{ "cells": [ { "cell_type": "markdown", "metadata": {}, "source": [ "# FMCW Radar 206 - Reflections" ] }, { "cell_type": "markdown", "metadata": { "id": "ievkv-71F_zH" }, "source": [ "swra705.pdf 2.9 is given in Table 3-1 as the permittivity for polycarbonate.\n", "\n", "| Material | Permitiviy | Dissipation |\n", "|---|---|---|\n", "| polycarbonate | 2.9 |0.012 |\n", "\n", "swra705 Equation 4 is:\n", "\n", "\\begin{align}\n", "\\lambda_m = \\frac{c}{f \\cdot \\sqrt{\\epsilon_R}}\n", "\\tag{0}\n", "\\end{align}\n", "\n", "$$ \\iff \\lambda_{void} = \\lambda_m \\cdot \\sqrt{\\epsilon_R}$$\n", "\n", "Refractive index n is defined as\n", "\n", "$n = \\frac{c}{v} \\iff c = v \\cdot n$\n", "\n", "and,\n", "\n", "$\\lambda_{medium} = \\frac {v_{medium}}{f} $\n", "\n", "\\begin{align}\n", "\\frac{\\lambda_{void}}{\\lambda_{polycarbonate}}\n", "= \\frac{\\frac{v_{void}}{f}}{\\frac {v_{poly}}{f}}\n", "= \\frac {v_{void}}{v_{poly}}\n", "= n\n", "\\iff\n", "\\lambda_{void}= n \\cdot \\lambda_{polycarbonate}\n", "\\tag{1.1}\n", "\\end{align}\n", "\n", "as per this online tutorial: https://www.tf.uni-kiel.de/matwis/amat/elmat_en/kap_3/backbone/r3_7_2.html\n", "\n", "$$n^2 = \\epsilon_R$$\n", "\n", "\n", "\n" ] }, { "cell_type": "code", "execution_count": null, "metadata": { "colab": { "base_uri": "https://localhost:8080/" }, "id": "AvQ1zGxRFRGB", "outputId": "c7e40289-5023-41e2-a49e-3d6d8547f999" }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "1.70293863659264\n" ] } ], "source": [ "from numpy import sqrt\n", "epsilon_R = 2.9\n", "n = 1.586\n", "print(sqrt(epsilon_R))" ] } ], "metadata": { "colab": { "provenance": [] }, "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": 4 }