wd15

{
 "metadata": {
  "name": "extremefill2D"
 },
 "nbformat": 3,
 "nbformat_minor": 0,
 "worksheets": [
  {
   "cells": [
    {

wd15

{
 "metadata": {
  "name": "upwind"
 },
 "nbformat": 3,
 "nbformat_minor": 0,
 "worksheets": [
  {
   "cells": [
    {

wd15

{
 "metadata": {
  "name": ""
 },
 "nbformat": 3,
 "nbformat_minor": 0,
 "worksheets": [
  {
   "cells": [
    {

wd15

import time
import fipy as fp
import numpy as np

np.random.seed(1)
L = 1.
N = 30
m = fp.GmshGrid3D(nx=N, ny=N, nz=N, dx=L / N, dy=L / N, dz=L / N)
v = fp.CellVariable(mesh=m)
v0 = np.random.random(m.numberOfCells)

wd15

#!/usr/bin/env python

import fipy as fp
import sys
from subprocess import Popen, PIPE
mshFile = 'tmsh3d.msh'

if fp.parallelComm.procID == 0:
   dimensions = 3
   geoFile = 'tmsh3d.geo'

wd15

{
 "metadata": {
  "name": ""
 },
 "nbformat": 3,
 "nbformat_minor": 0,
 "worksheets": [
  {
   "cells": [
    {

wd15

#!/usr/bin/env python

## 
 # ###################################################################
 #  FiPy - Python-based finite volume PDE solver
 # 
 #  FILE: "leveler.py"
 #
 #  Author: Jonathan Guyer <guyer@nist.gov>
 #  Author: Daniel Wheeler <daniel.wheeler@nist.gov>

wd15

#!/usr/bin/env python
from optparse import OptionParser
import numpy as nm

import sys
sys.path.append('.')



from sfepy.base.base import IndexedStruct

wd15

#!/usr/bin/env python
from optparse import OptionParser
import numpy as nm

import sys
sys.path.append('.')



from sfepy.base.base import IndexedStruct

wd15

import matplotlib.pyplot as plt
from matplotlib import colors
from numpy.random import normal
from matplotlib.mlab import bivariate_normal
from fipy import *
from fipy import numerix
import numpy as np

fig = plt.figure
ax1 = plt.subplot((111))