Mercurial > repos > iuc > icqsol_solve_laplace
comparison icqsol_solve_laplace.xml @ 0:2294ae1842d5 draft default tip
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| author | iuc |
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| date | Tue, 23 Aug 2016 15:04:45 -0400 |
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| -1:000000000000 | 0:2294ae1842d5 |
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| 1 <?xml version='1.0' encoding='UTF-8'?> | |
| 2 <tool id="icqsol_solve_laplace" name="Solve Laplace equation" version="@WRAPPER_VERSION@.0"> | |
| 3 <description>- computes the jump of normal electric field</description> | |
| 4 <macros> | |
| 5 <import>icqsol_macros.xml</import> | |
| 6 </macros> | |
| 7 <expand macro="requirements" /> | |
| 8 <command> | |
| 9 <![CDATA[ | |
| 10 python $__tool_directory__/icqsol_solve_laplace.py | |
| 11 --input "$input" | |
| 12 --input_file_format_and_type $input.ext | |
| 13 --input_dataset_type $input.metadata.dataset_type | |
| 14 --input_potential_name "$input_potential_name" | |
| 15 --output_jump_electric_field_name "$output_jump_electric_field_name" | |
| 16 --output "$output" | |
| 17 --output_vtk_type $output_vtk_type | |
| 18 ]]> | |
| 19 </command> | |
| 20 <inputs> | |
| 21 <param name="input" type="data" format="vtkascii,vtkbinary" label="Shape" help="Format can be vtkascii or vtkbinary." /> | |
| 22 <param name="input_potential_name" type="select" label="Field name" refresh_on_change="True"> | |
| 23 <options> | |
| 24 <filter type="data_meta" ref="input" key="field_names"/> | |
| 25 <validator type="no_options" message="The selected shape has no surface fields." /> | |
| 26 </options> | |
| 27 </param> | |
| 28 <param name="output_jump_electric_field_name" type="text" value="jumpEn" label="Output flux field name" help="Name of the jump of normal electric field in the output file." /> | |
| 29 <expand macro="output_vtk_type_params" /> | |
| 30 </inputs> | |
| 31 <outputs> | |
| 32 <data name="output" format_source="input"> | |
| 33 <actions> | |
| 34 <action type="format"> | |
| 35 <option type="from_param" name="output_vtk_type" /> | |
| 36 </action> | |
| 37 </actions> | |
| 38 </data> | |
| 39 </outputs> | |
| 40 <tests> | |
| 41 <test> | |
| 42 <param name="input" value="sphere.vtkbinary" ftype="vtkbinary" /> | |
| 43 <param name="input_file_format_and_type" value="vtkbinary" /> | |
| 44 <param name="input_dataset_type" value="POLYDATA" /> | |
| 45 <param name="input_potential_name" value="v" /> | |
| 46 <param name="output_jump_electric_field_name" value="E_normal_jump" /> | |
| 47 <output name="output" file="sphere_electric_field.vtkascii" ftype="vtkascii" /> | |
| 48 <param name="output_vtk_type" value="vtkascii" /> | |
| 49 </test> | |
| 50 </tests> | |
| 51 <help> | |
| 52 | |
| 53 **What it does** | |
| 54 | |
| 55 Computes the jump in flux-like (Neumann) boundary conditions given prescribed Dirichlet boundary | |
| 56 conditions by using the boundary element method. Depending on the problem, the jump can be the | |
| 57 surface flux or the normal electric field in electrostatic problems. The Dirichlet field is often | |
| 58 called the potential (e.g. electrostatic potential). When the domain extends from the object to | |
| 59 infinity and the interior of the object is perfectly conducting, the jump corresponds to the normal | |
| 60 electric field just outside the object. | |
| 61 | |
| 62 * **Shape** - Shape whose surface contains a potential field. | |
| 63 * **Output flux field name** - Name of the jump of normal electric field name in the output file. | |
| 64 | |
| 65 </help> | |
| 66 <expand macro="citations" /> | |
| 67 </tool> |