{ "cells": [ { "cell_type": "markdown", "id": "e0f4480a", "metadata": {}, "source": [ "# Dipole antenna\n", "\n", "This example demonstrates how to create and analyze a half-wave dipole\n", "antenna in HFSS.\n", "\n", "Keywords: **HFSS**, **antenna**, **3D component**, **far field**." ] }, { "cell_type": "markdown", "id": "486df7bb", "metadata": {}, "source": [ "## Prerequisites\n", "\n", "### Perform imports\n", "\n", "Import the packages required to run this example." ] }, { "cell_type": "code", "execution_count": null, "id": "b522d3bf", "metadata": {}, "outputs": [], "source": [ "import os\n", "import tempfile\n", "import time\n", "\n", "from ansys.aedt.core import Hfss" ] }, { "cell_type": "markdown", "id": "cc17e77d", "metadata": {}, "source": [ "### Define constants\n", "Constants help ensure consistency and avoid repetition throughout the example." ] }, { "cell_type": "code", "execution_count": null, "id": "5f626f46", "metadata": {}, "outputs": [], "source": [ "AEDT_VERSION = \"2025.1\"\n", "NUM_CORES = 4\n", "NG_MODE = False # Open AEDT UI when it is launched." ] }, { "cell_type": "markdown", "id": "2cf30108", "metadata": {}, "source": [ "### Create temporary directory\n", "\n", "Create a temporary working directory.\n", "The name of the working folder is stored in ``temp_folder.name``.\n", "\n", "> **Note:** The final cell in this notebook cleans up the temporary folder. If you want to\n", "> retrieve the AEDT project and data, do so before executing the final cell in the notebook." ] }, { "cell_type": "code", "execution_count": null, "id": "ca0427c2", "metadata": {}, "outputs": [], "source": [ "temp_folder = tempfile.TemporaryDirectory(suffix=\".ansys\")" ] }, { "cell_type": "markdown", "id": "4cfddd30", "metadata": {}, "source": [ "### Launch HFSS\n", "\n", "Create an instance of\n", "the ``Hfss`` class. The Ansys Electronics Desktop will be launched\n", "with an active HFSS design. The ``hfss`` object is subsequently\n", "used to\n", "create and simulate the dipole antenna." ] }, { "cell_type": "code", "execution_count": null, "id": "9a77738b", "metadata": {}, "outputs": [], "source": [ "project_name = os.path.join(temp_folder.name, \"dipole.aedt\")\n", "hfss = Hfss(version=AEDT_VERSION,\n", " non_graphical=NG_MODE,\n", " project=project_name,\n", " new_desktop=True,\n", " solution_type=\"Modal\",\n", " )" ] }, { "cell_type": "markdown", "id": "8d81dbb9", "metadata": {}, "source": [ "## Model Preparation\n", "\n", "### Define the dipole length as a parameter\n", "\n", "The dipole length can be modified by changing the\n", "parameter ``l_dipole`` to tune the resonance frequency.\n", "\n", "The dipole will nominally be resonant at the half-wavelength frequency:\n", "$$\n", "l = \\lambda / 2 = \\frac{c_0}{2f}\n", "$$" ] }, { "cell_type": "code", "execution_count": null, "id": "4172f38c", "metadata": { "lines_to_next_cell": 2 }, "outputs": [], "source": [ "hfss[\"l_dipole\"] = \"10.2cm\"\n", "component_name = \"Dipole_Antenna_DM\"\n", "freq_range = [\"1GHz\", \"2GHz\"] # Frequency range for analysis and post-processing.\n", "center_freq = \"1.5GHz\" # Center frequency\n", "freq_step = \"0.5GHz\"" ] }, { "cell_type": "markdown", "id": "8ac3cbd0", "metadata": {}, "source": [ "### Insert the dipole antenna model\n", "\n", "The 3D component \"Dipole_Antenna_DM\" will be inserted from\n", "the built-in ``syslib`` folder. The full path to the 3D components\n", "can be retrieved from ``hfss.components3d``.\n", "\n", "The component is inserted using the method\n", "``hfss.modeler.insert_3d_component()``.\n", "\n", " - The first argument passed to ``insert_3d_component()``\n", " is the full path and name of the\n", " ``*.a3dcomp`` file.\n", " - The second argument is a ``dict`` whose keys are the names of the parameters\n", " accessible in the 3D component. In this case, we assign the\n", " dipole length, ``\"l_dipole\"`` to the 3D Component\n", " parameter ``dipole_length`` and leave other parameters unchanged." ] }, { "cell_type": "code", "execution_count": null, "id": "5fa27a9b", "metadata": {}, "outputs": [], "source": [ "component_fn = hfss.components3d[component_name] # Full file name.\n", "comp_params = hfss.get_component_variables(component_name) # Retrieve dipole parameters.\n", "comp_params[\"dipole_length\"] = \"l_dipole\" # Update the dipole length.\n", "hfss.modeler.insert_3d_component(component_fn, geometry_parameters=comp_params)" ] }, { "cell_type": "markdown", "id": "ebc279c1", "metadata": {}, "source": [ "### Create the 3D domain region\n", "\n", "An open region object places a an airbox around the dipole antenna\n", "and assigns a radiation boundary to the outer surfaces of the region." ] }, { "cell_type": "code", "execution_count": null, "id": "2a642929", "metadata": {}, "outputs": [], "source": [ "hfss.create_open_region(frequency=center_freq)" ] }, { "cell_type": "markdown", "id": "7b46fd81", "metadata": {}, "source": [ "### Specify the solution setup\n", "\n", "The solution setup defines parameters that govern the HFSS solution process. This example demonstrates\n", "how to adapt the solution mesh simultaneously at two frequencies.\n", "- ``\"MaximumPasses\"`` specifies the maximum number of passes used for automatic\n", " adaptive mesh refinement. In this example the solution runs very fast since only two passes\n", " are used. Accuracy can be improved by increasing this value.\n", "- ``\"MultipleAdaptiveFreqsSetup\"`` specifies the solution frequencies used during adaptive\n", " mesh refinement. Selection of two frequencies, one above and one below the\n", " expected resonance frequency help improve mesh quality at the resonant frequency.\n", "\n", "> **Note:** The parameter names used here are passed directly to the native AEDT API and therfore\n", "> do not adhere to [PEP-8](https://peps.python.org/pep-0008/).\n", "\n", "Both a discrete frequency sweep and an interpolating sweep are added to the solution setup.\n", "The discrete sweep provides access to field solution data for post-processing.\n", "The interpolating sweep builds the\n", "rational polynomial fit for the network (scattering) parameters over the\n", "frequency interval defined by ``RangeStart`` and\n", "``RangeEnd``. The solutions from the discrete sweep are used as the starting\n", "solutions for the interpolating sweep." ] }, { "cell_type": "code", "execution_count": null, "id": "6e51dbf2", "metadata": {}, "outputs": [], "source": [ "setup = hfss.create_setup(name=\"MySetup\", MultipleAdaptiveFreqsSetup=freq_range, MaximumPasses=2)\n", "\n", "disc_sweep = setup.add_sweep(name=\"DiscreteSweep\", sweep_type=\"Discrete\",\n", " RangeStart=freq_range[0], RangeEnd=freq_range[1], RangeStep=freq_step,\n", " SaveFields=True)\n", "\n", "interp_sweep = setup.add_sweep(name=\"InterpolatingSweep\", sweep_type=\"Interpolating\",\n", " RangeStart=freq_range[0], RangeEnd=freq_range[1],\n", " SaveFields=False)" ] }, { "cell_type": "markdown", "id": "d63c0b4c", "metadata": {}, "source": [ "### Run simulation\n", "\n", "The following cell runs the analysis in HFSS including adaptive mesh refinement and\n", "solution of both frequency sweeps." ] }, { "cell_type": "code", "execution_count": null, "id": "8954a2b9", "metadata": {}, "outputs": [], "source": [ "setup.analyze()" ] }, { "cell_type": "markdown", "id": "95cc2c8f", "metadata": {}, "source": [ "### Postprocess\n", "\n", "Plot the return loss in Ansys Electronics Desktop (AEDT). A plot similar to the one shown here will be\n", "generated in the HFSS design.\n", "\n", "" ] }, { "cell_type": "code", "execution_count": null, "id": "4c433d3f", "metadata": {}, "outputs": [], "source": [ "spar_plot = hfss.create_scattering(plot=\"Return Loss\", sweep=interp_sweep.name)" ] }, { "cell_type": "markdown", "id": "a2142bfe", "metadata": {}, "source": [ "### Visualize far-field data\n", "\n", "Parameters passed to ``hfss.post.create_report()`` specify which quantities will be\n", "displayed in the HFSS design.\n", "Below you can see how parameters map from Python to the reporter in the AEDT user interface.\n", "\n", "\n", "\n", "\n", "> **Note:** These images were created using the 25R1 release." ] }, { "cell_type": "code", "execution_count": null, "id": "5c303777", "metadata": {}, "outputs": [], "source": [ "variations = hfss.available_variations.nominal_values\n", "variations[\"Freq\"] = [center_freq]\n", "variations[\"Theta\"] = [\"All\"]\n", "variations[\"Phi\"] = [\"All\"]\n", "elevation_ffd_plot = hfss.post.create_report(expressions=\"db(GainTheta)\",\n", " setup_sweep_name=disc_sweep.name,\n", " variations=variations,\n", " primary_sweep_variable=\"Theta\",\n", " context=\"Elevation\", # Far-field setup is pre-defined.\n", " report_category=\"Far Fields\",\n", " plot_type=\"Radiation Pattern\",\n", " plot_name=\"Elevation Gain (dB)\"\n", " )\n", "elevation_ffd_plot.children[\"Legend\"].properties[\"Show Trace Name\"] = False\n", "elevation_ffd_plot.children[\"Legend\"].properties[\"Show Solution Name\"] = False" ] }, { "cell_type": "markdown", "id": "c4ca1a49", "metadata": {}, "source": [ "### Create a far-field report\n", "\n", "The ``hfss.post.reports_by_category`` helps simplify the syntax required to access\n", "post-processing capabilities. In this case, results are shown for the current\n", "variation. The concept of\n", "\"variations\" is essential for managing parametric solutions\n", "in HFSS.\n", "\n", "The argument ``sphere_name`` specifies the far-field sphere used to generate the plot.\n", "In this case, the far-field sphere \"3D\" was automatically created when HFSS was launched by\n", "instantiating the ``Hfss`` class.\n", "\n", "" ] }, { "cell_type": "code", "execution_count": null, "id": "7664fa15", "metadata": {}, "outputs": [], "source": [ "report_3d = hfss.post.reports_by_category.far_field(\"db(RealizedGainTheta)\",\n", " disc_sweep.name,\n", " sphere_name=\"3D\",\n", " Freq= [center_freq],)\n", "\n", "report_3d.report_type = \"3D Polar Plot\"\n", "report_3d.create(name=\"Realized Gain (dB)\")" ] }, { "cell_type": "markdown", "id": "1284e9c8", "metadata": {}, "source": [ "### Retrieve solution data for post-processing in Python\n", "\n", "An instance of the ``SolutionData`` class can be created from the report by calling ``get_solution_data()``. \n", "This class provides access to data for further post-processing using\n", "[Matplotlib](https://matplotlib.org/)." ] }, { "cell_type": "code", "execution_count": null, "id": "45a8ec41", "metadata": {}, "outputs": [], "source": [ "report_3d_data = report_3d.get_solution_data()\n", "new_plot = report_3d_data.plot_3d()" ] }, { "cell_type": "markdown", "id": "1163c208", "metadata": {}, "source": [ "### View cross-polarization\n", "\n", "The dipole is linearly polarized as can be seen from the comparison of $\\theta$-polarized\n", "and $\\phi$-polarized \"realized gain\" at $\\theta=90^\\circ$ degrees.\n", "The following code creates the gain plots in AEDT." ] }, { "cell_type": "code", "execution_count": null, "id": "1547a959", "metadata": {}, "outputs": [], "source": [ "xpol_expressions = [\"db(RealizedGainTheta)\", \"db(RealizedGainPhi)\"]\n", "xpol = hfss.post.reports_by_category.far_field([\"db(RealizedGainTheta)\", \"db(RealizedGainPhi)\"],\n", " disc_sweep.name,\n", " name=\"Cross Polarization\",\n", " sphere_name=\"Azimuth\",\n", " Freq= [center_freq],)\n", "\n", "xpol.report_type = \"Radiation Pattern\"\n", "xpol.create(name=\"xpol\")\n", "xpol.children[\"Legend\"].properties[\"Show Solution Name\"] = False\n", "xpol.children[\"Legend\"].properties[\"Show Variation Key\"] = False" ] }, { "cell_type": "markdown", "id": "90d3df84", "metadata": {}, "source": [ "The ``get_solution_data()`` method is again used to create an inline plot of cross-polarization from\n", "the report in HFSS." ] }, { "cell_type": "code", "execution_count": null, "id": "db3c45a1", "metadata": { "lines_to_next_cell": 2 }, "outputs": [], "source": [ "ff_el_data = elevation_ffd_plot.get_solution_data()\n", "ff_el_data.plot(x_label=\"Theta\", y_label=\"Gain\", is_polar=True)" ] }, { "cell_type": "markdown", "id": "0a37ea99", "metadata": {}, "source": [ "## Release AEDT" ] }, { "cell_type": "code", "execution_count": null, "id": "b1b21b24", "metadata": {}, "outputs": [], "source": [ "hfss.save_project()\n", "hfss.release_desktop()\n", "\n", "# Wait 3 seconds to allow AEDT to shut down before cleaning the temporary directory.\n", "time.sleep(3)" ] }, { "cell_type": "markdown", "id": "d6950edf", "metadata": {}, "source": [ "## Clean up\n", "\n", "All project files are saved in the folder ``temp_folder.name``.\n", "If you've run this example as a Jupyter notebook, you\n", "can retrieve those project files.\n", "The following cell removes all temporary files, including the project folder." ] }, { "cell_type": "code", "execution_count": null, "id": "d20293fd", "metadata": {}, "outputs": [], "source": [ "temp_folder.cleanup()" ] } ], "metadata": { "jupytext": { "cell_metadata_filter": "-all", "main_language": "python", "notebook_metadata_filter": "-all" } }, "nbformat": 4, "nbformat_minor": 5 }