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author | Thomas Stephen Lee | 2015-09-04 22:04:10 +0530 |
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committer | Thomas Stephen Lee | 2015-09-04 22:04:10 +0530 |
commit | 64419e47f762802600b3a2b6d8c433a16ccd3d55 (patch) | |
tree | 14ad7c37c9547cd516f141494f3fa375621edbaa /Fluidization_Engineering_by_K_Daizo_And_O_Levenspiel/ch10.ipynb | |
parent | 10f6fb8cd1d840a3042651dfaa6fd5af4924b94a (diff) | |
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diff --git a/Fluidization_Engineering_by_K_Daizo_And_O_Levenspiel/ch10.ipynb b/Fluidization_Engineering_by_K_Daizo_And_O_Levenspiel/ch10.ipynb new file mode 100755 index 00000000..e44d1ebe --- /dev/null +++ b/Fluidization_Engineering_by_K_Daizo_And_O_Levenspiel/ch10.ipynb @@ -0,0 +1,304 @@ +{ + "metadata": { + "name": "", + "signature": "sha256:89c91579d721ed0f833b399593203d4eb19421ab1695bc830f1be612e46bd826" + }, + "nbformat": 3, + "nbformat_minor": 0, + "worksheets": [ + { + "cells": [ + { + "cell_type": "heading", + "level": 1, + "metadata": {}, + "source": [ + "Chapter 10 : Gas Dispersion and Gas Interchange in Bubbling Beds" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "%matplotlib inline" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "\n", + "Welcome to pylab, a matplotlib-based Python environment [backend: module://IPython.zmq.pylab.backend_inline].\n", + "For more information, type 'help(pylab)'.\n" + ] + } + ], + "prompt_number": 2 + }, + { + "cell_type": "heading", + "level": 3, + "metadata": {}, + "source": [ + "Example 1, Page 253\n" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "\n", + "from numpy import *\n", + "%matplotlib inline\n", + "#Variable declaration\n", + "umf=[0.01,0.045]; #Velocity at minimum fluidization condition in m/s\n", + "ephsilonmf=[0.5,0.5]; #Void fraction at minimum fluidization condition\n", + "D=[2E-5,7E-5]; #Diffusion coefficient of gas in m**2/s\n", + "g=9.81; #Acceleration due to gravity in m/s**2\n", + "\n", + "#CALCULATION\n", + "db=[5.,10.,15.,20.];\n", + "n=len(umf);\n", + "m=len(db)\n", + "Kbc = zeros((n,m))\n", + "Kce = zeros((n,m))\n", + "Kbe = zeros((n,m))\n", + " \n", + "for i in range(n):\n", + " for j in range(m):\n", + " Kbc[i][j]=4.5*(umf[i]/db[j])+5.85*((D[i]**0.5*g**0.25)/db[j]**(5.0/4));#Gas interchange coefficient between bubble and cloud from Eqn.(27)\n", + " Kce[i][j]=6.77*((D[i]*ephsilonmf[i]*0.711*(g*db[j])**0.5)/db[j]**3)**0.5;#Gas interchange coefficient between emulsion and cloud from Eqn.(34)\n", + " Kbe[i][j]=(Kbc[i][j]*Kce[i][j])/(Kbc[i][j]+Kce[i][j]);#Gas interchange coefficient between bubble and emulsion from Eqn.(14)\n", + "\n", + "#OUTPUT\n", + "i=0;\n", + "j=0;\n", + "k=0;\n", + "while k<m*n:\n", + " print '\\t\\tKbc for fine particles and He',\n", + " print '\\tKbc for coarse particles and ozone',\n", + " print '\\tKbe for fine particles and He',\n", + " print '\\tKbe for coarse particles and ozone'\n", + " j = 0\n", + " while j<m:\n", + " print 'db=%fm'%(db[j]*10**-2);\n", + " while i<n:\n", + " print '\\t%f'%Kbc[i][j],\n", + " print '\\t\\t\\t%f'%Kbe[i][j],\n", + " i=i+1; \n", + " k=k+1;\n", + " print '\\t\\t\\t',\n", + " i=0;\n", + " j=j+1;\n", + "import numpy\n", + "import matplotlib.pyplot as plt\n", + "a = numpy.matrix(Kbe)\n", + "b = numpy.matrix(Kbc)\n", + "db = array(db).T\n", + "Kbe=a.T\n", + "Kbc=b.T\n", + "\n", + "plt.plot(db,Kbc,db,Kbe)\n", + "#plt.plot(db,Kbe);\n", + "#Note : Python does not have plot2d function. so we can plot it \n", + "#plt.title('Plot of Kbc,Kbe vs db','db');\n", + "plt.show()\n", + "print 'Comparing the points with the plot of Kbc,Kbe vs db in Fig.(12), we can conlcude the following:'\n", + "print 'Kbc for fine particles and helium: line 2 in Fig.(12)'\n", + "print 'Kbc for coarser particles and ozone: line 3 in Fig.(12)'\n", + "print 'Kbe for fine particles and helium: line 4 in Fig.(12)'\n", + "print 'Kbe for coarser particles and ozone: line 5 in Fig.(12)'\n", + "\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "\n", + "Welcome to pylab, a matplotlib-based Python environment [backend: module://IPython.zmq.pylab.backend_inline].\n", + "For more information, type 'help(pylab)'.\n" + ] + }, + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "\t\tKbc for fine particles and He \tKbc for coarse particles and ozone \tKbe for fine particles and He \tKbe for coarse particles and ozone\n", + "db=0.050000m\n", + "\t0.015193 \t\t\t0.003335 \t\t\t\t0.052085 \t\t\t0.006930 \t\t\tdb=0.100000m\n", + "\t0.007104 \t\t\t0.001434 \t\t\t\t0.025121 \t\t\t0.002964 \t\t\tdb=0.150000m\n", + "\t0.004568 \t\t\t0.000875 \t\t\t\t0.016434 \t\t\t0.001803 \t\t\tdb=0.200000m\n", + "\t0.003345 \t\t\t0.000616 \t\t\t\t0.012173 \t\t\t0.001266 \t\t\t" + ] + }, + { + "metadata": {}, + "output_type": "display_data", + "png": 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0ZOQ/m48FexegXlePl2e/LHUkIuoHvAatnfq65muE7QvDStVKvKF5AzKZTOpIRGQBXnCc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\nkCHiGTl37ACKi8V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htvj329jYiNu3b+PEiROIiYnBCy+8IHUks9auXYsNGzZAq9Vi/fr1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\nRU5ErkJggg==\n" + }, + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "Comparing the points with the plot of Kbc,Kbe vs db in Fig.(12), we can conlcude the following:\n", + "Kbc for fine particles and helium: line 2 in Fig.(12)\n", + "Kbc for coarser particles and ozone: line 3 in Fig.(12)\n", + "Kbe for fine particles and helium: line 4 in Fig.(12)\n", + "Kbe for coarser particles and ozone: line 5 in Fig.(12)\n" + ] + } + ], + "prompt_number": 1 + }, + { + "cell_type": "heading", + "level": 3, + "metadata": {}, + "source": [ + "Example 2, Page 254\n" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "\n", + "D=0.69; #Diffusion coefficient of gas in cm**2/s\n", + "umf=1.0; #Velocity at minimum fluidization condition in cm/s\n", + "ephsilonmf=0.5; #Void fraction at minimum fluidization condition\n", + "db=[5,15]; #Equilibrium bubble size in cm\n", + "g=980; #Acceleration due to gravity in cm/s**2\n", + "\n", + "#CALCULATION\n", + "n=len(db);\n", + "i=0;\n", + "Kbc = [0.,0.]\n", + "Kce = [0.,0.]\n", + "Kbe = [0.,0.]\n", + "e = [0.,0.]\n", + "while i<n:\n", + " Kbc[i]=4.5*(umf/db[i])+5.85*((D**0.5*g**0.25)/db[i]**(5/4));#Gas interchange coefficient between bubble and cloud from Eqn.(27)\n", + " Kce[i]=6.77*((D*ephsilonmf*0.711*(g*db[i])**0.5)/db[i]**3)**0.5;#Gas interchange coefficient between emulsion and cloud from Eqn.(34)\n", + " Kbe[i]=(Kbc[i]*Kce[i])/(Kbc[i]+Kce[i]);#Gas interchange coefficient between bubble and emulsion from Eqn.(14)\n", + " e[i]=(Kce[i]-Kbe[i])/Kbe[i];#Error when minor resistance is ignored\n", + " i=i+1;\n", + "\n", + "#OUTPUT\n", + "print 'db(cm)',\n", + "print '\\t\\tCalculated Kbc',\n", + "print '\\tCalculated Kce',\n", + "print '\\t\\tKbe from Eqn.(14)',\n", + "print '\\tErron when minor resistance is ignored (in percentage)'\n", + "i=0;\n", + "while i<n:\n", + " print '%f'%db[i],\n", + " print '\\t%f'%Kbc[i],\n", + " print '\\t%f'%Kce[i],\n", + " print '\\t\\t%f'%Kbe[i],\n", + " print '\\t\\t%f'%(e[i]*100);\n", + " i=i+1; \n", + "\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "db(cm) \t\tCalculated Kbc \tCalculated Kce \t\tKbe from Eqn.(14) \tErron when minor resistance is ignored (in percentage)\n", + "5.000000 \t6.337721 \t2.509152 \t\t1.797506 \t\t39.590766\n", + "15.000000 \t2.112574 \t0.635514 \t\t0.488547 \t\t30.082477\n" + ] + } + ], + "prompt_number": 2 + }, + { + "cell_type": "heading", + "level": 3, + "metadata": {}, + "source": [ + "Example 3, Page 255\n" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "\n", + "Kbe=[0.028,0.05]; #Reported range for gas interchange coefficient between bubble and emulsion\n", + "uo=0.30; #Superficial gas velocity in m/s\n", + "db=0.13; #Equilibrium bubble size in m\n", + "m=7;\n", + "ephsilonmf=0.5; #Void fraction at minimum fluidization condition\n", + "umf=0.0018; #Velocity at minimum fluidization condition in m/s\n", + "D=[9E-6,22E-6]; #Diffusion coefficient of gas in m**2/s\n", + "g=9.81; #Acceleration due to gravity in m/s**2\n", + "\n", + "#CALCULATION\n", + "n=len(Kbe);\n", + "i=0;\n", + "Kbem = [0,0]\n", + "Kbc = [0,0]\n", + "Kce = [0,0]\n", + "#Kbe = [0,0]\n", + "c = [0,0]\n", + "\n", + "while i<n:\n", + " Kbem[i]=(6.0/db)*Kbe[i];#Gas interchange coefficient between bubble and emulsion from Eqn.(19)\n", + " Kbc[i]=4.5*(umf/db)+5.85*((D[i]**0.5*g**0.25)/db**(5.0/4));#Gas interchange coefficient between bubble and cloud from Eqn.(27)\n", + " Kce[i]=6.77*((D[i]*ephsilonmf*0.711*(g*db)**0.5)/db**3)**0.5;#Gas interchange coefficient between emulsion and cloud from Eqn.(34)\n", + " Kbe[i]=(Kbc[i]*Kce[i])/(Kbc[i]+Kce[i]);#Gas interchange coefficient between bubble and emulsion from Eqn.(14)\n", + " c[i]=(Kbem[i]/Kbe[i]);\n", + " i=i+1;\n", + "\n", + "#OUTPUT\n", + "print 'Kbe from Eqn.(19)',\n", + "print '\\tKbc from Eqn.(27)',\n", + "print '\\tKce from Eqn.(34)',\n", + "print '\\tKbe from Eqn.(14)',\n", + "print '\\tComparison of Kbe from Eqn.(19) and that from Eqn.(14)'\n", + "i=0\n", + "while i<n:\n", + " print '%f'%Kbem[i],\n", + " print '\\t\\t%f'%Kbc[i],\n", + " print '\\t\\t%f'%Kce[i],\n", + " print '\\t\\t%f'%Kbe[i],\n", + " print '\\t\\t%f'%c[i]\n", + " i=i+1; \n", + "\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "Kbe from Eqn.(19) \tKbc from Eqn.(27) \tKce from Eqn.(34) \tKbe from Eqn.(14) \tComparison of Kbe from Eqn.(19) and that from Eqn.(14)\n", + "1.292308 \t\t0.460200 \t\t0.274548 \t\t0.171959 \t\t7.515188\n", + "2.307692 \t\t0.684401 \t\t0.429248 \t\t0.263797 \t\t8.747978\n" + ] + } + ], + "prompt_number": 3 + }, + { + "cell_type": "code", + "collapsed": false, + "input": [], + "language": "python", + "metadata": {}, + "outputs": [] + } + ], + "metadata": {} + } + ] +}
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