High magnetic Field white dwarfs exceeding Chandrashekhar Mass Limit

In winter last year, I studied the effects of high magnetic field on Astrophysical objects ,specially related to the mass of a white dwarf.The origin of high magnetic field is stated briefly by http://www.iiap.res.in/meet/chandra/Chandra_files/Tout.pdf. Where it is briefly discussed about the origin of such high magnetic field white dwarfs and observational statistics.
In the article about super chadrasheker supernova from WD,they state that”Chandrasekhar’s 1931 model of stellar collapse was elegant and powerful; it won him the Nobel Prize,” says Nugent. “But it was a simple one-dimensional model. Just by adding rotation one can exceed the Chandrasekhar mass, as he himself recognized.”

Some readups on the topic/news are:

In my analysis, I used quantized hall effect-like phenomena for the relativistic electron degeneracy pressure, and calculated the mass limit analytically.As a function of the residual magnetic field, the mass of white dwarf seemed to exceed the chandrashekhar mass limit.
here is my analysis: http://arxiv.org/abs/1204.1463v1
here is the computational (more detailed) analysis of the problem by my guides PhD student later.


TIPS for preparing input file for Molecular dymnamics simulations using DL_POLY

DL_POLY is a classical Molecular dynamics software by http://simx.epfl.ch/simx/en/dl_poly.html

,which is tweaked to work best with large macro molecules.It best simulates Organic molecules and thus is of use in pharmaceutical purpose of drug design etc

The preparation of the input file i.e the CONFIG file is one of the most troublesome episodes that I had.

Firstly, use aten to prepare the basic setup box.You can read throught their manual ,but the disorder button didnt work much for me from the GUI.I had to write script, i.e. use it from commandline to make the disorder work.

Check the output file,such that the output is in sequence,i.e. it follows some definite pattern.

Ensure that you dont have molecules towards the edges of the box, if you are usin periodic boundary condition, as these will culminate in errors during simulation.

If the resulting CONFIG is not in sequence, adjust some molecules and regenerate file again.Check using a program that you have ordering/pattern
as you need to specify the pattern in your FORCE file.

once this is done identify the pattern and write the FORCE field file, with the parameters of potential appropriately chosen from different models(CHARAMM, AMBER,etc etc.)

DL_POLY a quick user guide-Installation to first simulation in Molecular Dynamics

This summer I spend my time in Ecole Centrale Paris, trying to run a computer simulation on NPLIN.I will post about that later, but this was my first introduction to molecular dynamics simulation,  and there I faced many problems.So I thought to write up a bit, in case it might be of help for someone in future.I am posting this , but you sure can find help from the DISCO forums.And yes, read through the manual!!

In this, I explain how we can run DL_POLY in parallel.It really did a 30 minuite simulation in 30 seconds in my 4X2 core processor in laptop

1.Download DL_POLY_4 from ftp://ftp.dl.ac.uk/ccp5/DL_POLY/
2.Obtain Liscense by mailing the authors for home/personal/educational use
4.In Linux install open mpi by typing
$ sudo apt-get install libopenmpi-dev openmpi-bin openmpi-doc
$ sudo apt-get install ssh
Generate keys and add to ssh
$ ssh-keygen -t dsa
$ cat id_dsa.pub >> authorized_keys

Test program:
#include <stdio.h>
#include <mpi.h>

int main(int argc, char** argv)

int myrank, nprocs;

MPI_Init(&argc, &argv);
MPI_Comm_size(MPI_COMM_WORLD, &nprocs);
MPI_Comm_rank(MPI_COMM_WORLD, &myrank);
for (;;){
printf(“Hello from processor %d of %d\n”, myrank, nprocs);
return 0;

$ mpicc MPI_Hello.c -o MPI_Hello
$ mpiexec -n 5 MPI_Hello         #specify to run on 5 processors,press Ctrl+Z to exit
You can install htop to see if the process is really parallel [sudo apt-get install htop]
Compiling DL_POLY for Laptop Dell XPS 15z
Requires fortran to be installed.[sudo apt-get install gfortran]
1.In the DL_POLY directory>Build>copy “Makefile_MPI” to source directory and rename to “make”
2.In terminal type “sudo make hpc”
3.The process will create a DLPOLY.Z in the execute directory. Which also has a JAVA gui which can be used.(Personally I find using GUI a bit cumbersome and problematic,so I run using terminal)
4. Terminal >browse to DL_POLY execcute directory> type $./gui to invoke gui

Running sample scripts:
Some example and basic examples can be found online in

Although they used GUI, I am going to use a mixture of both

DLPOLY requires some necessary files to run a simulation,The CONTROL,CONFIG,FIELD files.I am going to explain them as we go,but first lets see if its working!
Download the files for EXERCISE 1 which finds out the phase transition for KCl.
The CONFIG file lists the system in brief,it gives the coordinates and velocities of all atoms in the system in initial condition.
The CONTROL file is important,it determins the thermodynamics of the system.The temperature, pressure, cutoff, and configuration like NVT,NPT etc.
FIELD defines any other field which cannot be characterised by concrete mathematical formulas

The CONFIG file uses its own self-consistent set of units.

physical quantity symbol unit value
time t0 1×10−12 seconds (picoseconds)
length l0 1×10−10 metres (Angstroms)
mass m0 1.66054×10−27 kilograms (amu)
charge q0 1.60218×10−19 Coulombs (electron charge)
energy E0=m0(l0/t0)2 1.66054×10−23 Joules = 10 J mol−1
pressure p0=E0/l30 1.66054×107 Pascal = 166.054 bar
Planck constant 6.35078E0t0
Boltzmann constant kB 0.83145E0/K

The others can be found from the user manual(Page 7 of DL_POLY_4_USER_MANUAL)

will learn the process through a process through the first example of DL_POLY guide.i.e. phase transition of KCl


This exercise studies a well-known phase transition in potassium chloride using constant pressure molecular dynamics. The objective is to develop the best practice in using such algorithms and to learn how phase transitions can be induced, detected and monitored in a simulation.

The CONFIG file:

DL_POLY: Potassium Chloride Test Case                                           #heading
2         3      2000    0.5000000000E-02

!levcfg(0-2,2 :position,velocity,forces included in file)

! imcon(periodic boundary condition:0,1,2,3,6)

!megatm(total number of particles)

!crystallographic information for periodic boundary(x,y,z component of a,b,c cell vector)

18.6960000000        0.0000000000        0.0000000000
0.0000000000       18.6960000000        0.0000000000
0.0000000000        0.0000000000       18.6960000000
!since levcfg = 2 each record will contain 3 data position,veocity,force
K+               1                            #atom name, index
-7.608595309        -7.897790000        -7.892053559    #position
1.056610291        -1.218664448         3.345828610    #velocity
-1979.558687         739.7961625         1027.996603    #force
K+               2
-4.678562643        -4.509858530        -7.813252872
-0.7078383910         1.220785303       -0.9440783885
212.7300659        -4290.721728         1363.866117
K+               3
-7.821414265        -4.635443539        -4.732164540
2.637614561        0.5778767520E-01    -1.704765568
150.3309776        -812.6932914         1429.413120
K+               4
-4.577735234        -7.808222424        -4.540282303
4.950411107         3.576253827        0.2276058039
-782.7309730         1322.553499        -205.1240756
Cl-              5
-7.810782981        -4.845250366        -7.815286768
1.643324971       -0.6479194620         3.393130560
407.2394357         1675.508460         748.2506938

The details about preparing this file with other packages(Athen) will be discussed
Next we prepare the CONTROL file:

**–begins here–<We will at first discuss only relevant parameters>–**
DL_POLY: Potassium Chloride Test Case    !heading
temperature      600.0                !system temperature in Kelvin
pressure         144.0                !system pressure
steps             4000                !maximum no of steps,2000 is enough
equilibration      500                  !time for the system to equlibrate
timestep         0.005
multiple             1
print               10
stats               10
scale               10
restart scale
rdf                 10             !write radial distribution function at 10 timescale interval
print rdf
cutoff             7.0                !define cutoff for interactions to 7 Angstorms
rvdw               7.0
delr               1.0
ewald precision  1.e-6
ensemble nst hoover 0.1 1.0            !Ensemble
trajectory 20 30 0                !write history file
job time          3600                !set job time
close time         100
finish                        !control file ends


DL_POLY: Potassium Chloride Test Case

UNITS eV    !energy units

MOLECULES 1    ! number of molecule type

Potassium Chloride    !Molecule name

nummols 27        !number of molecules

atoms 8        ! no of atoms in this molecular type

K+           39.0983       0.994    4

Cl-          35.4530      -0.994    4


VDW 3            !number of van der wall interactions

K+      K+      buck      3796.9      0.2603      124.90

Cl-     Cl-     buck      1227.2      0.3214      124.90

K+      Cl-     buck      4117.9      0.3048      0.0000



To run the program make sure the CONFIG,CONTROL,FIELD files are there in the execute folder, from terminal invoke dlpoly



This will run the simulation and write the output files



  1. We will visualize the resulting system.This can be done through GUI by plotting the REVCON file(which is the system at the end of simulation)
    You can also visualize the CONFIG file.
    Another better alternative of visualizing the files is to convert the CONFIG file to XYZ files and plotting them on VMD

  2. Checking the Diffusion coefficient in OUTPUT file, if it is less than 10-5then it is liquid state.A value of zero suggests it to be solid state.

  3. Now we will analyze the output from the simulation using the RDFDAT file that was created.From GUI plot the RDF -> select the atom types K+ and Cl-

    This will extract the RDF for K+ and Cl- from the RDFDAT file and create a separate XY file.For various simulation parameters you can create different RDF files and merge them together and plot so that you can compare where the system is heading to and draw good conclusions.I have written a small script in python to do that.

# Import modules

import sys

import matplotlib.pyplot as plt

import numpy as np


to be invoked as

plot_rdf <option={-m,-p}> <no of files> <list of files>

option -m merges the given number of files using single X cordinates and

y coordinate.Option -p plots the given file


plot_rdf -m 2 RDF_100.XY RDF_14.XY

merges the two files


#import pylab as pl





#process data









#TODO: write names of field and parameters in first column

   for row in data:


       for element in row:

           X=X+’ ‘+str(element)



elif (option==’-p’):

   # Open the data

   datafile = sys.argv[index]

   #f = open(datafile, ‘r’)

   data = np.loadtxt(datafile)



   #plot all Y’s




   # Get axis labels

   xaxis_label = raw_input(‘X-axis label > ‘)

   yaxis_label = raw_input(‘Y-axis label > ‘)

   # Show the plot





The RDF is the measure of how the probability deviates from an uniform distribution.From the radial distribution function a number of parameters can be determined.We can also identify the phase transition from the change in pattern in the RDF

Picture stolen from Jacek Dziedzic,Gdansk University of Technology,Computational nanotechnology

Diracs Puzzle

I will post here with some musings I came across another blog:
http://www.minustwofish.com/Here is a question that was made to Dirac, the great genius !Here is it

Three fishermen come back from the sea. Each collapses in their respective tent. Fisherman #1 wakes up and decides to get his share of the catch. He counts the fish, realizes it is not a number divisible by three, throws away one fish to the sea correcting the situation, and takes a third of the remaining fish into his tent. Fisherman #2 wakes up later and also decides he is going to get his share of the catch. Fisherman #2 wants a third of the fish he sees. It is not a multiple of three, but he throws away one fish and takes a third of the fish and goes to sleep. Fisherman #3 wakes up after, and does the same: he throws away one fish, takes a third of the fish, and goes into his tent.
What is the smallest number of fish for which this would happen?

Ah its simple isnt it?

Guess what was Dirac’s answer -2! no wonder he came up with the idea of filled negative electrons in Dirac sea

Hello !

Hello all, i am shifting blogs from blogspot to wordpress, because of its ease with LaTeX and inconsistency of google,I dd not like the new getup of blogspot.Also I believed Google kept blogspot just for timepass, and wasnt serious about it.Also loved wordpress getup , simple and elegant…so here I come wordpress..