{ "cells": [ { "cell_type": "markdown", "metadata": {}, "source": [ "# Chapter18 Spectroscopy" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 18.1, Page no.69" ] }, { "cell_type": "code", "execution_count": 4, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "energy in ergs = 95.3 K cal moleˆ−1\n" ] } ], "source": [ "import math\n", "#initialisation of variables\n", "l=3000 #A\n", "h=6.62*10** -27 # erg sec\n", "c=3*10**10 #cm/ sec\n", "N=6*10**23 \n", "#CALCULATIONS\n", "E=h*c/(l*10**-8)\n", "E1=E*N/(4.18*10**7) \n", "#RESULTS\n", "E1=E1+276\n", "E1=E1/10**3\n", "E1=round(E1,1)\n", "print 'energy in ergs =',E1,'K cal moleˆ−1'" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 18.2, Page no.69" ] }, { "cell_type": "code", "execution_count": 2, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "energy in electron = 4.0 electron volts\n" ] } ], "source": [ "import math\n", "#initialisation of variables\n", "E=95300 # cal moleˆ−1 \n", "l=3000 #A\n", "e=23060 # cal moleˆ−1 evˆ−1 \n", "#CALCULATIONS \n", "e1=E/e \n", "#RESULTS\n", "e1=round(e1,3)\n", "print 'energy in electron =',e1,'electron volts'" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 18.3, Page no.70" ] }, { "cell_type": "code", "execution_count": 10, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "perentage transmmitancy= 56.1 percent\n" ] } ], "source": [ "import math\n", "#initialisation of variables\n", "p=19.2 # percent\n", "b=1 #cm\n", "c=5*10**-4 #mole l ˆ−1\n", "m=1.75*10** -4 #M\n", "#CALCULATIONS\n", "As=math.log10 (100/p)\n", "am=As/(b*c) \n", "r=100/10**(am*m) \n", "#RESULTS \n", "r=round(r,1)\n", "print 'perentage transmmitancy=',r,'percent'" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 18.4, Page no.70" ] }, { "cell_type": "code", "execution_count": 4, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "perentage = 25.217 percent\n" ] } ], "source": [ "import math\n", "#initialisation of variables\n", "a=193 #moleˆ−1 cmˆ−1 \n", "b=2 #cm \n", "c=1.55*10** -3 #mole l ˆ−1 \n", "#CALCULATIONS \n", "r=100/10**(a*b*c) \n", "#RESULTS \n", "r=round(r,3)\n", "print 'perentage =',r,'percent'" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 18.5, Page no.71" ] }, { "cell_type": "code", "execution_count": 3, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "reduced mass = 1.64 *10**-24 g\n", "moment of inertia = 2.7 * 10**-40 g cmˆ2\n" ] } ], "source": [ "import math\n", "#initialisation of variables\n", "m=1.008 #gms\n", "m1=36.98 #gm\n", "N=6*10**23 # molecules\n", "r=1.275*10** -8 #cm\n", "#CALCULATIONS\n", "u=m*m1/(N*(m+m1))\n", "I=u*r**2 \n", "#RESULTS \n", "u=u*10**24\n", "u=round(u,2)\n", "I=I*10**40\n", "I=round(I,1)\n", "print 'reduced mass =',u,'*10**-24 g'\n", "print 'moment of inertia =',I,'* 10**-40 g cmˆ2'" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 18.6, Page no.71" ] }, { "cell_type": "code", "execution_count": 6, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "frequency = 21.133 cmˆ−1\n" ] } ], "source": [ "import math\n", "#initialisation of variables\n", "from math import pi\n", "h=6.625*10**-27 # erg sec \n", "c= 3*10**10 #cm secˆ−1 \n", "k= 2.647*10** -40 #gm cmˆ2 \n", "#CALCULATIONS \n", "v=h/(4*pi**2*k*c) \n", "#RESULTS\n", "v=round(v,3)\n", "print 'frequency =',v,'cmˆ−1'" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 18.7, Page no.71" ] }, { "cell_type": "code", "execution_count": 7, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "force constant = 505321.24 dyne cmˆ−1\n" ] } ], "source": [ "import math\n", "#initialisation of variables\n", "v=8.867*10**13 # secˆ−1 \n", "u=1.628*10**-24 #gms \n", "#CALCULATIONS \n", "k=(pi*2*v)**2*u \n", "#RESULTS \n", "k=round(k,2)\n", "print 'force constant =',k,'dyne cmˆ−1'" ] }, { "cell_type": "markdown", "metadata": {}, "source": [ "## Example 18.8, Page no.72" ] }, { "cell_type": "code", "execution_count": 8, "metadata": { "collapsed": false }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "dissociation energy = 109.48 kcal moleˆ−1\n", "dissociation energy = 38299.56 cmˆ−1\n" ] } ], "source": [ "import math\n", "#initialisation of variables\n", "e=23.06 # kcal moleˆ−1\n", "E=4.476 # ev\n", "h=6.627*10** -27 # ergs sec\n", "c=3*10**10 #cm/ sec\n", "v=4395 #cmˆ−1\n", "e1=8060 # ev\n", "N=6*10**23 \n", "#CALCULATIONS\n", "D=E*e+(h*c*N*v/(2*10**3*4.184*10**7))\n", "D1=E*e1+(v/2)\n", "D=round(D,2)\n", "#RESULTS\n", "print 'dissociation energy =',D,'kcal moleˆ−1'\n", "print 'dissociation energy =',D1+26,'cmˆ−1'" ] } ], "metadata": { "anaconda-cloud": {}, "kernelspec": { "display_name": "Python [Root]", "language": "python", "name": "Python [Root]" }, "language_info": { "codemirror_mode": { "name": "ipython", "version": 2 }, "file_extension": ".py", "mimetype": "text/x-python", "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython2", "version": "2.7.11" } }, "nbformat": 4, "nbformat_minor": 0 }