{ "cells": [ { "cell_type": "markdown", "id": "652b8f17-158b-4a87-bf93-0174886a76ef", "metadata": {}, "source": [ "# FMCW Radar 108 - Antennas\n", "\n", "While it is beyond the scope of this writeup to cover the details of antenna designs. A few key points will be covered here." ] }, { "cell_type": "markdown", "id": "2a2e9f50-68a6-45a8-86c8-814503a6c89d", "metadata": {}, "source": [ "## Different types of antennas\n" ] }, { "cell_type": "markdown", "id": "39d912b5-fa98-4d56-bdce-f86c3e102e04", "metadata": {}, "source": [ "## Antenna patches\n", "\n", "### Fundamental Resonant Frequency\n", "\n", "The resonant frequency of a patch antenna depends on its physical dimensions, the dielectric material, and the mode of operation. For a rectangular microstrip patch antenna, the fundamental resonant frequency (dominant mode, TM₁₀ mode) is approximately given by:\n", "\n", "$$ f_r = \\frac{c}{2L \\sqrt{\\varepsilon_r^{\\text{eff}}}} $$\n", "\n", "where:\n", "\n", "- c is the speed of light in vacuum (3 \\times 10^8 m/s),\n", "- L is the length of the patch,\n", "- $\\varepsilon_r^{\\text{eff}}$ is the effective permittivity of the dielectric substrate, given by:\n", "\n", "$$\\varepsilon_r^{\\text{eff}} = \\frac{\\varepsilon_r + 1}{2} + \\frac{\\varepsilon_r - 1}{2} \\left( 1 + 12 \\frac{h}{W} \\right)^{-1/2}$$\n", "\n", "where:\n", "\n", "- $\\varepsilon_r$ is the relative permittivity of the substrate,\n", "- h is the substrate thickness,\n", "- W is the width of the patch.\n", "\n", "### Higher-Order Modes\n", "\n", "It should be noted that while the main mode offers the highest radiation efficiency (i.e. ratio of Pout/Pin, not to be confused with impedance matching - as a 50 Ohm impedance has perfect matching but zero radiations).\n", "\n", "Other modes such as TM₀₁ and TM₁₁ have different resonance conditions. While they have lower efficiency, they may provide in systems with strong space constraints lower footprint.\n", "\n", "$ f_{mn} = \\frac{c}{2} \\sqrt{\\left(\\frac{m}{L}\\right)^2 + \\left(\\frac{n}{W}\\right)^2} \\cdot \\frac{1}{\\sqrt{\\varepsilon_r^{\\text{eff}}}}$\n", "\n", "where m, n are the mode indices.\n", "\n", "Key Factors Affecting Resonance\n", "\n", "1. Patch Size: A larger patch lowers the resonant frequency.\n", "\n", "2. Dielectric Constant: A higher \\varepsilon_r lowers the resonant frequency.\n", "\n", "3. Substrate Thickness: Increasing h affects effective permittivity and bandwidth.\n", "\n", "4. Edge Effects: Fringing fields increase the effective electrical length, reducing resonance slightly.\n", "\n" ] } ], "metadata": { "kernelspec": { "display_name": "Python 3 (ipykernel)", "language": "python", "name": "python3" }, "language_info": { "codemirror_mode": { "name": "ipython", "version": 3 }, "file_extension": ".py", "mimetype": "text/x-python", "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython3", "version": "3.10.9" } }, "nbformat": 4, "nbformat_minor": 5 }