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maxwellian.py
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# -*- coding: utf-8 -*-
"""
demo of loading maxwellian VDF
@author: lbrieda
"""
import numpy as np
import pylab as pl
from random import random as rand
NP = 50000; #number of samples
NUM_BINS = 500; #number of uniques we would like
mass = 16*1.66e-27 #16amu
Kb = 1.3806e-23 #boltzmann constant
T = 1000 #temperature
vdrift = 3000 #drift velocity
vth = np.sqrt(2*Kb*T/mass) #thermal velocity
bins = np.zeros((NUM_BINS,1));
bin_min = 0;
bin_max = max(2*vdrift,10*vth)
dbin = (bin_max-bin_min)/NUM_BINS
def maxw1d(vth):
M = 12 #parameter for Birdsall's method
#sample Maxwellian using Birdsall's method
sum = 0
for i in range(M):
sum = sum+rand()
return np.sqrt(0.5)*vth*(sum-M/2)/np.sqrt(M/12);
#storage for particles
vels = np.zeros((NP,3))
for s in range (NP):
v1 = maxw1d(vth)
v2 = maxw1d(vth)
v3 = maxw1d(vth)+vdrift
mag = np.sqrt(v1*v1+v2*v2+v3*v3)
#bin result, add to nearest
bin = np.floor((mag-bin_min)/dbin+0.5)
if (bin<NUM_BINS):
bins[bin] = bins[bin] + 1
#save for later
vels[s] = [v1,v2,v3]
#compute temperature
#part 1), get average velocity
vel_ave = [np.sum(vels[:,0]),
np.sum(vels[:,1]),
np.sum(vels[:,2])]
vel_ave = np.divide(vel_ave,NP)
print("vel_ave = [%.3g %.3g %.3g]"%(vel_ave[0],vel_ave[1],vel_ave[2]))
#part 2, compute mv^2
v2_sum = 0
for s in range (NP):
dv = vels[s] - vel_ave
v2 = dv[0]*dv[0] + dv[1]*dv[1] + dv[2]*dv[2]
v2_sum = v2_sum + v2
v2_ave = np.divide(v2_sum,NP)
temp_computed = v2_ave * mass/(3.*Kb)
print("Computed temperature %.3g"%temp_computed)
bins = bins/np.max(bins); #%normalize bins
vel = np.arange(bin_min,bin_max,dbin) #velocities for plotting
#fm = np.exp(-vel**2/vth**2) #theoretical maxwellian
gm = (vel)**2*np.exp(-(vel-vdrift)**2/vth**2)
gm = gm/np.max(gm)
#vel = vel/vth; #normalize by thermal velocity
pl.figure(1)
pl.plot(vel,bins,'x');
pl.hold(True)
pl.plot(vel,gm,'r-'); #analytical
pl.grid()
pl.hold(False)
pl.figure(2);
pl.semilogy(vel,bins,'x');
pl.hold(True)
pl.semilogy(vel,gm,'r-');
pl.ylim([1e-4,1]);
pl.grid()
pl.hold(False)