\gamma$ is the active temperature-like quantity, and $\\eta(t)$ is a delta-correlated stationary Gaussian process.\n", "\n", "\n", "##### Brownian Dynamics\n", "Brownian dynamics only has forces and displacements, and no velocities. The positions after time $\\Delta t$, given by $x(t+\\Delta t)$ are computed based on the current forces $h(t)$ and positions $x(t)$.\n", "\n", "$$\n", "x_n(t+\\Delta t)=x_n(t)+\\frac{h_n(t)}{\\gamma}\\Delta t+\\sqrt{\\frac{2T}{\\gamma}\\Delta t}\\mathcal{N}(0,1)\n", "$$\n", "\n", "where the last term is the thermal kick at temperature $T$ with $\\mathcal{N}(0,1)$ representing a random Normal variable with zero mean and unit standard deviation. The net force experienced by the $n$-th monomer at time step $t$ is given by $h_n(t)$.\n", "\n", "$$\n", "h_n(t)= -\\frac{\\partial}{\\partial x}\\sum_{m}U(|x_n(t)-x_m(t)|)+f^{\\rm act}_n(t)\n", "$$\n", "\n", "The net force for a monomer $h(t)$, depends on the active force of the monomer $f^{\\rm act}(t)$, which is related to the active force in the previous time step $f^{\\rm act}(t-\\Delta t)$.\n", "The active force on the $n$-th monomer at time $t$ is obtained as follows:\n", "\n", "$$\n", "f^{\\rm act}_n(t)=f^{\\rm act}_n(t-\\Delta t)e^{-\\Delta t/\\tau}+{F}\\sqrt{1-e^{-2\\Delta t/\\tau}}\\mathcal{\\tilde{N}}(0,1)\n", "$$\n", "\n", "\n", "where $\\mathcal{\\tilde{N}}(0,1)$ is a random Normal variable that is different from the thermal one. \n", "\n", "Next is a step-by-step guidance on how to setup and run OpenMiChroM simulations with correlated active noise. Users not familiar with running OpenMiChroM simulations, would greatly benefit from first going through the practice of running equilibrium OpenMiChroM simulations - see [Tutorial_Single_Chromosome](https://open-michrom.readthedocs.io/en/latest/Tutorials/Tutorial_Single_Chromosome.html). For users already familiar with OpenMiChroM, it is still the same simulation object that is created and basic steps of running the simulations are the same. The main differences are two fold: \n", "1. Adding activity using a function **addCorrelatedNoise()**. One should make sure to add activity as the first force field. It is extremely important that the active force is assigned a force-group \"0\".\n", "2. Using a custom integrator **ActiveBrownianIntegrator** (see Integrator.py) that takes care of the active force which is hard-coded to be the force-group \"0\". Hence the catutionary statement above.\n", "\n", "Hope you follow along!" ] }, { "attachments": {}, "cell_type": "markdown", "metadata": {}, "source": [ "#### Simulations\n", "##### Import modules\n", "\n", "Active functions are \n" ] }, { "cell_type": "code", "execution_count": 1, "metadata": {}, "outputs": [], "source": [ "import sys \n", "sys.path.append('../../OpenMiChroM/')\n", "from ChromDynamics import MiChroM\n", "from Integrators import ActiveBrownianIntegrator\n", "import numpy as np" ] }, { "attachments": {}, "cell_type": "markdown", "metadata": {}, "source": [ "##### Initialize simulation" ] }, { "cell_type": "code", "execution_count": 2, "metadata": {}, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ " *************************************************************************************** \n", " **** **** *** *** *** *** *** *** OpenMiChroM-1.0.6 *** *** *** *** *** *** **** **** \n", "\n", " OpenMiChroM is a Python library for performing chromatin dynamics simulations. \n", " OpenMiChroM uses the OpenMM Python API, \n", " employing the MiChroM (Minimal Chromatin Model) energy function. \n", " The chromatin dynamics simulations generate an ensemble of 3D chromosomal structures \n", " that are consistent with experimental Hi-C maps, also allows simulations of a single \n", " or multiple chromosome chain using High-Performance Computing \n", " in different platforms (GPUs and CPUs). \n", " OpenMiChroM documentation is available at https://open-michrom.readthedocs.io \n", "\n", " OpenMiChroM is described in: Oliveira Junior, A. B & Contessoto, V, G et. al. \n", " A Scalable Computational Approach for Simulating Complexes of Multiple Chromosomes. \n", " Journal of Molecular Biology. doi:10.1016/j.jmb.2020.10.034. \n", " and \n", " Oliveira Junior, A. B. et al. \n", " Chromosome Modeling on Downsampled Hi-C Maps Enhances the Compartmentalization Signal. \n", " J. Phys. Chem. B, doi:10.1021/acs.jpcb.1c04174. \n", "\n", " Copyright (c) 2022, The OpenMiChroM development team at \n", " Rice University \n", " *************************************************************************************** \n" ] } ], "source": [ "# Instantiate MiChroM object\n", "sim = MiChroM(name='active_Rouse_sim', temperature=0.2, time_step=0.001, collision_rate=1.0)\n", "\n", "# specify platform and output destination\n", "sim.setup(platform=\"opencl\")\n", "sim.saveFolder('./out')\n", "active_correaltion_time = 5.0\n", "#specify the integrator for correlated noise\n", "#note that the force-group \"0\" is associated with the correlated active noise\n", "sim.integrator = ActiveBrownianIntegrator(timestep=sim.timestep, temperature=sim.temperature, \n", " collision_rate=sim.collisionRate, corr_time=active_correaltion_time)" ] }, { "attachments": {}, "cell_type": "markdown", "metadata": {}, "source": [ "##### Load initial structure" ] }, { "cell_type": "code", "execution_count": 3, "metadata": {}, "outputs": [], "source": [ "# generate a test sequence file of size n\n", "n=10\n", "with open('test_seq.txt','w') as seq_file:\n", " for ii in range(n):\n", " seq_file.write(f'{ii+1} A1\\n')\n", "\n", "# create a random configuration with the sequence file\n", "init_struct = sim.createRandomWalk(ChromSeq='test_seq.txt')\n", "sim.loadStructure(init_struct, center=True)\n", "\n", "#uncomment below to save the loaded structure\n", "# sim.saveStructure(mode = 'auto')" ] }, { "attachments": {}, "cell_type": "markdown", "metadata": {}, "source": [ "##### Add forces" ] }, { "cell_type": "code", "execution_count": 4, "metadata": {}, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "\n", " ==================================\n", " Active Monomers (correlated noise) added.\n", " Active correlation time: 5.0\n", " Total number of active monomers: 10\n", " Total number of monomers: 10\n", " ==================================\n", "\n" ] } ], "source": [ "# For the purpose of the simualtion we will consider a simple simulation of an active Rouse chain - harmonically bonded monomers with zero rest length\n", "# the good things about active Rouse chain is that the dynamics may be calculated analytically and compared for verification.\n", "# Any force-field available for OpenMiChroM, like self-avoidance, may be used. \n", "# However, since Brownian Dynamics does not have momentum, it is prudent to make sure the time step is small enough for steep potentials. \n", "# Using too large a time step with steep (or worse, diverging!) potentials will generate huge forces, possibly leading to explosion! wear your safety goggles!\n", "\n", "# Now the force-fields:\n", "# first, add correlated noise. \n", "# IMPORTANT: correlated noise should always be added as the *first* force-field.\n", "# This is because force-group \"0\" is hard-coded as the active force within ActiveBrownianIntegrator\n", "# act_seq contains the active force values F for each monomer. It needs to be the same size as the total number of monomers\n", "# the values F_i in the list need not be the same, they can be heterogenous depicting varied motor activity\n", "# below we consider a homogenously active polymer\n", "F = 0.5\n", "sim.addCorrelatedNoise(act_seq=F*np.ones(sim.N))\n", "\n", "# add Harmonic bonds between monomers of the chain. Use sim.chains to get the number of chains.\n", "# setting the rest length to zero since the analytical form is easier to calculate that way.\n", "kb=5.0\n", "sim.addHarmonicBonds(kfb=kb, r0=0.0)\n", "\n", "# adding soft-core self-avoidance \n", "# repulsion is modeled using a sigmoid function with a finite overlap energy Ecut\n", "# sim.addSelfAvoidance(Ecut=4.0, k_rep=20.0, r0=1.0)\n", "\n", "# half-harmonic restraint as confinement\n", "# sim.addFlatBottomHarmonic(kr=10.0, n_rad=20.0)" ] }, { "attachments": {}, "cell_type": "markdown", "metadata": {}, "source": [ "##### Run intial collapse" ] }, { "cell_type": "code", "execution_count": 5, "metadata": {}, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Number of exceptions: 9\n", "adding force ActiveForce 0\n", "adding force HarmonicBond 1\n", "Positions... \n", " loaded!\n", "potential energy is 2.250014\n", "bl=0 pos[1]=[-0.1 -0.6 0.4] dr=1.67 t=3.0ps kin=5.53 pot=0.39 Rg=0.631 SPS=7171 \n", "bl=0 pos[1]=[0.5 -1.6 1.8] dr=1.64 t=6.0ps kin=4.23 pot=-0.36 Rg=0.610 SPS=8611 \n", "bl=0 pos[1]=[0.7 -2.8 1.5] dr=0.99 t=9.0ps kin=2.77 pot=-0.19 Rg=0.699 SPS=8800 \n", "bl=0 pos[1]=[1.7 -2.8 1.7] dr=1.10 t=12.0ps kin=3.35 pot=-0.50 Rg=0.923 SPS=8863 \n", "bl=0 pos[1]=[2.2 -2.3 2.6] dr=0.86 t=15.0ps kin=2.37 pot=-0.70 Rg=0.530 SPS=8788 \n", "bl=0 pos[1]=[1.7 -2.6 3.0] dr=0.75 t=18.0ps kin=3.77 pot=-0.62 Rg=0.517 SPS=8933 \n", "bl=0 pos[1]=[1.6 -1.6 3.6] dr=1.13 t=21.0ps kin=3.43 pot=-0.39 Rg=0.972 SPS=8865 \n", "bl=0 pos[1]=[1.3 -2.0 3.1] dr=1.29 t=24.0ps kin=3.95 pot=0.10 Rg=0.891 SPS=8965 \n", "bl=0 pos[1]=[1.2 -3.6 1.4] dr=1.26 t=27.0ps kin=5.72 pot=0.83 Rg=0.717 SPS=8999 \n", "bl=0 pos[1]=[1.5 -4.1 1.2] dr=0.63 t=30.0ps kin=3.92 pot=0.74 Rg=0.530 SPS=9082 \n" ] } ], "source": [ "#run collapse simulation\n", "for _ in range(10):\n", " sim.runSimBlock(3000, increment=False)\n", "\n", "# save the collapsed structure -- uncomment below\n", "# sim.saveStructure(filename='collapse',mode='ndb')" ] }, { "attachments": {}, "cell_type": "markdown", "metadata": {}, "source": [ "##### Run simulation" ] }, { "cell_type": "code", "execution_count": 6, "metadata": {}, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "bl=1 pos[1]=[1.3 -5.0 1.1] dr=0.62 t=31.0ps kin=2.41 pot=0.79 Rg=0.588 SPS=7621 \n", "bl=2 pos[1]=[1.6 -4.5 1.2] dr=0.61 t=32.0ps kin=3.50 pot=0.55 Rg=0.624 SPS=7894 \n", "bl=3 pos[1]=[1.1 -5.2 1.3] dr=0.68 t=33.0ps kin=3.32 pot=0.83 Rg=0.890 SPS=8432 \n", "bl=4 pos[1]=[1.0 -4.6 1.3] dr=0.60 t=34.0ps kin=3.93 pot=1.05 Rg=0.706 SPS=8478 \n", "bl=5 pos[1]=[0.9 -5.4 1.2] dr=0.64 t=35.0ps kin=2.70 pot=1.35 Rg=0.897 SPS=8574 \n", "bl=6 pos[1]=[1.5 -5.2 1.3] dr=0.66 t=36.0ps kin=3.38 pot=0.93 Rg=0.774 SPS=8658 \n", "bl=7 pos[1]=[1.9 -5.3 1.8] dr=0.62 t=37.0ps kin=2.75 pot=0.97 Rg=0.833 SPS=8889 \n", "bl=8 pos[1]=[2.0 -5.1 2.3] dr=0.53 t=38.0ps kin=3.94 pot=0.70 Rg=0.517 SPS=8786 \n", "bl=9 pos[1]=[1.8 -5.4 2.4] dr=0.54 t=39.0ps kin=3.99 pot=0.69 Rg=0.544 SPS=8805 \n", "bl=10 pos[1]=[1.6 -5.9 3.1] dr=0.75 t=40.0ps kin=2.92 pot=0.54 Rg=0.468 SPS=8681 \n", "bl=11 pos[1]=[2.1 -6.0 3.2] dr=0.71 t=41.0ps kin=1.58 pot=0.87 Rg=0.451 SPS=8699 \n", "bl=12 pos[1]=[2.5 -6.8 3.3] dr=0.78 t=42.0ps kin=2.89 pot=0.69 Rg=0.360 SPS=8515 \n", "bl=13 pos[1]=[2.0 -6.6 3.4] dr=0.81 t=43.0ps kin=2.64 pot=0.81 Rg=0.444 SPS=8633 \n", "bl=14 pos[1]=[1.7 -7.1 3.2] dr=0.52 t=44.0ps kin=2.34 pot=1.00 Rg=0.476 SPS=8597 \n", "bl=15 pos[1]=[1.8 -6.6 3.3] dr=0.90 t=45.0ps kin=2.82 pot=1.51 Rg=0.600 SPS=8924 \n", "bl=16 pos[1]=[1.9 -6.9 2.9] dr=0.59 t=46.0ps kin=2.70 pot=2.04 Rg=0.533 SPS=8925 \n", "bl=17 pos[1]=[1.7 -6.3 2.3] dr=0.65 t=47.0ps kin=2.17 pot=2.08 Rg=0.623 SPS=8774 \n", "bl=18 pos[1]=[0.7 -7.1 2.6] dr=0.72 t=48.0ps kin=2.32 pot=1.98 Rg=0.651 SPS=8284 \n", "bl=19 pos[1]=[1.5 -7.2 3.0] dr=0.73 t=49.0ps kin=2.22 pot=1.70 Rg=0.239 SPS=8612 \n", "bl=20 pos[1]=[1.0 -7.7 3.5] dr=0.57 t=50.0ps kin=2.30 pot=1.83 Rg=0.368 SPS=8729 \n", "bl=21 pos[1]=[1.1 -7.5 4.5] dr=0.73 t=51.0ps kin=1.98 pot=1.71 Rg=0.629 SPS=8843 \n", "bl=22 pos[1]=[1.1 -7.6 4.4] dr=0.45 t=52.0ps kin=2.86 pot=1.61 Rg=0.725 SPS=8919 \n", "bl=23 pos[1]=[1.1 -7.6 3.6] dr=0.61 t=53.0ps kin=2.89 pot=1.53 Rg=0.522 SPS=8702 \n", "bl=24 pos[1]=[1.0 -7.3 3.9] dr=0.54 t=54.0ps kin=3.78 pot=1.54 Rg=0.455 SPS=8720 \n", "bl=25 pos[1]=[0.6 -7.3 4.2] dr=0.45 t=55.0ps kin=2.99 pot=1.53 Rg=0.688 SPS=8669 \n", "bl=26 pos[1]=[0.5 -7.1 3.8] dr=0.66 t=56.0ps kin=2.67 pot=2.00 Rg=0.691 SPS=8478 \n", "bl=27 pos[1]=[-0.1 -7.4 3.1] dr=0.54 t=57.0ps kin=2.49 pot=2.12 Rg=0.597 SPS=8733 \n", "bl=28 pos[1]=[0.3 -7.0 3.3] dr=0.64 t=58.0ps kin=2.04 pot=2.53 Rg=0.507 SPS=8880 \n", "bl=29 pos[1]=[-0.3 -7.2 3.7] dr=0.70 t=59.0ps kin=1.81 pot=2.13 Rg=0.478 SPS=8714 \n", "bl=30 pos[1]=[-0.4 -7.2 4.2] dr=0.67 t=60.0ps kin=2.98 pot=2.15 Rg=0.691 SPS=8777 \n", "bl=31 pos[1]=[0.3 -6.7 3.6] dr=0.72 t=61.0ps kin=2.48 pot=1.79 Rg=0.390 SPS=8590 \n", "bl=32 pos[1]=[0.2 -7.0 3.9] dr=0.38 t=62.0ps kin=2.82 pot=1.92 Rg=0.525 SPS=8689 \n", "bl=33 pos[1]=[0.6 -6.5 4.0] dr=0.53 t=63.0ps kin=3.03 pot=1.82 Rg=0.580 SPS=8618 \n", "bl=34 pos[1]=[0.6 -6.5 3.7] dr=0.43 t=64.0ps kin=2.71 pot=1.54 Rg=0.350 SPS=8732 \n", "bl=35 pos[1]=[0.2 -6.7 4.1] dr=0.57 t=65.0ps kin=3.25 pot=1.40 Rg=0.499 SPS=8902 \n", "bl=36 pos[1]=[0.7 -6.5 4.1] dr=0.78 t=66.0ps kin=2.26 pot=1.13 Rg=0.321 SPS=8771 \n", "bl=37 pos[1]=[0.5 -6.4 4.0] dr=0.50 t=67.0ps kin=1.75 pot=1.21 Rg=0.413 SPS=9004 \n", "bl=38 pos[1]=[0.3 -6.7 4.4] dr=0.48 t=68.0ps kin=2.10 pot=1.08 Rg=0.365 SPS=8660 \n", "bl=39 pos[1]=[0.2 -7.4 4.6] dr=0.72 t=69.0ps kin=2.33 pot=0.99 Rg=0.518 SPS=8627 \n", "bl=40 pos[1]=[0.9 -7.0 5.2] dr=0.87 t=70.0ps kin=2.63 pot=0.42 Rg=0.360 SPS=8620 \n", "bl=41 pos[1]=[1.4 -6.8 4.5] dr=0.67 t=71.0ps kin=2.64 pot=0.52 Rg=0.528 SPS=8807 \n", "bl=42 pos[1]=[0.7 -5.8 5.3] dr=0.73 t=72.0ps kin=3.55 pot=0.47 Rg=0.452 SPS=8790 \n", "bl=43 pos[1]=[0.6 -5.9 6.2] dr=0.79 t=73.0ps kin=3.02 pot=0.61 Rg=0.568 SPS=8901 \n", "bl=44 pos[1]=[0.0 -6.3 5.2] dr=0.81 t=74.0ps kin=3.40 pot=1.12 Rg=0.557 SPS=8937 \n", "bl=45 pos[1]=[-0.1 -7.4 5.6] dr=0.80 t=75.0ps kin=2.41 pot=1.57 Rg=0.484 SPS=8856 \n", "bl=46 pos[1]=[-1.1 -7.2 5.3] dr=0.75 t=76.0ps kin=4.20 pot=1.90 Rg=0.425 SPS=8737 \n", "bl=47 pos[1]=[-1.5 -7.3 4.7] dr=0.86 t=77.0ps kin=6.58 pot=2.32 Rg=0.405 SPS=8678 \n", "bl=48 pos[1]=[-1.7 -7.1 4.2] dr=0.90 t=78.0ps kin=5.83 pot=2.99 Rg=0.470 SPS=8809 \n", "bl=49 pos[1]=[-2.5 -7.0 4.0] dr=0.78 t=79.0ps kin=6.04 pot=3.31 Rg=0.555 SPS=8671 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [-2.5260031 -7.63105731 4.11936607] Rg = 0.555199\n", " median bond size is 0.2993247084597079\n", " three shortest/longest (<10)/ bonds are [0.0619413 0.18132575 0.26687537] [0.48378056 0.48624118 0.52440487]\n", " 95 percentile of distance to center is: 0.7736948328496079\n", " density of closest 95% monomers is: 4.896952672744252\n", " density of the core monomers is: 5.717321659637082\n", " min/median/mean/max coordinates are: \n", " x: -2.93, -2.53, -2.53, -2.17\n", " y: -8.26, -7.68, -7.63, -7.01\n", " z: 3.84, 4.10, 4.12, 4.60\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 6.038497269500298 should be: 1.5\n", " fastest particles are (in kT): [ 4.12132149 7.91483392 8.78585725 10.29837843 17.11273306]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 3.3082054138183596\n", "bl=50 pos[1]=[-2.4 -6.7 4.2] dr=0.84 t=80.0ps kin=5.53 pot=3.82 Rg=0.769 SPS=8882 \n", "bl=51 pos[1]=[-3.4 -7.3 4.4] dr=0.75 t=81.0ps kin=3.60 pot=4.06 Rg=0.507 SPS=8752 \n", "bl=52 pos[1]=[-3.3 -8.0 3.4] dr=1.18 t=82.0ps kin=2.91 pot=4.97 Rg=0.629 SPS=8653 \n", "bl=53 pos[1]=[-4.1 -7.9 3.5] dr=0.57 t=83.0ps kin=2.69 pot=4.81 Rg=0.584 SPS=8691 \n", "bl=54 pos[1]=[-3.8 -8.8 3.6] dr=0.53 t=84.0ps kin=3.32 pot=4.78 Rg=0.494 SPS=8960 \n", "bl=55 pos[1]=[-3.7 -9.5 3.0] dr=0.63 t=85.0ps kin=3.45 pot=5.15 Rg=0.389 SPS=8810 \n", "bl=56 pos[1]=[-3.2 -8.6 2.2] dr=0.80 t=86.0ps kin=2.76 pot=5.04 Rg=0.580 SPS=8745 \n", "bl=57 pos[1]=[-3.2 -8.5 1.7] dr=0.60 t=87.0ps kin=1.64 pot=5.17 Rg=0.476 SPS=8836 \n", "bl=58 pos[1]=[-2.8 -8.5 2.3] dr=0.54 t=88.0ps kin=3.29 pot=5.08 Rg=0.562 SPS=8871 \n", "bl=59 pos[1]=[-2.6 -8.1 2.3] dr=0.68 t=89.0ps kin=2.82 pot=4.93 Rg=0.351 SPS=8918 \n", "bl=60 pos[1]=[-2.8 -7.6 1.6] dr=0.66 t=90.0ps kin=3.23 pot=4.73 Rg=0.450 SPS=8534 \n", "bl=61 pos[1]=[-2.2 -7.6 1.2] dr=0.69 t=91.0ps kin=2.43 pot=4.52 Rg=0.618 SPS=8722 \n", "bl=62 pos[1]=[-1.6 -6.9 1.7] dr=0.65 t=92.0ps kin=2.53 pot=4.52 Rg=0.731 SPS=8448 \n", "bl=63 pos[1]=[-1.8 -6.9 1.1] dr=0.65 t=93.0ps kin=3.41 pot=4.43 Rg=0.776 SPS=7700 \n", "bl=64 pos[1]=[-2.4 -6.4 1.1] dr=0.69 t=94.0ps kin=4.03 pot=4.38 Rg=0.718 SPS=7988 \n", "bl=65 pos[1]=[-1.7 -6.0 0.9] dr=0.61 t=95.0ps kin=3.88 pot=4.20 Rg=0.679 SPS=7884 \n", "bl=66 pos[1]=[-1.2 -6.3 0.8] dr=0.46 t=96.0ps kin=3.68 pot=4.46 Rg=0.591 SPS=7482 \n", "bl=67 pos[1]=[-1.8 -5.9 1.5] dr=0.83 t=97.0ps kin=3.63 pot=4.16 Rg=0.717 SPS=7743 \n", "bl=68 pos[1]=[-2.3 -5.9 1.2] dr=0.75 t=98.0ps kin=4.69 pot=4.26 Rg=0.497 SPS=7625 \n", "bl=69 pos[1]=[-2.1 -5.3 0.6] dr=0.78 t=99.0ps kin=5.80 pot=4.54 Rg=0.683 SPS=8434 \n", "bl=70 pos[1]=[-3.3 -4.9 0.5] dr=0.82 t=100.0ps kin=6.19 pot=4.70 Rg=0.679 SPS=8482 \n", "bl=71 pos[1]=[-3.9 -4.5 0.2] dr=1.02 t=101.0ps kin=6.62 pot=4.68 Rg=0.565 SPS=8872 \n", "bl=72 pos[1]=[-4.3 -5.5 0.5] dr=1.14 t=102.0ps kin=7.04 pot=5.07 Rg=0.536 SPS=8607 \n", "bl=73 pos[1]=[-5.0 -4.5 0.5] dr=0.87 t=103.0ps kin=5.33 pot=5.05 Rg=0.554 SPS=8651 \n", "bl=74 pos[1]=[-5.3 -3.9 0.4] dr=0.88 t=104.0ps kin=4.96 pot=5.19 Rg=0.664 SPS=8740 \n", "bl=75 pos[1]=[-6.1 -3.7 0.1] dr=1.09 t=105.0ps kin=5.61 pot=5.87 Rg=0.775 SPS=8770 \n", "bl=76 pos[1]=[-6.3 -4.0 -0.1] dr=0.69 t=106.0ps kin=5.13 pot=6.20 Rg=0.804 SPS=8922 \n", "bl=77 pos[1]=[-6.1 -3.8 -0.6] dr=0.50 t=107.0ps kin=6.57 pot=6.13 Rg=0.596 SPS=8360 \n", "bl=78 pos[1]=[-6.3 -3.9 -1.4] dr=0.57 t=108.0ps kin=5.46 pot=6.38 Rg=0.440 SPS=8492 \n", "bl=79 pos[1]=[-6.9 -3.7 -1.6] dr=0.67 t=109.0ps kin=6.07 pot=6.93 Rg=0.430 SPS=8567 \n", "bl=80 pos[1]=[-7.3 -3.6 -2.7] dr=0.86 t=110.0ps kin=4.86 pot=6.89 Rg=0.531 SPS=8621 \n", "bl=81 pos[1]=[-7.3 -3.1 -2.9] dr=0.82 t=111.0ps kin=5.23 pot=7.06 Rg=0.498 SPS=8702 \n", "bl=82 pos[1]=[-7.0 -2.7 -3.2] dr=0.55 t=112.0ps kin=6.05 pot=7.02 Rg=0.477 SPS=8684 \n", "bl=83 pos[1]=[-6.8 -2.4 -2.9] dr=0.49 t=113.0ps kin=4.13 pot=6.67 Rg=0.406 SPS=8754 \n", "bl=84 pos[1]=[-7.9 -2.5 -3.4] dr=0.86 t=114.0ps kin=4.23 pot=7.06 Rg=0.410 SPS=8740 \n", "bl=85 pos[1]=[-7.9 -2.3 -3.3] dr=0.63 t=115.0ps kin=3.89 pot=7.38 Rg=0.496 SPS=8701 \n", "bl=86 pos[1]=[-8.0 -2.4 -3.2] dr=0.59 t=116.0ps kin=2.92 pot=7.54 Rg=0.611 SPS=8898 \n", "bl=87 pos[1]=[-8.0 -2.2 -3.4] dr=0.45 t=117.0ps kin=3.57 pot=7.70 Rg=0.791 SPS=8651 \n", "bl=88 pos[1]=[-8.5 -1.9 -2.6] dr=1.04 t=118.0ps kin=4.14 pot=8.09 Rg=0.879 SPS=8940 \n", "bl=89 pos[1]=[-9.2 -1.7 -3.1] dr=0.72 t=119.0ps kin=3.87 pot=8.01 Rg=0.643 SPS=9065 \n", "bl=90 pos[1]=[-9.6 -2.0 -3.3] dr=0.77 t=120.0ps kin=3.71 pot=8.50 Rg=0.759 SPS=8609 \n", "bl=91 pos[1]=[-9.9 -1.9 -2.7] dr=0.48 t=121.0ps kin=3.23 pot=8.31 Rg=0.616 SPS=8953 \n", "bl=92 pos[1]=[-10.3 -2.2 -3.6] dr=0.62 t=122.0ps kin=2.60 pot=8.64 Rg=0.559 SPS=8671 \n", "bl=93 pos[1]=[-10.5 -1.8 -3.0] dr=0.77 t=123.0ps kin=2.44 pot=8.60 Rg=0.711 SPS=8954 \n", "bl=94 pos[1]=[-10.8 -2.5 -2.9] dr=0.61 t=124.0ps kin=2.79 pot=8.43 Rg=0.412 SPS=8637 \n", "bl=95 pos[1]=[-10.7 -2.4 -2.6] dr=0.65 t=125.0ps kin=3.95 pot=8.89 Rg=0.578 SPS=8778 \n", "bl=96 pos[1]=[-10.7 -2.6 -3.5] dr=0.57 t=126.0ps kin=5.02 pot=9.36 Rg=0.823 SPS=8796 \n", "bl=97 pos[1]=[-10.8 -2.5 -2.2] dr=0.62 t=127.0ps kin=5.71 pot=9.22 Rg=0.897 SPS=8014 \n", "bl=98 pos[1]=[-10.5 -3.7 -2.3] dr=0.89 t=128.0ps kin=6.99 pot=9.75 Rg=1.023 SPS=7503 \n", "bl=99 pos[1]=[-11.3 -3.8 -2.8] dr=0.70 t=129.0ps kin=5.48 pot=9.72 Rg=0.653 SPS=7842 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [-11.6693655 -3.76013415 -3.52913654] Rg = 0.65312004\n", " median bond size is 0.2290878636694177\n", " three shortest/longest (<10)/ bonds are [0.07835139 0.17617395 0.20731799] [0.31495102 0.38001044 0.68796864]\n", " 95 percentile of distance to center is: 0.8599407829757514\n", " density of closest 95% monomers is: 3.5663943079826224\n", " density of the core monomers is: 1.6180429828063354\n", " min/median/mean/max coordinates are: \n", " x: -12.33, -11.57, -11.67, -11.15\n", " y: -3.94, -3.75, -3.76, -3.53\n", " z: -3.99, -3.67, -3.53, -2.77\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 5.478428732511492 should be: 1.5\n", " fastest particles are (in kT): [ 4.88943464 5.23413138 6.02967511 11.86918393 14.250708 ]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 9.717581176757813\n", "bl=100 pos[1]=[-11.6 -4.6 -2.7] dr=0.60 t=130.0ps kin=3.82 pot=10.00 Rg=0.693 SPS=8439 \n", "bl=101 pos[1]=[-11.7 -5.1 -2.5] dr=0.44 t=131.0ps kin=4.13 pot=10.19 Rg=0.795 SPS=8077 \n", "bl=102 pos[1]=[-11.5 -5.0 -2.8] dr=0.42 t=132.0ps kin=2.87 pot=10.05 Rg=0.748 SPS=7472 \n", "bl=103 pos[1]=[-11.3 -5.6 -3.8] dr=0.90 t=133.0ps kin=3.36 pot=10.43 Rg=0.795 SPS=7968 \n", "bl=104 pos[1]=[-11.4 -5.9 -3.8] dr=0.91 t=134.0ps kin=4.55 pot=10.78 Rg=0.522 SPS=7897 \n", "bl=105 pos[1]=[-11.4 -6.0 -3.8] dr=0.60 t=135.0ps kin=4.94 pot=10.77 Rg=0.399 SPS=7570 \n", "bl=106 pos[1]=[-11.7 -6.0 -4.0] dr=0.46 t=136.0ps kin=4.36 pot=10.88 Rg=0.310 SPS=8529 \n", "bl=107 pos[1]=[-11.8 -6.9 -4.3] dr=0.59 t=137.0ps kin=3.28 pot=11.15 Rg=0.455 SPS=8108 \n", "bl=108 pos[1]=[-11.7 -6.5 -4.5] dr=0.68 t=138.0ps kin=3.91 pot=11.31 Rg=0.404 SPS=8000 \n", "bl=109 pos[1]=[-12.1 -6.2 -4.2] dr=0.53 t=139.0ps kin=4.17 pot=11.15 Rg=0.630 SPS=8304 \n", "bl=110 pos[1]=[-12.4 -5.9 -5.1] dr=0.74 t=140.0ps kin=3.52 pot=11.25 Rg=0.831 SPS=8538 \n", "bl=111 pos[1]=[-12.2 -5.9 -5.2] dr=0.49 t=141.0ps kin=3.73 pot=11.25 Rg=0.843 SPS=8934 \n", "bl=112 pos[1]=[-12.3 -6.1 -4.3] dr=0.72 t=142.0ps kin=4.50 pot=10.93 Rg=0.905 SPS=8728 \n", "bl=113 pos[1]=[-12.3 -5.9 -5.5] dr=0.65 t=143.0ps kin=4.42 pot=11.36 Rg=1.113 SPS=8992 \n", "bl=114 pos[1]=[-11.7 -5.9 -5.3] dr=0.66 t=144.0ps kin=4.18 pot=11.36 Rg=0.980 SPS=8477 \n", "bl=115 pos[1]=[-11.5 -6.2 -5.3] dr=0.80 t=145.0ps kin=2.82 pot=11.73 Rg=1.060 SPS=8981 \n", "bl=116 pos[1]=[-10.3 -6.3 -5.7] dr=0.89 t=146.0ps kin=3.26 pot=11.29 Rg=0.684 SPS=8707 \n", "bl=117 pos[1]=[-10.6 -5.9 -4.4] dr=0.68 t=147.0ps kin=3.10 pot=11.00 Rg=0.614 SPS=8831 \n", "bl=118 pos[1]=[-10.9 -5.9 -4.4] dr=0.40 t=148.0ps kin=3.62 pot=11.28 Rg=0.844 SPS=8766 \n", "bl=119 pos[1]=[-11.0 -6.4 -5.0] dr=0.59 t=149.0ps kin=3.65 pot=11.41 Rg=0.864 SPS=8820 \n", "bl=120 pos[1]=[-11.4 -6.6 -5.3] dr=0.49 t=150.0ps kin=2.91 pot=11.55 Rg=0.913 SPS=8686 \n", "bl=121 pos[1]=[-10.5 -7.0 -5.5] dr=0.61 t=151.0ps kin=4.16 pot=11.48 Rg=0.846 SPS=8920 \n", "bl=122 pos[1]=[-10.2 -7.0 -5.5] dr=0.51 t=152.0ps kin=4.40 pot=11.18 Rg=0.784 SPS=8871 \n", "bl=123 pos[1]=[-9.8 -7.5 -6.1] dr=0.64 t=153.0ps kin=3.56 pot=11.34 Rg=0.884 SPS=8884 \n", "bl=124 pos[1]=[-9.0 -8.4 -5.5] dr=0.86 t=154.0ps kin=2.88 pot=11.30 Rg=0.752 SPS=8785 \n", "bl=125 pos[1]=[-8.7 -8.7 -5.1] dr=0.66 t=155.0ps kin=3.90 pot=11.31 Rg=0.687 SPS=8489 \n", "bl=126 pos[1]=[-8.8 -8.7 -5.4] dr=0.59 t=156.0ps kin=2.77 pot=11.24 Rg=0.766 SPS=8581 \n", "bl=127 pos[1]=[-8.9 -8.9 -4.9] dr=0.37 t=157.0ps kin=2.21 pot=11.23 Rg=0.772 SPS=8646 \n", "bl=128 pos[1]=[-8.2 -8.4 -4.7] dr=0.60 t=158.0ps kin=3.57 pot=10.79 Rg=0.778 SPS=8665 \n", "bl=129 pos[1]=[-8.3 -8.0 -5.1] dr=0.53 t=159.0ps kin=2.58 pot=10.93 Rg=0.554 SPS=8865 \n", "bl=130 pos[1]=[-9.4 -7.5 -5.3] dr=0.82 t=160.0ps kin=3.39 pot=10.67 Rg=0.616 SPS=8685 \n", "bl=131 pos[1]=[-9.2 -7.7 -4.6] dr=0.68 t=161.0ps kin=4.05 pot=10.29 Rg=0.789 SPS=8779 \n", "bl=132 pos[1]=[-8.2 -8.0 -4.7] dr=0.76 t=162.0ps kin=3.43 pot=10.28 Rg=0.833 SPS=9041 \n", "bl=133 pos[1]=[-8.1 -7.8 -5.0] dr=0.62 t=163.0ps kin=3.67 pot=9.90 Rg=0.847 SPS=8675 \n", "bl=134 pos[1]=[-7.7 -8.0 -4.5] dr=0.74 t=164.0ps kin=3.16 pot=9.67 Rg=1.020 SPS=8687 \n", "bl=135 pos[1]=[-7.8 -7.6 -4.0] dr=0.46 t=165.0ps kin=3.25 pot=9.66 Rg=0.798 SPS=8760 \n", "bl=136 pos[1]=[-7.9 -7.0 -4.7] dr=0.72 t=166.0ps kin=4.77 pot=9.73 Rg=0.559 SPS=8771 \n", "bl=137 pos[1]=[-7.5 -6.7 -5.0] dr=0.65 t=167.0ps kin=3.90 pot=9.72 Rg=0.618 SPS=8176 \n", "bl=138 pos[1]=[-7.8 -7.1 -6.0] dr=0.62 t=168.0ps kin=3.33 pot=10.09 Rg=0.749 SPS=7768 \n", "bl=139 pos[1]=[-6.8 -7.0 -5.3] dr=0.73 t=169.0ps kin=3.33 pot=9.77 Rg=0.824 SPS=8358 \n", "bl=140 pos[1]=[-6.6 -7.0 -5.3] dr=0.86 t=170.0ps kin=3.05 pot=9.62 Rg=0.623 SPS=8412 \n", "bl=141 pos[1]=[-6.2 -6.9 -4.7] dr=0.62 t=171.0ps kin=4.91 pot=9.59 Rg=0.788 SPS=8749 \n", "bl=142 pos[1]=[-6.2 -6.8 -4.9] dr=0.55 t=172.0ps kin=4.14 pot=9.42 Rg=0.687 SPS=8627 \n", "bl=143 pos[1]=[-6.4 -7.8 -5.4] dr=0.78 t=173.0ps kin=3.52 pot=9.99 Rg=0.741 SPS=8807 \n", "bl=144 pos[1]=[-7.3 -8.1 -5.4] dr=0.62 t=174.0ps kin=3.58 pot=9.87 Rg=0.710 SPS=8736 \n", "bl=145 pos[1]=[-6.9 -7.7 -5.9] dr=0.75 t=175.0ps kin=3.66 pot=10.24 Rg=0.651 SPS=8913 \n", "bl=146 pos[1]=[-6.9 -7.7 -5.9] dr=0.62 t=176.0ps kin=3.75 pot=10.44 Rg=0.496 SPS=8652 \n", "bl=147 pos[1]=[-7.0 -8.1 -6.1] dr=0.56 t=177.0ps kin=3.70 pot=10.53 Rg=0.386 SPS=8847 \n", "bl=148 pos[1]=[-6.9 -8.3 -6.6] dr=0.63 t=178.0ps kin=3.98 pot=10.68 Rg=0.487 SPS=8808 \n", "bl=149 pos[1]=[-6.9 -8.0 -6.6] dr=0.60 t=179.0ps kin=2.48 pot=10.69 Rg=0.427 SPS=8774 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [-6.82088323 -7.50743847 -6.68795452] Rg = 0.4274377\n", " median bond size is 0.2728078873850459\n", " three shortest/longest (<10)/ bonds are [0.11215107 0.1341288 0.20583282] [0.3524502 0.36537533 0.4069931 ]\n", " 95 percentile of distance to center is: 0.5868341187853655\n", " density of closest 95% monomers is: 11.222482273223775\n", " density of the core monomers is: 19.40923865788274\n", " min/median/mean/max coordinates are: \n", " x: -7.13, -6.85, -6.82, -6.54\n", " y: -8.08, -7.35, -7.51, -7.10\n", " z: -7.01, -6.63, -6.69, -6.41\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 2.483699793026253 should be: 1.5\n", " fastest particles are (in kT): [2.04613018 3.49250093 4.2438562 4.56766627 5.57791057]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 10.687487792968751\n", "bl=150 pos[1]=[-7.4 -8.3 -6.7] dr=0.54 t=180.0ps kin=2.55 pot=11.11 Rg=0.413 SPS=9017 \n", "bl=151 pos[1]=[-6.7 -7.6 -6.9] dr=0.58 t=181.0ps kin=2.92 pot=10.95 Rg=0.400 SPS=8790 \n", "bl=152 pos[1]=[-6.4 -7.9 -7.0] dr=0.52 t=182.0ps kin=4.86 pot=11.09 Rg=0.526 SPS=8676 \n", "bl=153 pos[1]=[-6.9 -7.6 -7.1] dr=0.82 t=183.0ps kin=3.33 pot=11.18 Rg=0.446 SPS=8637 \n", "bl=154 pos[1]=[-8.1 -7.5 -6.9] dr=0.90 t=184.0ps kin=3.70 pot=11.44 Rg=0.654 SPS=8592 \n", "bl=155 pos[1]=[-8.0 -7.6 -6.9] dr=0.57 t=185.0ps kin=4.94 pot=11.50 Rg=0.555 SPS=8735 \n", "bl=156 pos[1]=[-8.7 -7.1 -7.2] dr=0.66 t=186.0ps kin=4.42 pot=11.65 Rg=0.597 SPS=8932 \n", "bl=157 pos[1]=[-9.0 -7.0 -7.4] dr=0.74 t=187.0ps kin=3.29 pot=12.21 Rg=0.753 SPS=8720 \n", "bl=158 pos[1]=[-9.1 -6.8 -7.6] dr=0.47 t=188.0ps kin=3.36 pot=12.14 Rg=0.632 SPS=8936 \n", "bl=159 pos[1]=[-9.4 -7.4 -7.9] dr=0.56 t=189.0ps kin=4.86 pot=12.32 Rg=0.568 SPS=7975 \n", "bl=160 pos[1]=[-9.7 -7.0 -7.9] dr=0.81 t=190.0ps kin=4.27 pot=12.75 Rg=0.708 SPS=8499 \n", "bl=161 pos[1]=[-9.3 -7.3 -8.6] dr=0.62 t=191.0ps kin=4.43 pot=12.97 Rg=0.632 SPS=8702 \n", "bl=162 pos[1]=[-10.1 -7.6 -9.1] dr=0.61 t=192.0ps kin=4.43 pot=13.01 Rg=0.854 SPS=8941 \n", "bl=163 pos[1]=[-10.5 -8.1 -9.6] dr=0.90 t=193.0ps kin=4.03 pot=13.50 Rg=1.490 SPS=8691 \n", "bl=164 pos[1]=[-10.4 -7.7 -9.9] dr=0.60 t=194.0ps kin=5.04 pot=13.00 Rg=1.358 SPS=8793 \n", "bl=165 pos[1]=[-10.0 -6.8 -10.2] dr=0.80 t=195.0ps kin=4.96 pot=13.03 Rg=1.081 SPS=8873 \n", "bl=166 pos[1]=[-9.7 -6.8 -9.5] dr=0.49 t=196.0ps kin=5.06 pot=12.85 Rg=0.978 SPS=8703 \n", "bl=167 pos[1]=[-9.5 -7.0 -9.7] dr=0.63 t=197.0ps kin=4.54 pot=12.63 Rg=0.911 SPS=9041 \n", "bl=168 pos[1]=[-9.4 -7.0 -9.3] dr=0.70 t=198.0ps kin=4.33 pot=12.87 Rg=1.272 SPS=8666 \n", "bl=169 pos[1]=[-8.8 -6.3 -8.9] dr=0.64 t=199.0ps kin=4.69 pot=12.54 Rg=1.156 SPS=8783 \n", "bl=170 pos[1]=[-8.2 -6.7 -9.3] dr=0.50 t=200.0ps kin=3.92 pot=12.40 Rg=1.083 SPS=8960 \n", "bl=171 pos[1]=[-7.8 -6.5 -9.6] dr=0.83 t=201.0ps kin=3.11 pot=12.07 Rg=0.847 SPS=9090 \n", "bl=172 pos[1]=[-7.3 -6.3 -10.1] dr=0.69 t=202.0ps kin=4.05 pot=11.83 Rg=0.547 SPS=9007 \n", "bl=173 pos[1]=[-7.0 -5.2 -9.6] dr=0.95 t=203.0ps kin=3.52 pot=11.06 Rg=0.643 SPS=8860 \n", "bl=174 pos[1]=[-6.7 -4.9 -9.4] dr=0.54 t=204.0ps kin=4.55 pot=10.90 Rg=0.730 SPS=8716 \n", "bl=175 pos[1]=[-6.4 -5.0 -9.6] dr=0.68 t=205.0ps kin=3.58 pot=10.52 Rg=0.687 SPS=8770 \n", "bl=176 pos[1]=[-6.4 -4.9 -9.7] dr=0.77 t=206.0ps kin=4.89 pot=10.17 Rg=0.791 SPS=8478 \n", "bl=177 pos[1]=[-6.5 -4.3 -10.5] dr=0.66 t=207.0ps kin=6.39 pot=10.41 Rg=0.820 SPS=7717 \n", "bl=178 pos[1]=[-6.3 -4.7 -10.8] dr=0.69 t=208.0ps kin=5.16 pot=10.58 Rg=0.795 SPS=7589 \n", "bl=179 pos[1]=[-7.2 -5.1 -10.8] dr=0.79 t=209.0ps kin=4.82 pot=11.12 Rg=0.994 SPS=8405 \n", "bl=180 pos[1]=[-7.5 -5.2 -10.9] dr=0.50 t=210.0ps kin=5.86 pot=11.17 Rg=0.903 SPS=8493 \n", "bl=181 pos[1]=[-7.2 -5.4 -10.7] dr=0.69 t=211.0ps kin=6.43 pot=11.17 Rg=1.130 SPS=8970 \n", "bl=182 pos[1]=[-7.0 -5.3 -10.7] dr=0.52 t=212.0ps kin=5.85 pot=11.27 Rg=0.939 SPS=8771 \n", "bl=183 pos[1]=[-7.3 -5.7 -10.8] dr=0.73 t=213.0ps kin=3.85 pot=11.40 Rg=1.003 SPS=8741 \n", "bl=184 pos[1]=[-7.5 -5.4 -10.9] dr=0.88 t=214.0ps kin=3.51 pot=11.40 Rg=1.045 SPS=8750 \n", "bl=185 pos[1]=[-6.5 -5.3 -11.4] dr=0.70 t=215.0ps kin=4.05 pot=11.25 Rg=0.668 SPS=8777 \n", "bl=186 pos[1]=[-6.3 -5.0 -11.4] dr=0.48 t=216.0ps kin=2.97 pot=11.01 Rg=0.587 SPS=9078 \n", "bl=187 pos[1]=[-6.3 -4.1 -11.4] dr=0.69 t=217.0ps kin=4.14 pot=11.10 Rg=0.412 SPS=8699 \n", "bl=188 pos[1]=[-5.8 -3.9 -11.0] dr=0.55 t=218.0ps kin=4.36 pot=11.16 Rg=0.529 SPS=9099 \n", "bl=189 pos[1]=[-6.1 -4.2 -11.4] dr=0.75 t=219.0ps kin=5.34 pot=11.70 Rg=0.547 SPS=8713 \n", "bl=190 pos[1]=[-6.4 -5.1 -10.9] dr=0.77 t=220.0ps kin=4.45 pot=11.69 Rg=0.904 SPS=8757 \n", "bl=191 pos[1]=[-7.1 -4.5 -10.7] dr=0.55 t=221.0ps kin=4.01 pot=11.57 Rg=0.762 SPS=8964 \n", "bl=192 pos[1]=[-7.4 -4.9 -10.3] dr=0.59 t=222.0ps kin=4.21 pot=11.54 Rg=0.890 SPS=8456 \n", "bl=193 pos[1]=[-7.8 -4.7 -9.8] dr=0.49 t=223.0ps kin=3.76 pot=11.92 Rg=0.956 SPS=8736 \n", "bl=194 pos[1]=[-7.6 -5.2 -9.8] dr=0.61 t=224.0ps kin=3.36 pot=12.00 Rg=0.958 SPS=8698 \n", "bl=195 pos[1]=[-7.2 -4.7 -9.5] dr=0.53 t=225.0ps kin=3.35 pot=11.68 Rg=0.895 SPS=8780 \n", "bl=196 pos[1]=[-7.6 -4.6 -9.0] dr=0.64 t=226.0ps kin=3.40 pot=11.49 Rg=0.915 SPS=8714 \n", "bl=197 pos[1]=[-7.6 -5.0 -9.4] dr=0.72 t=227.0ps kin=2.65 pot=11.21 Rg=0.733 SPS=8862 \n", "bl=198 pos[1]=[-7.8 -4.5 -9.6] dr=0.45 t=228.0ps kin=3.44 pot=11.27 Rg=0.597 SPS=8672 \n", "bl=199 pos[1]=[-7.7 -4.4 -9.7] dr=0.74 t=229.0ps kin=4.96 pot=11.50 Rg=0.637 SPS=8774 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [-8.5616169 -4.05691307 -9.71910019] Rg = 0.6367024\n", " median bond size is 0.3957872159944983\n", " three shortest/longest (<10)/ bonds are [0.21130998 0.21727112 0.29695257] [0.40486586 0.42093309 0.58961049]\n", " 95 percentile of distance to center is: 0.9417336909333655\n", " density of closest 95% monomers is: 2.715505411951045\n", " density of the core monomers is: 4.113783843695203\n", " min/median/mean/max coordinates are: \n", " x: -9.10, -8.70, -8.56, -7.66\n", " y: -4.71, -4.07, -4.06, -3.62\n", " z: -10.30, -9.70, -9.72, -9.36\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 4.959772554216446 should be: 1.5\n", " fastest particles are (in kT): [4.86005697 4.97256635 6.36384215 6.9767307 8.77262691]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 11.497875213623047\n", "bl=200 pos[1]=[-8.0 -4.5 -8.9] dr=0.56 t=230.0ps kin=6.56 pot=11.59 Rg=0.793 SPS=8716 \n", "bl=201 pos[1]=[-8.5 -5.0 -9.1] dr=0.77 t=231.0ps kin=5.89 pot=11.87 Rg=1.020 SPS=8960 \n", "bl=202 pos[1]=[-8.4 -5.5 -8.4] dr=0.63 t=232.0ps kin=6.09 pot=11.51 Rg=1.127 SPS=8577 \n", "bl=203 pos[1]=[-9.0 -5.4 -7.7] dr=0.76 t=233.0ps kin=5.01 pot=11.61 Rg=1.087 SPS=7812 \n", "bl=204 pos[1]=[-8.7 -4.7 -7.5] dr=0.71 t=234.0ps kin=4.60 pot=11.38 Rg=0.907 SPS=7845 \n", "bl=205 pos[1]=[-9.0 -5.0 -7.2] dr=0.59 t=235.0ps kin=3.77 pot=11.54 Rg=1.157 SPS=8219 \n", "bl=206 pos[1]=[-9.7 -5.5 -7.8] dr=0.72 t=236.0ps kin=3.41 pot=11.82 Rg=1.087 SPS=8531 \n", "bl=207 pos[1]=[-10.2 -5.5 -7.6] dr=0.60 t=237.0ps kin=3.81 pot=11.76 Rg=0.820 SPS=8783 \n", "bl=208 pos[1]=[-10.1 -5.6 -7.0] dr=0.62 t=238.0ps kin=3.53 pot=11.95 Rg=0.825 SPS=8750 \n", "bl=209 pos[1]=[-10.5 -5.2 -7.0] dr=0.61 t=239.0ps kin=3.77 pot=11.84 Rg=0.677 SPS=8676 \n", "bl=210 pos[1]=[-10.4 -6.0 -6.9] dr=1.02 t=240.0ps kin=3.34 pot=12.22 Rg=0.803 SPS=8616 \n", "bl=211 pos[1]=[-10.0 -6.1 -7.2] dr=0.62 t=241.0ps kin=3.27 pot=12.29 Rg=0.825 SPS=8743 \n", "bl=212 pos[1]=[-9.9 -5.9 -7.4] dr=0.46 t=242.0ps kin=2.92 pot=12.35 Rg=0.888 SPS=8891 \n", "bl=213 pos[1]=[-10.1 -6.7 -7.2] dr=0.72 t=243.0ps kin=5.24 pot=12.51 Rg=0.832 SPS=8732 \n", "bl=214 pos[1]=[-10.8 -6.1 -6.6] dr=0.94 t=244.0ps kin=6.76 pot=12.74 Rg=0.649 SPS=8777 \n", "bl=215 pos[1]=[-11.7 -5.7 -7.0] dr=0.72 t=245.0ps kin=5.25 pot=12.56 Rg=0.457 SPS=8762 \n", "bl=216 pos[1]=[-12.0 -5.7 -6.4] dr=0.66 t=246.0ps kin=3.63 pot=12.42 Rg=0.261 SPS=8696 \n", "bl=217 pos[1]=[-11.6 -5.3 -6.0] dr=0.56 t=247.0ps kin=4.13 pot=12.36 Rg=0.573 SPS=8452 \n", "bl=218 pos[1]=[-11.6 -5.9 -6.5] dr=0.65 t=248.0ps kin=3.55 pot=12.35 Rg=0.395 SPS=8338 \n", "bl=219 pos[1]=[-11.1 -6.6 -6.0] dr=0.69 t=249.0ps kin=2.88 pot=12.66 Rg=0.606 SPS=8862 \n", "bl=220 pos[1]=[-10.6 -6.0 -6.3] dr=0.82 t=250.0ps kin=3.00 pot=12.81 Rg=0.765 SPS=8700 \n", "bl=221 pos[1]=[-11.2 -5.1 -7.0] dr=0.75 t=251.0ps kin=3.74 pot=13.09 Rg=0.992 SPS=8627 \n", "bl=222 pos[1]=[-11.1 -5.2 -7.0] dr=0.54 t=252.0ps kin=2.93 pot=12.97 Rg=0.862 SPS=8884 \n", "bl=223 pos[1]=[-12.2 -5.4 -7.0] dr=0.78 t=253.0ps kin=3.82 pot=13.17 Rg=0.593 SPS=8780 \n", "bl=224 pos[1]=[-12.1 -6.0 -7.4] dr=0.63 t=254.0ps kin=4.10 pot=13.17 Rg=0.448 SPS=8754 \n", "bl=225 pos[1]=[-11.8 -6.3 -7.7] dr=0.66 t=255.0ps kin=3.45 pot=13.21 Rg=0.402 SPS=8817 \n", "bl=226 pos[1]=[-12.4 -6.0 -7.9] dr=0.51 t=256.0ps kin=3.43 pot=13.33 Rg=0.429 SPS=8640 \n", "bl=227 pos[1]=[-11.7 -6.2 -7.9] dr=0.88 t=257.0ps kin=3.47 pot=12.76 Rg=0.506 SPS=9079 \n", "bl=228 pos[1]=[-11.6 -5.7 -8.1] dr=0.78 t=258.0ps kin=3.23 pot=12.53 Rg=0.697 SPS=8756 \n", "bl=229 pos[1]=[-11.6 -5.7 -9.0] dr=0.77 t=259.0ps kin=3.77 pot=12.45 Rg=0.927 SPS=8950 \n", "bl=230 pos[1]=[-11.0 -5.1 -8.3] dr=0.68 t=260.0ps kin=3.28 pot=11.90 Rg=0.672 SPS=8786 \n", "bl=231 pos[1]=[-10.6 -4.9 -8.4] dr=0.57 t=261.0ps kin=1.92 pot=11.94 Rg=0.748 SPS=8968 \n", "bl=232 pos[1]=[-9.7 -5.3 -8.7] dr=0.78 t=262.0ps kin=1.82 pot=11.72 Rg=0.490 SPS=8782 \n", "bl=233 pos[1]=[-9.3 -5.3 -9.8] dr=0.83 t=263.0ps kin=2.16 pot=11.82 Rg=0.647 SPS=8805 \n", "bl=234 pos[1]=[-9.2 -5.0 -9.0] dr=0.58 t=264.0ps kin=3.25 pot=11.55 Rg=0.442 SPS=9014 \n", "bl=235 pos[1]=[-9.5 -5.1 -10.1] dr=0.55 t=265.0ps kin=3.34 pot=11.70 Rg=0.722 SPS=8845 \n", "bl=236 pos[1]=[-8.6 -4.5 -9.7] dr=0.63 t=266.0ps kin=4.42 pot=11.32 Rg=0.646 SPS=8774 \n", "bl=237 pos[1]=[-9.3 -5.4 -9.8] dr=0.81 t=267.0ps kin=3.40 pot=11.86 Rg=0.986 SPS=9021 \n", "bl=238 pos[1]=[-9.4 -5.5 -9.8] dr=0.59 t=268.0ps kin=3.58 pot=11.83 Rg=0.834 SPS=8654 \n", "bl=239 pos[1]=[-9.7 -4.9 -9.5] dr=0.71 t=269.0ps kin=2.88 pot=11.74 Rg=0.814 SPS=8820 \n", "bl=240 pos[1]=[-9.9 -4.3 -9.3] dr=0.69 t=270.0ps kin=1.90 pot=11.69 Rg=0.440 SPS=8966 \n", "bl=241 pos[1]=[-10.3 -4.7 -9.9] dr=0.55 t=271.0ps kin=2.93 pot=12.10 Rg=0.408 SPS=8817 \n", "bl=242 pos[1]=[-10.2 -4.0 -9.2] dr=0.75 t=272.0ps kin=3.17 pot=11.97 Rg=0.503 SPS=9002 \n", "bl=243 pos[1]=[-10.1 -4.4 -9.3] dr=0.72 t=273.0ps kin=3.98 pot=11.54 Rg=0.532 SPS=8580 \n", "bl=244 pos[1]=[-10.4 -4.5 -8.5] dr=0.64 t=274.0ps kin=3.58 pot=11.80 Rg=0.390 SPS=8623 \n", "bl=245 pos[1]=[-10.4 -4.2 -9.0] dr=0.53 t=275.0ps kin=3.63 pot=11.98 Rg=0.420 SPS=7829 \n", "bl=246 pos[1]=[-10.3 -4.5 -8.6] dr=0.60 t=276.0ps kin=3.21 pot=11.83 Rg=0.406 SPS=7772 \n", "bl=247 pos[1]=[-10.2 -4.1 -8.7] dr=0.42 t=277.0ps kin=2.90 pot=11.63 Rg=0.450 SPS=8413 \n", "bl=248 pos[1]=[-11.1 -4.0 -9.1] dr=0.49 t=278.0ps kin=3.98 pot=11.63 Rg=0.511 SPS=8684 \n", "bl=249 pos[1]=[-11.0 -4.3 -7.8] dr=0.97 t=279.0ps kin=3.50 pot=11.56 Rg=0.800 SPS=8980 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [-10.4594903 -3.83772054 -8.16871872] Rg = 0.79989004\n", " median bond size is 0.3026642386826154\n", " three shortest/longest (<10)/ bonds are [0.13822635 0.20094276 0.27603895] [0.42819588 0.48072175 0.65386942]\n", " 95 percentile of distance to center is: 1.2738780717178375\n", " density of closest 95% monomers is: 1.097113124705863\n", " density of the core monomers is: 13.557885674028837\n", " min/median/mean/max coordinates are: \n", " x: -10.98, -10.65, -10.46, -9.64\n", " y: -4.35, -4.00, -3.84, -3.06\n", " z: -8.95, -8.09, -8.17, -7.61\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 3.502574610084163 should be: 1.5\n", " fastest particles are (in kT): [3.26750747 4.13017533 4.85604577 8.90375692 9.75589561]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 11.558139038085939\n", "bl=250 pos[1]=[-10.8 -4.1 -7.3] dr=0.61 t=280.0ps kin=3.74 pot=11.34 Rg=0.516 SPS=8712 \n", "bl=251 pos[1]=[-10.5 -4.0 -7.2] dr=0.61 t=281.0ps kin=3.97 pot=11.21 Rg=0.348 SPS=8832 \n", "bl=252 pos[1]=[-10.7 -4.1 -7.7] dr=0.69 t=282.0ps kin=6.63 pot=11.55 Rg=0.524 SPS=8753 \n", "bl=253 pos[1]=[-10.3 -3.5 -7.8] dr=0.56 t=283.0ps kin=5.74 pot=11.48 Rg=0.425 SPS=9047 \n", "bl=254 pos[1]=[-10.0 -3.8 -8.2] dr=0.77 t=284.0ps kin=6.09 pot=11.08 Rg=0.345 SPS=8830 \n", "bl=255 pos[1]=[-9.6 -3.9 -8.3] dr=0.78 t=285.0ps kin=4.90 pot=10.80 Rg=0.408 SPS=8946 \n", "bl=256 pos[1]=[-9.3 -3.7 -7.7] dr=0.61 t=286.0ps kin=4.83 pot=10.55 Rg=0.488 SPS=8946 \n", "bl=257 pos[1]=[-8.5 -3.6 -7.8] dr=0.70 t=287.0ps kin=5.44 pot=10.35 Rg=0.312 SPS=8822 \n", "bl=258 pos[1]=[-8.2 -3.7 -7.7] dr=0.58 t=288.0ps kin=4.12 pot=10.20 Rg=0.350 SPS=8941 \n", "bl=259 pos[1]=[-7.8 -3.7 -7.5] dr=0.88 t=289.0ps kin=4.05 pot=10.03 Rg=0.484 SPS=8957 \n", "bl=260 pos[1]=[-7.2 -3.6 -7.0] dr=0.59 t=290.0ps kin=4.27 pot=9.77 Rg=0.623 SPS=8704 \n", "bl=261 pos[1]=[-7.8 -3.2 -7.0] dr=0.47 t=291.0ps kin=3.93 pot=9.87 Rg=0.792 SPS=9065 \n", "bl=262 pos[1]=[-8.0 -2.6 -7.2] dr=0.49 t=292.0ps kin=4.27 pot=9.77 Rg=0.893 SPS=8969 \n", "bl=263 pos[1]=[-7.9 -2.8 -7.6] dr=0.52 t=293.0ps kin=4.73 pot=9.71 Rg=0.785 SPS=8853 \n", "bl=264 pos[1]=[-7.6 -2.7 -7.5] dr=0.35 t=294.0ps kin=4.04 pot=9.46 Rg=0.636 SPS=8673 \n", "bl=265 pos[1]=[-7.0 -2.8 -7.7] dr=0.61 t=295.0ps kin=4.17 pot=9.74 Rg=0.590 SPS=8882 \n", "bl=266 pos[1]=[-7.7 -3.4 -7.7] dr=0.61 t=296.0ps kin=3.40 pot=9.71 Rg=0.822 SPS=9039 \n", "bl=267 pos[1]=[-7.6 -3.4 -8.7] dr=0.65 t=297.0ps kin=3.11 pot=9.82 Rg=0.693 SPS=8850 \n", "bl=268 pos[1]=[-7.0 -4.8 -8.9] dr=0.71 t=298.0ps kin=2.70 pot=10.19 Rg=0.789 SPS=8772 \n", "bl=269 pos[1]=[-6.8 -3.8 -9.3] dr=0.70 t=299.0ps kin=3.54 pot=10.33 Rg=0.472 SPS=8710 \n", "bl=270 pos[1]=[-6.8 -4.3 -9.6] dr=0.86 t=300.0ps kin=2.81 pot=10.69 Rg=0.731 SPS=8786 \n", "bl=271 pos[1]=[-6.8 -3.9 -10.0] dr=0.71 t=301.0ps kin=2.13 pot=10.77 Rg=0.420 SPS=8722 \n", "bl=272 pos[1]=[-7.2 -3.9 -10.4] dr=0.64 t=302.0ps kin=3.21 pot=11.05 Rg=0.664 SPS=8825 \n", "bl=273 pos[1]=[-7.9 -3.7 -10.3] dr=0.81 t=303.0ps kin=3.80 pot=10.59 Rg=0.737 SPS=8818 \n", "bl=274 pos[1]=[-7.4 -3.9 -10.2] dr=0.49 t=304.0ps kin=3.19 pot=10.65 Rg=0.921 SPS=8750 \n", "bl=275 pos[1]=[-7.2 -3.9 -10.7] dr=0.76 t=305.0ps kin=3.55 pot=10.79 Rg=0.866 SPS=8939 \n", "bl=276 pos[1]=[-7.7 -3.9 -10.9] dr=0.57 t=306.0ps kin=4.01 pot=10.87 Rg=1.187 SPS=8727 \n", "bl=277 pos[1]=[-7.9 -4.0 -11.4] dr=0.80 t=307.0ps kin=4.36 pot=11.54 Rg=1.146 SPS=8678 \n", "bl=278 pos[1]=[-7.4 -3.1 -12.3] dr=1.01 t=308.0ps kin=5.84 pot=11.41 Rg=0.683 SPS=8802 \n", "bl=279 pos[1]=[-8.0 -2.7 -13.1] dr=0.90 t=309.0ps kin=4.78 pot=11.78 Rg=0.551 SPS=8975 \n", "bl=280 pos[1]=[-7.2 -3.3 -13.4] dr=0.59 t=310.0ps kin=4.18 pot=11.71 Rg=0.582 SPS=9024 \n", "bl=281 pos[1]=[-7.5 -2.1 -13.4] dr=0.85 t=311.0ps kin=3.64 pot=11.73 Rg=0.496 SPS=8842 \n", "bl=282 pos[1]=[-7.5 -2.1 -13.7] dr=0.67 t=312.0ps kin=2.84 pot=11.95 Rg=0.519 SPS=8833 \n", "bl=283 pos[1]=[-7.8 -2.0 -14.5] dr=0.62 t=313.0ps kin=2.95 pot=12.04 Rg=0.669 SPS=8698 \n", "bl=284 pos[1]=[-7.3 -2.0 -14.8] dr=0.65 t=314.0ps kin=3.59 pot=12.41 Rg=0.704 SPS=8940 \n", "bl=285 pos[1]=[-7.1 -2.0 -14.9] dr=0.51 t=315.0ps kin=3.54 pot=12.40 Rg=0.910 SPS=8717 \n", "bl=286 pos[1]=[-8.0 -1.9 -15.1] dr=0.66 t=316.0ps kin=2.89 pot=12.35 Rg=0.870 SPS=8694 \n", "bl=287 pos[1]=[-7.1 -1.8 -15.3] dr=0.55 t=317.0ps kin=3.27 pot=12.22 Rg=0.942 SPS=8698 \n", "bl=288 pos[1]=[-6.9 -1.6 -15.1] dr=0.64 t=318.0ps kin=4.43 pot=12.27 Rg=1.023 SPS=9026 \n", "bl=289 pos[1]=[-6.8 -0.6 -15.4] dr=0.73 t=319.0ps kin=5.76 pot=12.32 Rg=0.908 SPS=8805 \n", "bl=290 pos[1]=[-7.2 -0.4 -14.9] dr=0.81 t=320.0ps kin=4.49 pot=11.94 Rg=0.482 SPS=8913 \n", "bl=291 pos[1]=[-6.8 -0.7 -15.0] dr=0.78 t=321.0ps kin=3.19 pot=11.93 Rg=0.453 SPS=8595 \n", "bl=292 pos[1]=[-7.1 -1.0 -14.8] dr=0.59 t=322.0ps kin=2.40 pot=12.10 Rg=0.465 SPS=8690 \n", "bl=293 pos[1]=[-8.0 -1.3 -14.7] dr=0.78 t=323.0ps kin=2.27 pot=12.61 Rg=0.775 SPS=8658 \n", "bl=294 pos[1]=[-7.6 -2.2 -15.2] dr=0.78 t=324.0ps kin=1.83 pot=12.92 Rg=0.608 SPS=8692 \n", "bl=295 pos[1]=[-8.1 -2.2 -15.9] dr=0.62 t=325.0ps kin=2.78 pot=13.11 Rg=0.596 SPS=8780 \n", "bl=296 pos[1]=[-8.2 -1.9 -16.2] dr=0.69 t=326.0ps kin=2.91 pot=13.65 Rg=0.678 SPS=8665 \n", "bl=297 pos[1]=[-8.4 -2.0 -16.4] dr=0.56 t=327.0ps kin=2.58 pot=13.61 Rg=0.753 SPS=8722 \n", "bl=298 pos[1]=[-7.7 -2.6 -16.6] dr=0.54 t=328.0ps kin=2.68 pot=13.57 Rg=0.716 SPS=8690 \n", "bl=299 pos[1]=[-7.8 -2.9 -17.1] dr=0.67 t=329.0ps kin=3.47 pot=13.57 Rg=0.770 SPS=8681 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [ -6.9570581 -2.07691833 -17.46098576] Rg = 0.7699985\n", " median bond size is 0.3846091488148675\n", " three shortest/longest (<10)/ bonds are [0.06967954 0.19571746 0.22984745] [0.42773662 0.45362855 0.65423995]\n", " 95 percentile of distance to center is: 1.1236539676747523\n", " density of closest 95% monomers is: 1.5985904974651821\n", " density of the core monomers is: 12.181893131569245\n", " min/median/mean/max coordinates are: \n", " x: -7.77, -6.86, -6.96, -6.36\n", " y: -2.91, -2.05, -2.08, -1.47\n", " z: -18.01, -17.47, -17.46, -16.90\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 3.4704621021467426 should be: 1.5\n", " fastest particles are (in kT): [3.06574961 4.06743248 4.39896676 6.1819497 7.19053327]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 13.570306396484376\n", "bl=300 pos[1]=[-7.3 -2.3 -17.4] dr=0.63 t=330.0ps kin=3.88 pot=13.57 Rg=0.380 SPS=8689 \n", "bl=301 pos[1]=[-7.5 -2.5 -17.5] dr=0.57 t=331.0ps kin=3.33 pot=13.81 Rg=0.495 SPS=8201 \n", "bl=302 pos[1]=[-7.5 -2.1 -16.9] dr=0.59 t=332.0ps kin=3.46 pot=13.84 Rg=0.760 SPS=8549 \n", "bl=303 pos[1]=[-6.5 -2.5 -16.8] dr=0.66 t=333.0ps kin=2.43 pot=13.79 Rg=0.765 SPS=8913 \n", "bl=304 pos[1]=[-6.8 -1.8 -17.3] dr=0.70 t=334.0ps kin=3.78 pot=13.65 Rg=0.618 SPS=8615 \n", "bl=305 pos[1]=[-6.1 -2.6 -17.2] dr=0.73 t=335.0ps kin=3.13 pot=13.22 Rg=0.651 SPS=8659 \n", "bl=306 pos[1]=[-5.9 -1.5 -17.3] dr=0.72 t=336.0ps kin=3.37 pot=13.04 Rg=0.648 SPS=8958 \n", "bl=307 pos[1]=[-6.0 -1.9 -17.7] dr=0.71 t=337.0ps kin=3.13 pot=13.08 Rg=0.610 SPS=8667 \n", "bl=308 pos[1]=[-5.6 -2.1 -18.0] dr=0.89 t=338.0ps kin=5.31 pot=13.06 Rg=0.624 SPS=8397 \n", "bl=309 pos[1]=[-4.7 -2.1 -18.8] dr=0.93 t=339.0ps kin=4.86 pot=12.84 Rg=0.496 SPS=8928 \n", "bl=310 pos[1]=[-4.7 -2.5 -19.9] dr=0.85 t=340.0ps kin=4.09 pot=13.02 Rg=0.568 SPS=8629 \n", "bl=311 pos[1]=[-4.0 -2.6 -21.2] dr=0.86 t=341.0ps kin=4.40 pot=13.30 Rg=0.517 SPS=8782 \n", "bl=312 pos[1]=[-3.8 -1.7 -20.3] dr=0.76 t=342.0ps kin=4.30 pot=13.04 Rg=0.539 SPS=8862 \n", "bl=313 pos[1]=[-3.0 -1.2 -20.4] dr=0.89 t=343.0ps kin=4.37 pot=12.82 Rg=0.476 SPS=8989 \n", "bl=314 pos[1]=[-3.0 -0.6 -20.9] dr=0.51 t=344.0ps kin=3.88 pot=13.01 Rg=0.636 SPS=8711 \n", "bl=315 pos[1]=[-3.4 -1.0 -21.2] dr=0.62 t=345.0ps kin=3.94 pot=13.07 Rg=0.513 SPS=8890 \n", "bl=316 pos[1]=[-3.0 -0.9 -20.8] dr=0.55 t=346.0ps kin=4.44 pot=13.25 Rg=0.477 SPS=8849 \n", "bl=317 pos[1]=[-3.8 -1.3 -20.8] dr=1.05 t=347.0ps kin=4.57 pot=14.01 Rg=0.513 SPS=8756 \n", "bl=318 pos[1]=[-3.5 -1.5 -21.9] dr=0.75 t=348.0ps kin=3.83 pot=14.25 Rg=0.516 SPS=8904 \n", "bl=319 pos[1]=[-4.5 -1.5 -23.0] dr=0.75 t=349.0ps kin=2.73 pot=14.46 Rg=0.336 SPS=8768 \n", "bl=320 pos[1]=[-4.1 -1.7 -22.9] dr=0.57 t=350.0ps kin=2.76 pot=14.41 Rg=0.262 SPS=8847 \n", "bl=321 pos[1]=[-4.2 -1.7 -23.2] dr=0.53 t=351.0ps kin=3.12 pot=14.70 Rg=0.330 SPS=8987 \n", "bl=322 pos[1]=[-4.1 -1.8 -24.2] dr=0.72 t=352.0ps kin=3.50 pot=15.07 Rg=0.398 SPS=8325 \n", "bl=323 pos[1]=[-4.2 -2.7 -23.4] dr=0.69 t=353.0ps kin=2.22 pot=15.41 Rg=0.627 SPS=8682 \n", "bl=324 pos[1]=[-4.5 -2.6 -23.8] dr=0.47 t=354.0ps kin=2.45 pot=15.34 Rg=0.432 SPS=8744 \n", "bl=325 pos[1]=[-4.5 -2.1 -23.5] dr=0.60 t=355.0ps kin=2.36 pot=15.27 Rg=0.337 SPS=8620 \n", "bl=326 pos[1]=[-4.3 -2.3 -23.3] dr=0.59 t=356.0ps kin=3.01 pot=15.43 Rg=0.406 SPS=8187 \n", "bl=327 pos[1]=[-4.1 -2.6 -24.1] dr=0.88 t=357.0ps kin=3.32 pot=15.71 Rg=0.537 SPS=8506 \n", "bl=328 pos[1]=[-4.2 -2.7 -23.5] dr=0.68 t=358.0ps kin=4.05 pot=15.74 Rg=0.403 SPS=8987 \n", "bl=329 pos[1]=[-4.3 -2.8 -23.9] dr=0.59 t=359.0ps kin=3.86 pot=15.95 Rg=0.453 SPS=8908 \n", "bl=330 pos[1]=[-4.5 -2.8 -23.4] dr=0.61 t=360.0ps kin=2.93 pot=16.38 Rg=0.639 SPS=8447 \n", "bl=331 pos[1]=[-4.9 -2.1 -23.9] dr=0.99 t=361.0ps kin=4.03 pot=15.82 Rg=0.533 SPS=9007 \n", "bl=332 pos[1]=[-4.5 -2.0 -23.8] dr=0.50 t=362.0ps kin=3.41 pot=15.46 Rg=0.536 SPS=8564 \n", "bl=333 pos[1]=[-4.1 -2.1 -24.3] dr=0.51 t=363.0ps kin=2.48 pot=15.51 Rg=0.623 SPS=8895 \n", "bl=334 pos[1]=[-4.1 -1.9 -24.2] dr=0.84 t=364.0ps kin=3.05 pot=14.96 Rg=0.777 SPS=8844 \n", "bl=335 pos[1]=[-2.9 -1.6 -24.4] dr=0.76 t=365.0ps kin=3.31 pot=14.71 Rg=0.580 SPS=9045 \n", "bl=336 pos[1]=[-3.4 -1.6 -23.8] dr=0.54 t=366.0ps kin=2.28 pot=14.39 Rg=0.440 SPS=8761 \n", "bl=337 pos[1]=[-2.7 -1.4 -22.7] dr=0.76 t=367.0ps kin=2.98 pot=14.51 Rg=0.601 SPS=8865 \n", "bl=338 pos[1]=[-2.7 -1.9 -23.0] dr=0.70 t=368.0ps kin=2.88 pot=14.69 Rg=0.555 SPS=8854 \n", "bl=339 pos[1]=[-3.5 -2.0 -23.9] dr=0.62 t=369.0ps kin=2.90 pot=15.01 Rg=0.455 SPS=9010 \n", "bl=340 pos[1]=[-3.7 -2.7 -23.5] dr=0.62 t=370.0ps kin=3.87 pot=15.25 Rg=0.341 SPS=8780 \n", "bl=341 pos[1]=[-3.9 -3.5 -23.7] dr=0.54 t=371.0ps kin=5.11 pot=15.46 Rg=0.364 SPS=8835 \n", "bl=342 pos[1]=[-4.6 -2.5 -23.5] dr=0.82 t=372.0ps kin=4.99 pot=15.50 Rg=0.604 SPS=8590 \n", "bl=343 pos[1]=[-4.4 -2.7 -23.1] dr=0.49 t=373.0ps kin=3.83 pot=15.57 Rg=0.654 SPS=8972 \n", "bl=344 pos[1]=[-5.1 -2.6 -23.8] dr=0.64 t=374.0ps kin=4.36 pot=15.65 Rg=0.739 SPS=8369 \n", "bl=345 pos[1]=[-5.0 -3.0 -24.1] dr=0.64 t=375.0ps kin=4.59 pot=15.62 Rg=0.588 SPS=8883 \n", "bl=346 pos[1]=[-4.8 -2.7 -23.5] dr=0.54 t=376.0ps kin=4.04 pot=15.72 Rg=0.372 SPS=8802 \n", "bl=347 pos[1]=[-4.8 -3.0 -22.7] dr=0.85 t=377.0ps kin=4.01 pot=15.49 Rg=0.304 SPS=9060 \n", "bl=348 pos[1]=[-4.5 -2.6 -23.3] dr=0.55 t=378.0ps kin=2.24 pot=15.47 Rg=0.455 SPS=8478 \n", "bl=349 pos[1]=[-4.7 -3.0 -22.9] dr=0.75 t=379.0ps kin=3.66 pot=15.29 Rg=0.677 SPS=8877 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [ -4.74920974 -2.77802436 -22.48913288] Rg = 0.6768085\n", " median bond size is 0.2989124361455544\n", " three shortest/longest (<10)/ bonds are [0.19539162 0.21329073 0.21400585] [0.39466932 0.52073099 0.52660154]\n", " 95 percentile of distance to center is: 0.948579731888487\n", " density of closest 95% monomers is: 2.6571341017828782\n", " density of the core monomers is: 7.666077833382917\n", " min/median/mean/max coordinates are: \n", " x: -4.95, -4.80, -4.75, -4.45\n", " y: -3.40, -2.90, -2.78, -1.98\n", " z: -22.95, -22.62, -22.49, -21.77\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 3.6605388313841636 should be: 1.5\n", " fastest particles are (in kT): [3.77285172 4.5262635 5.47088405 5.69470256 7.50751067]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 15.290472412109375\n", "bl=350 pos[1]=[-5.5 -3.0 -22.0] dr=0.95 t=380.0ps kin=4.16 pot=15.56 Rg=0.796 SPS=8983 \n", "bl=351 pos[1]=[-5.9 -3.2 -21.9] dr=0.72 t=381.0ps kin=4.50 pot=15.79 Rg=0.710 SPS=8579 \n", "bl=352 pos[1]=[-5.8 -3.2 -21.6] dr=0.67 t=382.0ps kin=3.96 pot=15.54 Rg=0.501 SPS=8945 \n", "bl=353 pos[1]=[-6.3 -3.2 -22.0] dr=0.47 t=383.0ps kin=4.33 pot=15.99 Rg=0.509 SPS=8763 \n", "bl=354 pos[1]=[-6.5 -2.1 -21.9] dr=0.82 t=384.0ps kin=4.86 pot=15.79 Rg=0.467 SPS=8856 \n", "bl=355 pos[1]=[-7.0 -2.0 -21.4] dr=0.86 t=385.0ps kin=5.59 pot=15.49 Rg=0.497 SPS=8820 \n", "bl=356 pos[1]=[-7.4 -2.8 -21.3] dr=0.52 t=386.0ps kin=4.25 pot=15.51 Rg=0.503 SPS=8062 \n", "bl=357 pos[1]=[-7.7 -2.4 -20.8] dr=0.54 t=387.0ps kin=4.38 pot=15.54 Rg=0.476 SPS=8996 \n", "bl=358 pos[1]=[-7.6 -1.8 -20.5] dr=0.65 t=388.0ps kin=3.96 pot=15.33 Rg=0.441 SPS=8985 \n", "bl=359 pos[1]=[-7.8 -1.1 -19.8] dr=0.88 t=389.0ps kin=4.36 pot=15.15 Rg=0.622 SPS=9067 \n", "bl=360 pos[1]=[-8.4 -1.2 -18.9] dr=0.97 t=390.0ps kin=4.00 pot=14.85 Rg=0.933 SPS=8504 \n", "bl=361 pos[1]=[-8.3 -0.9 -18.7] dr=0.76 t=391.0ps kin=4.37 pot=14.73 Rg=0.944 SPS=8796 \n", "bl=362 pos[1]=[-8.8 -1.4 -19.3] dr=0.64 t=392.0ps kin=3.99 pot=14.91 Rg=0.830 SPS=8940 \n", "bl=363 pos[1]=[-8.8 -0.5 -19.7] dr=0.63 t=393.0ps kin=4.02 pot=14.81 Rg=0.778 SPS=8728 \n", "bl=364 pos[1]=[-8.8 -0.4 -20.4] dr=0.48 t=394.0ps kin=3.30 pot=14.95 Rg=0.752 SPS=8854 \n", "bl=365 pos[1]=[-9.1 -0.9 -19.6] dr=0.80 t=395.0ps kin=3.00 pot=14.79 Rg=0.427 SPS=8482 \n", "bl=366 pos[1]=[-9.4 -1.1 -19.7] dr=0.43 t=396.0ps kin=3.57 pot=14.92 Rg=0.354 SPS=8819 \n", "bl=367 pos[1]=[-8.7 -0.9 -19.6] dr=0.48 t=397.0ps kin=3.37 pot=14.97 Rg=0.281 SPS=8738 \n", "bl=368 pos[1]=[-8.7 -0.7 -19.3] dr=0.46 t=398.0ps kin=3.80 pot=14.74 Rg=0.385 SPS=8935 \n", "bl=369 pos[1]=[-8.4 -1.1 -18.8] dr=0.82 t=399.0ps kin=3.08 pot=15.18 Rg=0.899 SPS=8713 \n", "bl=370 pos[1]=[-8.1 -0.5 -18.6] dr=0.76 t=400.0ps kin=4.69 pot=14.97 Rg=0.871 SPS=8899 \n", "bl=371 pos[1]=[-9.2 -0.3 -18.5] dr=0.77 t=401.0ps kin=4.40 pot=15.03 Rg=0.688 SPS=8854 \n", "bl=372 pos[1]=[-9.5 -0.4 -18.1] dr=0.69 t=402.0ps kin=5.97 pot=14.68 Rg=0.592 SPS=8528 \n", "bl=373 pos[1]=[-8.5 -0.4 -17.9] dr=0.85 t=403.0ps kin=5.22 pot=14.14 Rg=0.603 SPS=9021 \n", "bl=374 pos[1]=[-8.8 -0.8 -17.0] dr=0.68 t=404.0ps kin=6.38 pot=14.28 Rg=0.894 SPS=8848 \n", "bl=375 pos[1]=[-8.5 -0.1 -16.7] dr=0.60 t=405.0ps kin=6.40 pot=13.83 Rg=0.848 SPS=8717 \n", "bl=376 pos[1]=[-7.4 0.4 -17.0] dr=1.01 t=406.0ps kin=4.55 pot=13.21 Rg=0.619 SPS=8921 \n", "bl=377 pos[1]=[-8.4 1.0 -17.3] dr=0.65 t=407.0ps kin=4.11 pot=13.29 Rg=0.539 SPS=8211 \n", "bl=378 pos[1]=[-8.3 0.6 -17.7] dr=0.48 t=408.0ps kin=3.75 pot=13.19 Rg=0.451 SPS=8871 \n", "bl=379 pos[1]=[-8.5 0.2 -17.6] dr=0.90 t=409.0ps kin=4.80 pot=13.79 Rg=0.589 SPS=9010 \n", "bl=380 pos[1]=[-8.1 0.2 -17.7] dr=0.53 t=410.0ps kin=3.61 pot=13.66 Rg=0.801 SPS=8974 \n", "bl=381 pos[1]=[-8.6 0.6 -18.2] dr=0.60 t=411.0ps kin=4.42 pot=13.55 Rg=0.701 SPS=9023 \n", "bl=382 pos[1]=[-8.8 1.0 -17.7] dr=0.68 t=412.0ps kin=5.75 pot=13.45 Rg=0.718 SPS=8545 \n", "bl=383 pos[1]=[-8.3 1.3 -18.1] dr=0.54 t=413.0ps kin=4.45 pot=13.95 Rg=0.888 SPS=8880 \n", "bl=384 pos[1]=[-8.4 2.0 -18.1] dr=0.98 t=414.0ps kin=4.15 pot=13.83 Rg=0.949 SPS=8949 \n", "bl=385 pos[1]=[-8.5 1.9 -18.5] dr=0.50 t=415.0ps kin=3.64 pot=13.64 Rg=0.785 SPS=9044 \n", "bl=386 pos[1]=[-8.2 1.7 -17.9] dr=0.77 t=416.0ps kin=3.28 pot=13.17 Rg=0.698 SPS=8730 \n", "bl=387 pos[1]=[-8.7 1.7 -17.2] dr=0.62 t=417.0ps kin=3.61 pot=12.95 Rg=0.586 SPS=8881 \n", "bl=388 pos[1]=[-8.9 1.6 -17.5] dr=0.56 t=418.0ps kin=3.35 pot=12.85 Rg=0.409 SPS=9010 \n", "bl=389 pos[1]=[-9.3 2.6 -17.5] dr=0.72 t=419.0ps kin=3.58 pot=12.76 Rg=0.403 SPS=8401 \n", "bl=390 pos[1]=[-9.9 2.6 -16.3] dr=0.70 t=420.0ps kin=3.74 pot=12.84 Rg=0.538 SPS=8732 \n", "bl=391 pos[1]=[-9.8 1.8 -16.6] dr=0.62 t=421.0ps kin=4.33 pot=13.08 Rg=0.594 SPS=8751 \n", "bl=392 pos[1]=[-10.1 1.4 -16.3] dr=0.76 t=422.0ps kin=4.17 pot=13.37 Rg=0.718 SPS=8472 \n", "bl=393 pos[1]=[-10.3 1.8 -16.0] dr=0.69 t=423.0ps kin=2.80 pot=13.50 Rg=0.645 SPS=8995 \n", "bl=394 pos[1]=[-10.6 1.7 -16.3] dr=0.73 t=424.0ps kin=3.10 pot=13.86 Rg=0.634 SPS=8691 \n", "bl=395 pos[1]=[-10.0 1.7 -16.2] dr=0.69 t=425.0ps kin=4.02 pot=14.08 Rg=0.954 SPS=9132 \n", "bl=396 pos[1]=[-10.5 0.7 -16.7] dr=0.81 t=426.0ps kin=4.87 pot=13.47 Rg=0.391 SPS=8306 \n", "bl=397 pos[1]=[-9.5 1.2 -16.6] dr=0.70 t=427.0ps kin=6.31 pot=13.10 Rg=0.516 SPS=9112 \n", "bl=398 pos[1]=[-8.3 1.2 -17.2] dr=0.73 t=428.0ps kin=4.56 pot=13.17 Rg=0.863 SPS=8692 \n", "bl=399 pos[1]=[-8.1 -0.1 -17.3] dr=0.98 t=429.0ps kin=4.04 pot=13.49 Rg=0.816 SPS=8275 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [-9.24929199e+00 4.68029212e-03 -1.68227570e+01] Rg = 0.81600845\n", " median bond size is 0.3156951985452715\n", " three shortest/longest (<10)/ bonds are [0.21112407 0.22013005 0.25008355] [0.43194624 0.58942245 0.87153261]\n", " 95 percentile of distance to center is: 1.2066041299419954\n", " density of closest 95% monomers is: 1.2910426024195374\n", " density of the core monomers is: 3.137301104939283\n", " min/median/mean/max coordinates are: \n", " x: -10.28, -8.95, -9.25, -8.10\n", " y: -0.35, -0.03, 0.00, 0.37\n", " z: -17.27, -16.93, -16.82, -16.28\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 4.0439508026924 should be: 1.5\n", " fastest particles are (in kT): [ 3.03522292 3.23582706 6.87122308 6.87513162 12.11280547]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 13.486607360839844\n", "bl=400 pos[1]=[-7.7 -0.7 -16.4] dr=0.87 t=430.0ps kin=3.54 pot=13.31 Rg=0.733 SPS=8689 \n", "bl=401 pos[1]=[-7.1 -0.6 -17.2] dr=0.68 t=431.0ps kin=4.00 pot=13.08 Rg=0.971 SPS=8673 \n", "bl=402 pos[1]=[-7.4 -0.9 -17.8] dr=1.01 t=432.0ps kin=3.26 pot=12.69 Rg=0.781 SPS=8663 \n", "bl=403 pos[1]=[-6.6 -0.6 -17.7] dr=0.59 t=433.0ps kin=4.09 pot=12.40 Rg=0.611 SPS=8633 \n", "bl=404 pos[1]=[-6.0 -1.1 -18.0] dr=0.78 t=434.0ps kin=4.23 pot=12.63 Rg=0.641 SPS=8824 \n", "bl=405 pos[1]=[-6.1 -1.6 -17.5] dr=0.67 t=435.0ps kin=4.02 pot=12.87 Rg=0.648 SPS=8854 \n", "bl=406 pos[1]=[-5.6 -1.1 -18.0] dr=0.57 t=436.0ps kin=3.91 pot=12.87 Rg=0.596 SPS=8606 \n", "bl=407 pos[1]=[-5.1 -1.3 -17.7] dr=0.74 t=437.0ps kin=3.35 pot=12.88 Rg=0.697 SPS=8769 \n", "bl=408 pos[1]=[-5.1 -0.9 -17.4] dr=0.54 t=438.0ps kin=2.83 pot=12.63 Rg=0.600 SPS=8807 \n", "bl=409 pos[1]=[-5.5 0.3 -17.2] dr=0.68 t=439.0ps kin=2.64 pot=12.59 Rg=0.805 SPS=8921 \n", "bl=410 pos[1]=[-5.8 -0.6 -17.1] dr=0.68 t=440.0ps kin=2.71 pot=12.34 Rg=0.636 SPS=8855 \n", "bl=411 pos[1]=[-6.2 -0.9 -17.2] dr=0.60 t=441.0ps kin=4.35 pot=12.57 Rg=0.757 SPS=8924 \n", "bl=412 pos[1]=[-5.7 -0.8 -16.8] dr=0.52 t=442.0ps kin=3.43 pot=12.23 Rg=0.736 SPS=9063 \n", "bl=413 pos[1]=[-5.1 -0.9 -17.0] dr=0.63 t=443.0ps kin=3.44 pot=12.13 Rg=0.710 SPS=8733 \n", "bl=414 pos[1]=[-4.8 -0.4 -16.4] dr=0.62 t=444.0ps kin=3.82 pot=11.75 Rg=0.674 SPS=8630 \n", "bl=415 pos[1]=[-4.8 -0.3 -16.7] dr=0.40 t=445.0ps kin=3.34 pot=11.67 Rg=0.698 SPS=9060 \n", "bl=416 pos[1]=[-5.1 0.7 -16.8] dr=0.82 t=446.0ps kin=3.79 pot=12.12 Rg=0.760 SPS=8725 \n", "bl=417 pos[1]=[-5.4 -0.3 -16.1] dr=0.88 t=447.0ps kin=3.53 pot=11.54 Rg=0.515 SPS=8995 \n", "bl=418 pos[1]=[-5.5 0.1 -16.1] dr=0.65 t=448.0ps kin=3.31 pot=11.13 Rg=0.494 SPS=8408 \n", "bl=419 pos[1]=[-6.1 0.2 -16.1] dr=0.76 t=449.0ps kin=3.43 pot=11.33 Rg=0.565 SPS=8870 \n", "bl=420 pos[1]=[-5.7 0.6 -16.1] dr=0.60 t=450.0ps kin=4.76 pot=11.11 Rg=0.428 SPS=8874 \n", "bl=421 pos[1]=[-5.6 0.7 -15.7] dr=0.61 t=451.0ps kin=3.49 pot=11.06 Rg=0.594 SPS=8892 \n", "bl=422 pos[1]=[-5.4 1.1 -15.1] dr=0.51 t=452.0ps kin=4.57 pot=10.81 Rg=0.543 SPS=8728 \n", "bl=423 pos[1]=[-5.7 0.9 -15.9] dr=0.70 t=453.0ps kin=2.60 pot=10.93 Rg=0.415 SPS=9052 \n", "bl=424 pos[1]=[-4.9 -0.2 -16.2] dr=0.71 t=454.0ps kin=3.45 pot=10.85 Rg=0.390 SPS=8810 \n", "bl=425 pos[1]=[-5.0 -0.0 -16.0] dr=0.53 t=455.0ps kin=2.29 pot=10.94 Rg=0.644 SPS=8867 \n", "bl=426 pos[1]=[-5.4 0.4 -16.4] dr=0.65 t=456.0ps kin=2.81 pot=11.19 Rg=0.611 SPS=8682 \n", "bl=427 pos[1]=[-4.7 0.7 -16.8] dr=0.52 t=457.0ps kin=4.06 pot=11.25 Rg=0.879 SPS=8668 \n", "bl=428 pos[1]=[-5.2 0.8 -16.9] dr=0.75 t=458.0ps kin=4.36 pot=11.26 Rg=0.597 SPS=9039 \n", "bl=429 pos[1]=[-5.0 0.5 -16.3] dr=0.73 t=459.0ps kin=4.27 pot=11.12 Rg=0.577 SPS=8645 \n", "bl=430 pos[1]=[-5.3 0.7 -16.4] dr=0.64 t=460.0ps kin=4.41 pot=10.87 Rg=0.424 SPS=8647 \n", "bl=431 pos[1]=[-5.2 0.5 -16.5] dr=0.54 t=461.0ps kin=2.29 pot=10.61 Rg=0.421 SPS=9061 \n", "bl=432 pos[1]=[-5.3 0.4 -16.9] dr=0.72 t=462.0ps kin=1.74 pot=10.55 Rg=0.708 SPS=8815 \n", "bl=433 pos[1]=[-5.1 0.8 -16.7] dr=0.90 t=463.0ps kin=2.84 pot=10.22 Rg=0.488 SPS=9016 \n", "bl=434 pos[1]=[-5.5 0.9 -16.7] dr=0.65 t=464.0ps kin=2.00 pot=10.46 Rg=0.537 SPS=8285 \n", "bl=435 pos[1]=[-4.4 0.6 -16.3] dr=0.85 t=465.0ps kin=2.61 pot=9.99 Rg=0.450 SPS=9021 \n", "bl=436 pos[1]=[-4.8 1.1 -16.6] dr=0.51 t=466.0ps kin=2.56 pot=9.95 Rg=0.247 SPS=8641 \n", "bl=437 pos[1]=[-5.1 1.3 -16.4] dr=0.46 t=467.0ps kin=2.13 pot=10.26 Rg=0.483 SPS=8826 \n", "bl=438 pos[1]=[-5.3 1.3 -16.2] dr=0.59 t=468.0ps kin=2.30 pot=10.46 Rg=0.702 SPS=9060 \n", "bl=439 pos[1]=[-5.1 1.3 -15.5] dr=0.81 t=469.0ps kin=3.31 pot=10.25 Rg=0.860 SPS=8042 \n", "bl=440 pos[1]=[-5.0 1.4 -15.6] dr=0.60 t=470.0ps kin=3.55 pot=9.84 Rg=0.721 SPS=8436 \n", "bl=441 pos[1]=[-4.8 2.0 -16.3] dr=0.60 t=471.0ps kin=4.48 pot=9.91 Rg=0.652 SPS=9022 \n", "bl=442 pos[1]=[-4.0 2.2 -16.3] dr=0.76 t=472.0ps kin=4.23 pot=9.87 Rg=0.595 SPS=8958 \n", "bl=443 pos[1]=[-3.0 2.0 -17.9] dr=1.01 t=473.0ps kin=3.53 pot=10.32 Rg=0.994 SPS=8784 \n", "bl=444 pos[1]=[-3.8 2.0 -17.5] dr=0.63 t=474.0ps kin=3.09 pot=10.52 Rg=0.982 SPS=8932 \n", "bl=445 pos[1]=[-3.3 1.6 -17.4] dr=0.58 t=475.0ps kin=2.87 pot=10.23 Rg=0.801 SPS=8850 \n", "bl=446 pos[1]=[-3.6 1.8 -17.7] dr=0.42 t=476.0ps kin=3.03 pot=10.26 Rg=0.699 SPS=8519 \n", "bl=447 pos[1]=[-3.2 1.6 -17.7] dr=0.63 t=477.0ps kin=2.62 pot=10.07 Rg=0.547 SPS=8831 \n", "bl=448 pos[1]=[-3.4 2.4 -17.3] dr=0.59 t=478.0ps kin=3.02 pot=9.77 Rg=0.669 SPS=9094 \n", "bl=449 pos[1]=[-3.4 1.5 -16.4] dr=0.71 t=479.0ps kin=4.42 pot=9.83 Rg=0.395 SPS=8639 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [ -3.36345565 1.21985627 -16.87211704] Rg = 0.39454287\n", " median bond size is 0.3842564318687674\n", " three shortest/longest (<10)/ bonds are [0.16260213 0.19316801 0.19575652] [0.43907618 0.45354976 0.57944568]\n", " 95 percentile of distance to center is: 0.5350407463409294\n", " density of closest 95% monomers is: 14.807250524458647\n", " density of the core monomers is: 15.212422000844722\n", " min/median/mean/max coordinates are: \n", " x: -3.73, -3.44, -3.36, -3.11\n", " y: 0.97, 1.17, 1.22, 1.54\n", " z: -17.26, -16.83, -16.87, -16.36\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 4.422873201247623 should be: 1.5\n", " fastest particles are (in kT): [4.31831137 6.61352599 6.78292078 8.14318957 9.08868905]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 9.8281982421875\n", "bl=450 pos[1]=[-2.8 0.9 -16.7] dr=0.77 t=480.0ps kin=4.68 pot=10.10 Rg=0.424 SPS=8643 \n", "bl=451 pos[1]=[-3.4 0.7 -16.9] dr=0.63 t=481.0ps kin=5.00 pot=10.25 Rg=0.402 SPS=9143 \n", "bl=452 pos[1]=[-2.8 -0.2 -16.3] dr=0.77 t=482.0ps kin=4.15 pot=10.57 Rg=0.724 SPS=8524 \n", "bl=453 pos[1]=[-2.3 -0.6 -16.2] dr=0.63 t=483.0ps kin=5.34 pot=10.79 Rg=0.936 SPS=8974 \n", "bl=454 pos[1]=[-2.2 -0.0 -17.1] dr=0.90 t=484.0ps kin=4.55 pot=10.49 Rg=0.561 SPS=8614 \n", "bl=455 pos[1]=[-2.3 0.4 -17.8] dr=0.68 t=485.0ps kin=4.56 pot=10.41 Rg=0.392 SPS=8666 \n", "bl=456 pos[1]=[-1.8 0.4 -17.0] dr=0.83 t=486.0ps kin=5.58 pot=10.31 Rg=0.501 SPS=8850 \n", "bl=457 pos[1]=[-2.0 0.4 -17.9] dr=0.52 t=487.0ps kin=3.64 pot=10.17 Rg=0.457 SPS=9128 \n", "bl=458 pos[1]=[-2.3 0.7 -18.0] dr=0.66 t=488.0ps kin=2.96 pot=10.32 Rg=0.444 SPS=8707 \n", "bl=459 pos[1]=[-2.2 1.1 -17.6] dr=0.81 t=489.0ps kin=3.82 pot=9.58 Rg=0.548 SPS=8666 \n", "bl=460 pos[1]=[-2.5 1.0 -17.4] dr=0.46 t=490.0ps kin=3.16 pot=9.90 Rg=0.524 SPS=8799 \n", "bl=461 pos[1]=[-2.6 1.1 -16.9] dr=0.66 t=491.0ps kin=3.02 pot=9.43 Rg=0.450 SPS=8414 \n", "bl=462 pos[1]=[-3.0 1.3 -17.0] dr=0.79 t=492.0ps kin=3.72 pot=9.20 Rg=0.558 SPS=8780 \n", "bl=463 pos[1]=[-3.4 1.8 -16.4] dr=0.85 t=493.0ps kin=3.09 pot=9.52 Rg=0.537 SPS=8800 \n", "bl=464 pos[1]=[-3.4 1.8 -16.9] dr=0.49 t=494.0ps kin=2.90 pot=9.25 Rg=0.566 SPS=8799 \n", "bl=465 pos[1]=[-3.3 2.2 -15.8] dr=0.94 t=495.0ps kin=2.57 pot=9.42 Rg=0.823 SPS=8110 \n", "bl=466 pos[1]=[-3.4 2.4 -15.7] dr=0.54 t=496.0ps kin=3.58 pot=9.47 Rg=0.992 SPS=8872 \n", "bl=467 pos[1]=[-3.7 3.2 -15.8] dr=0.63 t=497.0ps kin=3.38 pot=9.32 Rg=0.970 SPS=9070 \n", "bl=468 pos[1]=[-3.4 3.3 -15.4] dr=0.72 t=498.0ps kin=3.76 pot=8.91 Rg=1.074 SPS=9097 \n", "bl=469 pos[1]=[-2.9 3.3 -15.3] dr=0.59 t=499.0ps kin=2.56 pot=8.83 Rg=1.211 SPS=8032 \n", "bl=470 pos[1]=[-2.7 2.9 -15.4] dr=0.56 t=500.0ps kin=3.02 pot=8.73 Rg=0.927 SPS=8178 \n", "bl=471 pos[1]=[-2.9 3.2 -15.3] dr=0.54 t=501.0ps kin=3.37 pot=8.59 Rg=0.997 SPS=8240 \n", "bl=472 pos[1]=[-3.3 2.0 -15.3] dr=0.78 t=502.0ps kin=4.78 pot=9.15 Rg=0.999 SPS=8574 \n", "bl=473 pos[1]=[-3.4 2.5 -15.6] dr=0.60 t=503.0ps kin=3.74 pot=9.06 Rg=0.824 SPS=9052 \n", "bl=474 pos[1]=[-3.8 2.0 -15.4] dr=0.55 t=504.0ps kin=3.82 pot=9.17 Rg=0.838 SPS=8789 \n", "bl=475 pos[1]=[-4.3 1.7 -15.5] dr=0.75 t=505.0ps kin=3.62 pot=9.58 Rg=0.682 SPS=8895 \n", "bl=476 pos[1]=[-3.7 2.6 -15.6] dr=0.73 t=506.0ps kin=4.37 pot=9.18 Rg=0.699 SPS=7879 \n", "bl=477 pos[1]=[-3.8 2.2 -16.1] dr=0.48 t=507.0ps kin=4.35 pot=9.26 Rg=0.574 SPS=8235 \n", "bl=478 pos[1]=[-4.3 2.8 -16.2] dr=0.77 t=508.0ps kin=3.21 pot=9.37 Rg=0.753 SPS=8693 \n", "bl=479 pos[1]=[-4.9 3.0 -16.4] dr=0.57 t=509.0ps kin=2.95 pot=9.09 Rg=0.716 SPS=8887 \n", "bl=480 pos[1]=[-4.6 2.8 -16.5] dr=0.59 t=510.0ps kin=3.72 pot=9.37 Rg=0.818 SPS=8602 \n", "bl=481 pos[1]=[-4.7 2.8 -16.1] dr=0.52 t=511.0ps kin=3.24 pot=8.89 Rg=0.460 SPS=9097 \n", "bl=482 pos[1]=[-3.8 3.1 -16.2] dr=0.87 t=512.0ps kin=2.98 pot=8.88 Rg=0.298 SPS=8982 \n", "bl=483 pos[1]=[-3.5 3.0 -15.6] dr=0.51 t=513.0ps kin=2.61 pot=9.01 Rg=0.478 SPS=8244 \n", "bl=484 pos[1]=[-3.1 3.3 -15.8] dr=0.57 t=514.0ps kin=2.49 pot=8.58 Rg=0.559 SPS=8796 \n", "bl=485 pos[1]=[-3.0 3.6 -15.6] dr=0.71 t=515.0ps kin=3.17 pot=8.46 Rg=0.467 SPS=8985 \n", "bl=486 pos[1]=[-3.7 3.7 -16.2] dr=0.50 t=516.0ps kin=2.78 pot=8.47 Rg=0.457 SPS=8917 \n", "bl=487 pos[1]=[-3.6 3.6 -16.3] dr=0.67 t=517.0ps kin=3.15 pot=8.49 Rg=0.536 SPS=9059 \n", "bl=488 pos[1]=[-3.5 3.1 -16.1] dr=0.68 t=518.0ps kin=4.88 pot=8.50 Rg=0.829 SPS=8624 \n", "bl=489 pos[1]=[-3.2 4.0 -15.8] dr=0.81 t=519.0ps kin=3.84 pot=8.29 Rg=0.649 SPS=7971 \n", "bl=490 pos[1]=[-3.3 4.2 -16.2] dr=0.69 t=520.0ps kin=3.76 pot=8.02 Rg=0.506 SPS=8754 \n", "bl=491 pos[1]=[-3.1 4.5 -16.6] dr=0.42 t=521.0ps kin=5.14 pot=8.14 Rg=0.504 SPS=8608 \n", "bl=492 pos[1]=[-3.4 4.9 -16.0] dr=0.59 t=522.0ps kin=4.02 pot=8.06 Rg=0.657 SPS=8906 \n", "bl=493 pos[1]=[-3.1 4.6 -16.3] dr=0.63 t=523.0ps kin=3.74 pot=8.35 Rg=0.621 SPS=8214 \n", "bl=494 pos[1]=[-2.9 4.5 -16.6] dr=0.67 t=524.0ps kin=3.34 pot=8.16 Rg=0.468 SPS=8960 \n", "bl=495 pos[1]=[-3.4 4.4 -17.6] dr=0.67 t=525.0ps kin=2.69 pot=8.10 Rg=0.491 SPS=8917 \n", "bl=496 pos[1]=[-3.0 4.7 -17.4] dr=0.61 t=526.0ps kin=3.33 pot=8.13 Rg=0.627 SPS=8328 \n", "bl=497 pos[1]=[-2.8 4.2 -17.5] dr=0.64 t=527.0ps kin=3.72 pot=8.15 Rg=0.609 SPS=9020 \n", "bl=498 pos[1]=[-3.1 3.9 -17.1] dr=0.60 t=528.0ps kin=3.24 pot=8.13 Rg=0.475 SPS=8863 \n", "bl=499 pos[1]=[-3.6 4.1 -16.4] dr=0.69 t=529.0ps kin=3.91 pot=8.12 Rg=0.795 SPS=8753 \n", "\n", "Statistics for the simulation active_Rouse_sim, number of particles: 10, number of chains: 1\n", "\n", "Statistics for particle position\n", " mean position is: [ -2.47716504 3.65138638 -16.65024223] Rg = 0.795313\n", " median bond size is 0.4209681207354708\n", " three shortest/longest (<10)/ bonds are [0.13492316 0.17139959 0.21711373] [0.51791027 0.52394512 0.54103503]\n", " 95 percentile of distance to center is: 1.1945790582981135\n", " density of closest 95% monomers is: 1.3304247175121318\n", " density of the core monomers is: 2.6692225971358483\n", " min/median/mean/max coordinates are: \n", " x: -3.63, -2.16, -2.48, -1.78\n", " y: 2.85, 3.73, 3.65, 4.10\n", " z: -16.91, -16.70, -16.65, -16.35\n", "\n", "Statistics for velocities:\n", " mean kinetic energy is: 3.914693554708942 should be: 1.5\n", " fastest particles are (in kT): [ 2.92848127 3.30493509 3.3941556 7.45132754 13.9429566 ]\n", "\n", "Statistics for the system:\n", " Forces are: ['ActiveForce', 'HarmonicBond']\n", " Number of exceptions: 9\n", "\n", "Potential Energy Ep = 8.116238403320313\n", "bl=500 pos[1]=[-2.8 3.9 -16.1] dr=0.49 t=530.0ps kin=3.70 pot=8.03 Rg=0.608 SPS=8727 \n", "(501, 10, 3)\n" ] } ], "source": [ "# For the purpose of the tutorial we will just store the data in the xyz array for plotting\n", "# you may instead save the data into cndb/ndb/pdb files and load into numpy arrays using cndbtools\n", "# if you would like to save the data uncomment the lines below\n", "\n", "# sim.initStorage(filename=\"active_Rouse_sim\"\") # initiate storage\n", "\n", "xyz = [sim.getPositions()]\n", "\n", "n_blocks = 500 # number of simulation blocks\n", "block_size = 1000 # size of each block\n", "\n", "for _ in range(int(n_blocks)):\n", " sim.runSimBlock(int(block_size), increment=True)\n", " # sim.saveStructure()\n", " xyz.append(sim.getPositions())\n", " \n", "# sim.saveStructure(filename='lastframe',mode='ndb')\n", "# sim.storage[0].close()\n", "\n", "xyz = np.array(xyz)\n", "print(xyz.shape) # the shape should be: (number of blocks, number of monos, deg. of freedom)\n" ] }, { "attachments": {}, "cell_type": "markdown", "metadata": {}, "source": [ "##### Visualize trajectory" ] }, { "cell_type": "code", "execution_count": 7, "metadata": {}, "outputs": [ { "data": { "application/vnd.jupyter.widget-view+json": { "model_id": "4575ca3d728b4a7db3b8e61cae498c54", "version_major": 2, "version_minor": 0 }, "image/png": 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", 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