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

Getting started

  1. Download and uncompress a recent version of Gmsh, or the ONELAB bundle for Windows64, Windows32, Linux64, Linux32 or MacOSX.
  2. Double-click on the Gmsh executable (gmsh.exe GmshIcon.png on Windows).
  3. Load the Python script (.py file) through the File/Open menu, e.g. load the 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: 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 module. You can also install 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

# 1) launch "gmsh"
# 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')

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')

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))

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, 
phi0 = c.defineNumber('Init/initial phi angle [deg]', value=180,

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

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


   if refr >= refresh:
      refr = 0
      c.setNumber( + '/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( + '/Action') == 'stop'):

      exportMsh(l1, l2)
      exportIter(iter, time, x1, y1+l1, x2, y2+l1+l2)
      iter += 1

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

Direct link to file `pendulum/'

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

import onelab

The script then creates a ONELAB client with:

c = onelab.client(__file__)

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.:

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

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:

if c.action == 'check' :

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:

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

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


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:

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.
If readOnly is set, the value cannot be changed server-side, and the value provided in the python script is always used
Should the parameter be visible in the interface?
Help string for this parameter
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:

Minimum value allowed when scrolling in the interface, and when looping on the parameter
Maximum value allowed when scrolling in the interface, and when looping on the parameter
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:

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

Access to runtime Gmsh front-end parameters

Accessing 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. See above.
c.loop == 0|1
Gmsh can loop on parameters to perform simple parametric analyses. The variable c.loop is 1 when Gmsh is engaged 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 is called by Gmsh with no GUI, i.e. with gmsh -. It is 0 otherwise.
c.getPath | c.checkPath
The function 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. The function 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.

Saving/loading models and solutions

If the Archive output files automatically checkbox is checked in the gear menu of Gmsh, the files declared in the python script by the statement

c.outputFiles( [file1.ext1, file2.ext2, …] )

as well as the database state, are copied at the end of each run of the model into the /archive subdirectory of the working directory with names


The automatically appended stamp consists of a to the second accurate timestamp yyyy-mm-dd_hh-mm-ss, augmented with the user-defined ONELAB string parameter named Metamodel/Tag (which can be a null string). The purpose of automatic archiving is to keep track of all simulations done, which might be memory-space consuming. The declared output files should therefore not be too large in size, and contain in a concise form the main results of a simulation. The archived database, on the other hand, allows reproducing the simulation if needed.

When a metamodel involves heavy and time-consuming computations, it is also interesting, in addition to the output files, to also save the solution files. This allows making series of post-processing runs on the same simulation data. To do this, the Load Database and Save Database commands of the gear menu are used. If the script contains a statement

c.solutionFiles( [file1.ext1, file2.ext2, …] )

saving the database under the name onelab_tag.db into the directory dbdir with the Save Database widget will save the ONELAB database and additionally rename on disk the declared solution files into


It is a good practice to save the databases in the working directory, so that the saved solution files end up in the same directory as the automatically archived output files.

Be sure to clearly understand the difference between 'output files' and 'solution files'. The former are small-size files (order of a few kB) that summarize a simulation in a concise way, typically data for graphs. The latter are large-size files (order of MB) containing solutions at all nodes and all time steps of the finite element problem. The user is invited to clean up the /archive subdirectory regularly. Practically, when a simulation is completed that you want to save,

  • click on gear menu/Save database,
  • enter a filename of the form onelab_tag.db in the Save as box, with an explicit tag that characterizes the simulation at hand (e.g. onelab_case1.db or onelab_reference.db)
  • browse to the directory where the database should be saved (recommended: in the working directory)
  • click on Save.

To reload a simulation,

  • click on gear menu/Open database
  • select the database to restore (e.g. onelab_case1.db)
  • click on Open.

As long as the Use restored solution checkbox remains checked, model runs will use the restored solution files.