--- /dev/null	Thu Jan 01 00:00:00 1970 +0000
+++ b/icqsol_solve_laplace.xml	Tue Aug 23 15:04:45 2016 -0400
@@ -0,0 +1,67 @@
+<?xml version='1.0' encoding='UTF-8'?>
+<tool id="icqsol_solve_laplace" name="Solve Laplace equation" version="@WRAPPER_VERSION@.0">
+    <description>- computes the jump of normal electric field</description>
+    <macros>
+        <import>icqsol_macros.xml</import>
+    </macros>
+    <expand macro="requirements" />
+    <command>
+        <![CDATA[
+            python $__tool_directory__/icqsol_solve_laplace.py
+            --input "$input"
+            --input_file_format_and_type $input.ext
+            --input_dataset_type $input.metadata.dataset_type
+            --input_potential_name "$input_potential_name"
+            --output_jump_electric_field_name "$output_jump_electric_field_name"
+            --output "$output"
+            --output_vtk_type $output_vtk_type
+        ]]>
+    </command>
+    <inputs>
+        <param name="input" type="data" format="vtkascii,vtkbinary" label="Shape" help="Format can be vtkascii or vtkbinary." />
+        <param name="input_potential_name" type="select" label="Field name" refresh_on_change="True"> 
+            <options>
+                <filter type="data_meta" ref="input" key="field_names"/>
+                <validator type="no_options" message="The selected shape has no surface fields." />
+            </options>
+        </param>
+        <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." />
+        <expand macro="output_vtk_type_params" />
+    </inputs>
+    <outputs>
+        <data name="output" format_source="input">
+            <actions>
+                <action type="format">
+                    <option type="from_param" name="output_vtk_type" />
+                </action>
+            </actions>
+        </data>
+    </outputs>
+    <tests>
+        <test>
+            <param name="input" value="sphere.vtkbinary" ftype="vtkbinary" />
+            <param name="input_file_format_and_type" value="vtkbinary" />
+            <param name="input_dataset_type" value="POLYDATA" />
+            <param name="input_potential_name" value="v" />
+            <param name="output_jump_electric_field_name" value="E_normal_jump" />
+            <output name="output" file="sphere_electric_field.vtkascii" ftype="vtkascii" />
+            <param name="output_vtk_type" value="vtkascii" />
+        </test>
+    </tests>
+    <help>
+
+**What it does**
+
+Computes the jump in flux-like (Neumann) boundary conditions given prescribed Dirichlet boundary
+conditions by using the boundary element method.  Depending on the problem, the jump can be the
+surface flux or the normal electric field in electrostatic problems. The Dirichlet field is often
+called the potential (e.g. electrostatic potential). When the domain extends from the object to
+infinity and the interior of the object is perfectly conducting, the jump corresponds to the normal
+electric field just outside the object.
+
+* **Shape** - Shape whose surface contains a potential field.
+* **Output flux field name** - Name of the jump of normal electric field name in the output file.
+
+    </help>
+    <expand macro="citations" />
+</tool>