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author | Prashant S | 2020-04-14 10:25:32 +0530 |
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committer | GitHub | 2020-04-14 10:25:32 +0530 |
commit | 06b09e7d29d252fb2f5a056eeb8bd1264ff6a333 (patch) | |
tree | 2b1df110e24ff0174830d7f825f43ff1c134d1af /Applied_Physics_ii_by_H_J_Sawant/4-Lasers.ipynb | |
parent | abb52650288b08a680335531742a7126ad0fb846 (diff) | |
parent | 476705d693c7122d34f9b049fa79b935405c9b49 (diff) | |
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diff --git a/Applied_Physics_ii_by_H_J_Sawant/4-Lasers.ipynb b/Applied_Physics_ii_by_H_J_Sawant/4-Lasers.ipynb new file mode 100644 index 0000000..00c42dc --- /dev/null +++ b/Applied_Physics_ii_by_H_J_Sawant/4-Lasers.ipynb @@ -0,0 +1,135 @@ +{ +"cells": [ + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "# Chapter 4: Lasers" + ] + }, +{ + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 4.6_1: find_the_number_of_emitted_photons.sce" + ] + }, + { +"cell_type": "code", + "execution_count": null, + "metadata": { + "collapsed": true + }, + "outputs": [], +"source": [ +"//Chapter-4,Example4_6_1,pg 4-7\n", +"\n", +"P=3.147*10^-3 //output power \n", +"\n", +"t=60 //time\n", +"\n", +"wavelength=632.8*10^-9 //wavelength of He-Ne laser\n", +"\n", +"h=6.63*10^-34 //Plancks constant\n", +"\n", +"c=3*10^8 //velocity of light in air\n", +"\n", +"N=P*t*wavelength/(h*c) //No. of photons emitted \n", +"\n", +"printf('\nNo. of photons emitted each minute\n')\n", +"\n", +"disp(N)" + ] + } +, +{ + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 4.6_2: find_the_ratio_of_population_of_two_energy_levels.sce" + ] + }, + { +"cell_type": "code", + "execution_count": null, + "metadata": { + "collapsed": true + }, + "outputs": [], +"source": [ +"//Chapter-4,Example4_6_2,pg 4-7\n", +"\n", +"wavelength=694.3*10^-9 //wavelength of He-Ne laser\n", +"\n", +"h=6.63*10^-34 //Plancks constant\n", +"\n", +"c=3*10^8 //velocity of light in air\n", +"\n", +"k=1.38*10^-23 //Boltzmann constant\n", +"\n", +"T=300 //ambient temperature in kelvin\n", +"\n", +"ratio=%e^-(h*c/(wavelength*k*T)) //ratio of population of two energy level in laser \n", +"\n", +"printf('\nRatio of population of two energy level in laser N2/N1 is\n')\n", +"\n", +"disp(ratio)" + ] + } +, +{ + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Example 4.6_3: calculate_the_wavelength_of_photons.sce" + ] + }, + { +"cell_type": "code", + "execution_count": null, + "metadata": { + "collapsed": true + }, + "outputs": [], +"source": [ +"//Chapter-4,Example4_6_3,pg 4-8\n", +"\n", +"P=100*10^3 //avrage power per pulse\n", +"\n", +"t=20*10^-9 //time duration\n", +"\n", +"h=6.63*10^-34 //Plancks constant\n", +"\n", +"c=3*10^8 //velocity of light in air\n", +"\n", +"N=6.981*10^15 //No. of photons per pulse\n", +"\n", +"wavelength=N*h*c/(P*t)*10^10 \n", +"\n", +"printf('\nWavelength of photons = %.f A.\n',wavelength)\n", +"" + ] + } +], +"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 +} |