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diff --git a/Electronic_Communication_by_D_Roddy/16-ANTENNAS.ipynb b/Electronic_Communication_by_D_Roddy/16-ANTENNAS.ipynb new file mode 100644 index 0000000..37ad774 --- /dev/null +++ b/Electronic_Communication_by_D_Roddy/16-ANTENNAS.ipynb @@ -0,0 +1,129 @@ +{ +"cells": [ + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "# Chapter 16: ANTENNAS" + ] + }, +{ + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 16.19_1: example_3.sce" + ] + }, + { +"cell_type": "code", + "execution_count": null, + "metadata": { + "collapsed": true + }, + "outputs": [], +"source": [ +"clc;\n", +"//prob no. 16.19.1\n", +"// Paraboloida reflector antenna is given with\n", +"D=6;//reflector diameter in m\n", +"n=0.65;//illumination effeciency\n", +"f=10^10;//frequency of operation in Hz\n", +"c=3*10^8;//velo of light in m/s\n", +"wl=c/f;\n", +"A=(%pi*D^2)/4;\n", +"A_eff=n*A;\n", +"disp('m^2',A_eff,'Effective area is');\n", +"D0=4*%pi*A_eff/wl^2;\n", +"disp(D0,'The directivity is');\n", +"BW_dB=70*wl/D;\n", +"disp('degree',BW_dB,'The -3dB beamwidth is');\n", +"BW_null=2*BW_dB;\n", +"disp('degree',BW_null,'The null beamwidth is');" + ] + } +, +{ + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 16.7_2: example_1.sce" + ] + }, + { +"cell_type": "code", + "execution_count": null, + "metadata": { + "collapsed": true + }, + "outputs": [], +"source": [ +"clc;\n", +"//page no 590\n", +"//prob no. 16.7.2\n", +"//For the Hertzian dipole, the radiation pattern is described by g(x)=sin^2(x) and g(y)=1\n", +"// Determination of -3dB beamwidth\n", +"// from the polar diagram shown we have\n", +"g_x=0.5;\n", +"x=asind(sqrt(g_x));\n", +"g_y=0.5;\n", +"y1=asind(sqrt(g_y));\n", +"y=y1+90;\n", +"//Therefore\n", +"z=y-x;\n", +"disp('degree',z,'The -3dB beamwidth is');" + ] + } +, +{ + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 16.9_1: example_2.sce" + ] + }, + { +"cell_type": "code", + "execution_count": null, + "metadata": { + "collapsed": true + }, + "outputs": [], +"source": [ +"clc;\n", +"//prob no. 16.9.1\n", +"//Half dipole antenna is given with I=Io*cos(Bl) where l=0\n", +"//The physical length of the antenna is wl/2\n", +"//consider wl=unity and current Io=unity\n", +"Io=1;\n", +"wl=1;\n", +"phy_length=wl/2;\n", +"I_av=2*Io/%pi;\n", +"//Thus area is given as \n", +"Area=I_av*phy_length;\n", +"// From the above eq l_effective is given as\n", +"disp('l_eff= wl/pi');" + ] + } +], +"metadata": { + "kernelspec": { + "display_name": "Scilab", + "language": "scilab", + "name": "scilab" + }, + "language_info": { + "file_extension": ".sce", + "help_links": [ + { + "text": "MetaKernel Magics", + "url": "https://github.com/calysto/metakernel/blob/master/metakernel/magics/README.md" + } + ], + "mimetype": "text/x-octave", + "name": "scilab", + "version": "0.7.1" + } + }, + "nbformat": 4, + "nbformat_minor": 0 +} |