Kratos For Dummies
(→Using the GiD problemtype)
(→Using the GiD problemtype)
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==== Using the GiD problemtype ====
==== Using the GiD problemtype ====
Using the GiD interfase allows you to manage much more complex geometries. Moreover, you can launch Kratos directly from the (visual) GiD interfase, so there's no longer need to use a console. To do so simply download [[File:PureDiffusion.gid.zip
Using the GiD interfase allows you to manage much more complex geometries. Moreover, you can launch Kratos directly from the (visual) GiD interfase, so there's no longer need to use a console. To do so simply download [[File:PureDiffusion.gid.zip]] and unzip it inside the GiD problemtypes folder. The interfase is really easy to use so you should have no problems understanding how to use it.
Revision as of 08:56, 3 October 2013
As explained in the What is Kratos page, the Kratos framework is oriented towards finite element modelling. This is a major advantage when creating standard finite element formulations. In these cases, Kratos will provide most of the tedious code necesary, such as ensambling the matrices, solving the system, priting the results in a file, and other task that would probably be more time consuming than transcribing the formulation itself into programming code. The aim of this tutorial is to describe step by step the implementation of a really simple element using as much as possible all these tools provided by Kratos. This way, we'll only have to create the element, boundary conditions and then tell Kratos that our problemtype is a standard FEM. At first the code might seem a little scary but we'll try to explain the lines as much as possible. Let's begin!
(it must be noted that the framework is completely flexible and we could create a problemtype without even creating an element that does something, for example in edgebased formulations)
Basic description of the problem and main tools of Kratos used:
We'll create the simplest possible finite element formulation. For that porpuose we'll create an application that solves a stationary heat conduction problem for 2D. This is a difussion only problem with only one degree of freedom (DoF) per node.
- , where K is the material conductivity
In this problem we're going to use a residualbased formulation. Kratos already has a solver so we won't have to program it.
As seen in the previous section, our problem consists of a simple rigidity matrix K , that depends only on the geometry and the scalar permittivity (a closer look reveals that is simply the laplacian matrix multiplied by this scalar). The other components of our problem are boundary conditions , which we'll asume fixed or free, and thermal loads .
The rigidity matrix will be calculated element by element, adding the rigidity of each element K to the global matrix. This reveals the first tool needed in ourproblemtype: an element.
For the Dirichlet conditions , since we're using a residualbased calculation we'll have to multiply our boundary conditions by the K matrix. This can be done both elementwisely once we have K or at the end of the problem. We chose to do it elementwisely.
Finaly, for the node thermal loads we have to add them node by node and add it to the right hand side vector of the system of equations (RHS). To do so we'll use a tool in Kratos called Condition.
As you can see, we now have our main components:
-an element (loop in elements, including K and Dirichlet conditions)
-a condition (loop in nodes)
residualbased builder and solver
What is missing is a tool to assemble all these components. We could do it "by hand", but it is much simpler if we just use a builder and solver. Kratos include a residualbased builder and solver. This way we only have to declare in our problemtype that we'll be using this tool and which are the elements and conditions. And that's it. We won't even need to tell the builder to loop the nodes or elements, just declaring them and then initializing the solver is enough and the process will be done.
Of course, to do so we'll have to respect the structure for both the element and conditions, but this is achieved by simply copying an existing one and modifying it to suit our needs, as will be seen below.
Structure of the problemtype and other components
In the previous section we explained the code needed inside Kratos to solve a Poisson problem. However no information regarding loading the model or telling Kratos that we want to execute our problemtype was given. All these tasks are not compiled in the Kratos, they're simply executed by python scripts. Some of them will belong to our problemtype itself and other will be contained inside the folder of the specific problem (mesh) to be solved.
The big advantage of using these scripts over compiled code is that changes can be done really quicky, for example changing the tolerance of a solver or even changing boundary conditions. Of course, since it's interpreted languange it will be slower; so it's better to limit its use to simple, non iterative tasks as much as possible.
In this sense, the python scripts do the following tasks:
- Load Kratos and import our application
- read the problem data and create the model part in Kratos : mesh, elements, materials, variables, degrees of freedom.
- Define the builder&solver used
- Call the solver
- Write a file with the mesh and results
Basic Structure of Conditions and Elements
Elements and Conditions are both classes in C++ tha include a series of subroutines required by the builder and solver. they both share the following structure. In pseudo code:
class mycondition void CalculateLocalSystem void CalculateRightHandSide void EquationIdVector void GetDofList
Files needed in our application
- static_poisson_solver.py Our python file
- kPoisson.h and kPoisson.cpp to define our application
- poisson_2d.h and poisson_2d.cpp to define our element
- pointsource.h and pointsource.cpp to define our condition (thermal load)
- extra files such as a .py in the folder of the problem and a cmake so that our files are compiled.
Sections of this tutorial
Creating our application: PureDifussion
To begin with we must create a new application. Using cmake this is a straightforward task. Since we have a pure diffusion problem we'll name it PureDiffusion. To do so follow the steps in the How to Create a New Application using cmake page. Therefore we'll set in the prepare_cmake.sh:
NEW_NAME_LOWERCASE=purediffusion NEW_NAME_MIXED=PureDiffusion NEW_NAME_UPPERCASE=PUREDIFFUSION
Once you've followed all the steps in the how to you should be able to import your newly created application, although it is not able to do anything for the moment.
Editing the main files of the application and creating elements and conditions
4. Modify the purediffusion_python_application.cpp file in the folder /custom_python so that we can add our new variable from python (the others are included in the Kernel so we only need to add POINT_HEAT_SOURCE:
//registering variables in python KRATOS_REGISTER_IN_PYTHON_VARIABLE(POINT_HEAT_SOURCE);
5. Tutorial:Creating an Utility (optional)
Once you've completed these 4/5 first steps and compiled the kratos you have all the c++ code necessary for your application. So compile the Kratos and the rest of the tasks can be managed using python, which has the advantages mentioned above. So now we proceed with the python scripts required.
After you've finished these 6 steps your new application is ready. what is left is creating the particular files of our problem.
Creating a first problem to be solved
Despite the GID interface can both create and launch the files needed to solve a problem, we'll start by writing 'by hand' a very simple example so that we underestand the instruction we're giving KRATOS through the python interface we have just created in the previous step. So hands at work!
We need two files to launch an example:
- a .mdpa' (meaning modelpart) file defining the geometry, material, loads, etc.
- a .py file to tell KRATOS what to do with that file.
For our first problem we'll create a simple, two element problem:
with CONDUCTIVY=10.0, we'll fix the TEMPERATURE=100.0 in node 1 and we'll add a POINT_HEAT_SOURCE=5.0 in node 3
with this information, the model part file looks like this:
Begin ModelPartData // nothing here End ModelPartData Begin Properties 1 CONDUCTIVITY 10.0 // all the elements of the group 1 (second column in the list of elements) will have this property End Properties Begin Nodes 1 0.0 0.0 0.0 //node number, coord x, cord y, coord z 2 1.0 0.0 0.0 //node number, coord x, cord y, coord z 3 1.0 1.0 0.0 //node number, coord x, cord y, coord z 4 0.0 1.0 0.0 //node number, coord x, cord y, coord z End Nodes Begin Elements Poisson2D //here we must write the name of the element that we created 1 1 1 2 4 //the first column is the property 2 1 3 4 2 End Elements Begin NodalData TEMPERATURE //be careful, variables are case sensitive! 1 1 100.0 // pos1 is the node, pos2 (a 1) means that the DOF is fixed, then (position 3) we write the fixed displacement (in this case, temperature) End NodalData Begin NodalData POINT_HEAT_SOURCE 3 0 5.0 //fixing it or not does not change anything since it is not a degree of freedom, it's just info that will be used by the condition End NodalData Begin Conditions PointSource 1 1 3 //pos1:condition ID(irrelevant) ; pos2:cond Property ( = 1 in this case) ; pos3:node to apply the condition. End Conditions
and our python file:
################################################################## ################################################################## #setting the domain size for the problem to be solved domain_size = 2 # 2D problem #including kratos path from KratosMultiphysics import * #we import the KRATOS from KratosMultiphysics.PureDiffusionApplication import * #and now our application. note that we can import as many as we need to solve our specific problem #defining a model part model_part = ModelPart("ExampleModelPart"); #we create a model part import pure_diffusion_solver #we import the python file that includes the commands that we need pure_diffusion_solver.AddVariables(model_part) #from the static_poisson_solver.py we call the function Addvariables so that the model part we have just created has the needed variables # (note that our model part does not have nodes or elements yet) #now we proceed to use the GID interface (both to import the infomation inside the .mdpa file and later print the results in a file gid_mode = GiDPostMode.GiD_PostAscii #we import the python file that includes the commands that we need multifile = MultiFileFlag.SingleFile deformed_mesh_flag = WriteDeformedMeshFlag.WriteUndeformed write_conditions = WriteConditionsFlag.WriteElementsOnly gid_io = GidIO("art4",gid_mode,multifile,deformed_mesh_flag,write_conditions) model_part_io = ModelPartIO("example") # we set the name of the .mdpa file model_part_io.ReadModelPart(model_part) # we load the info from the .mdpa # we create a mesh for the postprocess mesh_name = 0.0 gid_io.InitializeMesh( mesh_name ); gid_io.WriteMesh((model_part).GetMesh()); gid_io.FinalizeMesh() #the buffer size should be set up here after the mesh is read for the first time (this is important for transcient problems, in this static problem =1 is enough) model_part.SetBufferSize(1) # we add the DoFs pure_diffusion_solver.AddDofs(model_part) #creating a solver object solver = pure_diffusion_solver.StaticPoissonSolver(model_part,domain_size) solver.time_order = 1 solver.echo_level = 0 solver.Initialize() print "about to solve!" solver.Solve() print "Solved!" #and we print the results gid_io.InitializeResults(mesh_name,(model_part).GetMesh()) gid_io.WriteNodalResults(TEMPERATURE,model_part.Nodes,0,0) gid_io.FinalizeResults() #since we have already calculated the temp, we can get the mean value #first the constructor (it could have been called before) calc_mean=CalculateMeanTemperature(model_part) #and we calculate! calc_mean.Execute()
Launching and viewing the postprocess file
Once you have both files, you must open a console, go the directory where you created both files and type:
This launches the script you've created and several files are created after it has finished. The ones we are interested in are output.res and output.msh (results and mesh respectively). They are ascii files so you can view them using the text editor you prefer. Alternatively, you can open the .res with GiD to visualize them. THe result should look like this:
Congratulations!, you have successfully created and launched your first python application.
Using the GiD problemtype
Using the GiD interfase allows you to manage much more complex geometries. Moreover, you can launch Kratos directly from the (visual) GiD interfase, so there's no longer need to use a console. To do so simply download File:PureDiffusion.gid.zip and unzip it inside the GiD problemtypes folder. The interfase is really easy to use so you should have no problems understanding how to use it.