Python

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Revision as of 17:15, 12 January 2015 by Francois (talk | contribs) (Communication with the Gmsh front-end)

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Any Python script can become a native ONELAB client by importing the onelab.py module.

Getting started

  1. Download and uncompress a recent version of Gmsh, or the Gmsh/GetDP bundle for Windows64, Windows32, Linux64, Linux32 or MacOSX.
  2. Double-click on the Gmsh executable (gmsh.exe
    Error creating thumbnail: Unable to save thumbnail to destination
    on Windows).
  3. Load the Python script (.py file) through the File/Open menu, e.g. load the pend.py example given below.
  4. Click on Run.
  5. ... that's it!

How does it work?

The Python ONELAB interface is implemented in a single Python module: onelab.py. This module comes pre-installed with Gmsh, in the same directory as the Gmsh executable. When you open a ONELAB-enabled Python solver with Gmsh, Gmsh automatically finds the onelab.py module. You can also install onelab.py in any directory of your choosing; in this case don't forget to update your PYTHONPATH environment variable.

The following example (a simple Python solver for the double pendulum problem) highlights the main features of the Python interface:
#!/usr/bin/env python
#coding=utf-8

# 1) launch "gmsh pend.py"
# 2) there is no 2... :-)

import onelab
import math, os

c = onelab.client(__file__)

def exportMsh(le1,le2):
   mshFile = open(c.getPath("pend.msh"), 'w')
   mshFile.write('$MeshFormat\n2.2 0 8\n$EndMeshFormat\n')
   mshFile.write('$Nodes\n3\n1 0 0 0\n2 0 %s 0\n3 0 %s 0\n$EndNodes\n' %(-le1, -le1-le2))
   mshFile.write('$Elements\n3\n1 1 2 0 1 1 2\n2 1 2 0 1 2 3\n3 15 2 0 2 3\n$EndElements\n')
   mshFile.close()

def exportMshOpt():
   optFile = open(c.getPath("pend.msh.opt"),'w')
   optFile.write('n = PostProcessing.NbViews - 1;\n')
   optFile.write('If(n >= 0)\nView[n].ShowScale = 0;\nView[n].VectorType = 5;\n')
   optFile.write('View[n].ExternalView = 0;\nView[n].DisplacementFactor = 1 ;\n')
   optFile.write('View[n].PointType = 1;\nView[n].PointSize = 5;\n')
   optFile.write('View[n].LineWidth = 2;\nEndIf\n')
   optFile.close()

def exportIter(iter,t,x1,y1,x2,y2):
   mshFile = open(c.getPath("pend.msh"),'a')
   mshFile.write('$NodeData\n1\n"motion"\n1\n\t%f\n3\n\t%d\n3\n' % (t, iter))
   mshFile.write('\t3\n\t1 0 0 0\n\t2 %f %f 0\n\t3 %f %f 0\n$EndNodeData\n' %(x1,y1,x2,y2))
   mshFile.close()

g = 9.8	# acceleration of gravity
m = 0.3 # mass of pendulum balls

l = c.defineNumber('Geom/arm length [m]', value=1.0)
time = c.defineNumber('Dyna/time [s]', value=0.0)
dt = c.defineNumber('Dyna/time step [s]', value=0.001)
tmax = c.defineNumber('Dyna/max time [s]', value=20)
refresh = c.defineNumber('Dyna/refresh interval [s]', value=0.1)
theta0 = c.defineNumber('Init/initial theta angle [deg]', value=10, 
                         attributes={'Highlight':'Pink'})
phi0 = c.defineNumber('Init/initial phi angle [deg]', value=180,
                       attributes={'Highlight':'Pink'})

# we're done if we are in the "check" phase
if c.action == 'check' :
   exit(0)

l1 = l;
l2 = l;
m1 = m;
m2 = m;
theta = theta0 / 180.*math.pi;
phi = phi0 / 180.*math.pi;
theta_dot = 0.0
phi_dot = 0.0
refr = 0.0
iter = 0
time = 0.0

while (time < tmax):
   delta = phi - theta
   sdelta = math.sin(delta)
   cdelta = math.cos(delta)
   theta_dot_dot = ( m2*l1*(theta_dot**2.0)*sdelta*cdelta
                     + m2*g*math.sin(phi)*cdelta
                     + m2*l2*(phi_dot**2.0)*sdelta
                     - (m1+m2)*g*math.sin(theta) )
   theta_dot_dot /= ( (m1+m2)*l1 - m2*l1*(cdelta)**2.0 )
   
   phi_dot_dot = ( -m2*l2*(phi_dot**2.0)*sdelta*cdelta
                    + (m1+m2)*(g*math.sin(theta)*cdelta
                               - l1*(theta_dot**2.0)*sdelta
                               - g*math.sin(phi)) )
   phi_dot_dot /= ( (m1+m2)*l2 - m2*l2*(cdelta)**2.0 )
   
   theta_dot = theta_dot + theta_dot_dot*dt
   phi_dot = phi_dot + phi_dot_dot*dt

   theta = theta + theta_dot*dt
   phi = phi + phi_dot*dt

   x1 =  l1*math.sin(theta)
   y1 = -l1*math.cos(theta)
   x2 =  l1*math.sin(theta) + l2*math.sin(phi)
   y2 = -l1*math.cos(theta) - l2*math.cos(phi)

   time += dt
   refr += dt

   exportMshOpt()

   if refr >= refresh:
      refr = 0
      c.setNumber(c.name + '/Progress', value=time, min=0, max=tmax, visible=0)
      c.setNumber('Dyna/time [s]', value=time)
      c.setNumber('Solu/phi', value=phi)
      c.addNumberChoice('Solu/phi', phi)
      c.setNumber('Solu/theta', value=theta)
      c.addNumberChoice('Solu/theta', theta)
      c.setNumber('Solu/phi dot', value=phi_dot)
      c.addNumberChoice('Solu/phi dot', phi_dot)
      c.setNumber('Solu/theta dot', value=theta_dot)
      c.addNumberChoice('Solu/theta dot', theta_dot)

      # ask Gmsh to refresh
      c.setString('Gmsh/Action', value='refresh')

      # stop if we are asked to (by Gmsh)
      if(c.getString(c.name + '/Action') == 'stop'):
         break;

      exportMsh(l1, l2)
      exportIter(iter, time, x1, y1+l1, x2, y2+l1+l2)
      c.mergeFile(c.checkPath('pend.msh'))
      iter += 1

c.setNumber(c.name + '/Progress', value=0)

Direct link to file `pendulum/pend.py'


To interact with ONELAB, the script must first import the onelab.py module:

<syntaxhighlight lang="python" enclose="div">

import onelab

</syntaxhighlight>

The script then creates a ONELAB client with:

<syntaxhighlight lang="python" enclose="div">

c = onelab.client(__file__)

</syntaxhighlight>

Creating the client connects the script to the onelab server, through a socket. The __file__ argument is a python variable. It tells ONELAB in which directory the script being executed is located. New ONELAB variables can then be defined using defineNumber, e.g.:

<syntaxhighlight lang="python" enclose="div">

l = c.defineNumber('Geom/arm length [m]', value=1.0)

</syntaxhighlight>

When the script is run, if the parameter Geom/arm length [m] has not been previously defined, it takes the value (1.0) provided in defineNumber and is sent to the ONELAB server. The "/" character in the variable name is interpreted as a path separator, and results in the creation of a sub-tree in the graphical user interface. If the script is re-run later, the value will be updated using the value from the server (unless it is labeled as readOnly: see below). When Gmsh runs a ONELAB client, the client can be run in two modes: c.action=='check' to check the coherence of the ONELAB database and make adjustments if necessary, and c.action=='compute' to perform the actual computation. For instance, in 'check' mode, the double pendulum client simply defines the ONELAB variables it wants to share with the server, then exits:

<syntaxhighlight lang="python" enclose="div">

if c.action == 'check' : exit(0)

</syntaxhighlight>

In 'compute' mode, the code enters a loop and performs the actual computation. During the computation the script can directly set a value in the ONELAB database with setNumber, as is done in the example with:

<syntaxhighlight lang="python" enclose="div">

c.setNumber('Solu/phi', value=phi)

</syntaxhighlight>

It can also e.g. ask the server to read a file with mergeFile:

<syntaxhighlight lang="python" enclose="div">

c.mergeFile(c.checkPath('pend.msh'))

</syntaxhighlight>

The check path function (c.checkPath) builds the pathname of a file named pend.msh located in the same directory as the script under execution, and then checks on whether the pathname exists on disk. If not, an error message is issued. Use the regular path function (c.getPath) to build a pathname without checking on the presence on disk of the file.

Common parameter attributes

Here's the list of attributes available for all ONELAB parameters:

name=string
The name of the parameter in the ONELAB database, in the form of a "/"-separated path. The name attribute is mandatory to exchange the variable with the ONELAB server.
readOnly=0|1
If readOnly is set, the value cannot be changed server-side, and the value provided in the python script is always used
visible=0|1
Should the parameter be visible in the interface?
help=string
Help string for this parameter
label=string
Alternative label used in the graphical user interface, replacing the part of "Name" located after the last "/"

Other attributes can be specified using the generic attribute dictionary, e.g. attribute={'Highlight':string}. See ONELAB Syntax for Gmsh and GetDP for a list of all other attributes.

Number attributes

In addition, numbers can take the following specific attributes:

min=number
Minimum value allowed when scrolling in the interface, and when looping on the parameter
max=number
Maximum value allowed when scrolling in the interface, and when looping on the parameter
step=number
Step value used when scrolling in the interface, and when looping on the parameter
choices={number, number, ...}
Possible choices for the parameter
labels={number:string, number:string, ...}
Possible choices for the parameter, with string labels for each choice

String attributes

Strings accept the following specific attributes:

kind=string
Mutable kind of the string (currently: "file")
choices={string, string, ...}
Possible choices for the parameter

Communication with the Gmsh front-end

A number of Gmsh runtime parameters can be useful to develop more involved on more user-friendly Python-ONELAB solvers.

c.action == 'check' | 'compute'
Test on the string variable c.action can be done to branch on parts of the script to be executed or not according to the mode.
c.loop == 0|1
Gmsh can loop on parameters to perform simple parametric analyses. The variable c.loop is 1 when Gmsh is in such a loop, 0 otherwise. See Beam3D for an example.
c.batch == 0|1
The variable c.batch is 1 when a Python script « script.py » is called by Gmsh with no GUI, i.e. with gmsh script.py -
c.getPath | c.checkPath
c.getPath(subdir/filename) returns a pathname built by appending ‘subdir/filename’ to the pathname of the directory where the Python script under execution is located.
c.checkPath is the same as c.getPpath but also checks whether the built pathname exists on disk. If the pathname does not exist, an error is issued.