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author | Trupti Kini | 2016-09-09 23:30:25 +0600 |
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committer | Trupti Kini | 2016-09-09 23:30:25 +0600 |
commit | 5e4af9aebb389109363666017f67e986e96a9906 (patch) | |
tree | c742461131f848fc6bc7a1938672eba69f20ceb2 /Heat_Transfer_in_SI_units_by_Holman/Chapter11.ipynb | |
parent | cd810407802a7f89116285be29c37f8e4c477111 (diff) | |
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Added(A)/Deleted(D) following books
A Heat_Transfer_Principles_And_Applications_by_Dutta/README.txt
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch10.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch11.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch2.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch3.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch4.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch5.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch6.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch7.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch8.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/ch9.ipynb
A Heat_Transfer_Principles_And_Applications_by_Dutta/screenshots/10.png
A Heat_Transfer_Principles_And_Applications_by_Dutta/screenshots/5.png
A Heat_Transfer_Principles_And_Applications_by_Dutta/screenshots/51.png
A Heat_Transfer_in_SI_units_by_Holman/Chapter1.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter10.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter11.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter2.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter3.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter4.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter5.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter6.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter7.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter8.ipynb
A Heat_Transfer_in_SI_units_by_Holman/Chapter9.ipynb
A Heat_Transfer_in_SI_units_by_Holman/README.txt
A Heat_Transfer_in_SI_units_by_Holman/screenshots/9.1.png
A Heat_Transfer_in_SI_units_by_Holman/screenshots/9.2.png
A Heat_Transfer_in_SI_units_by_Holman/screenshots/9.4.png
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter1.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter2.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter3.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter4.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter5.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter6.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter7.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter8.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/Chapter9.ipynb
A Power_Electronics_Principles_and_Applications_by_Jacob/README.txt
A Power_Electronics_Principles_and_Applications_by_Jacob/screenshots/4.png
A Power_Electronics_Principles_and_Applications_by_Jacob/screenshots/5.png
A Power_Electronics_Principles_and_Applications_by_Jacob/screenshots/6.png
A sample_notebooks/AviralYadav/Chapter5.ipynb
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diff --git a/Heat_Transfer_in_SI_units_by_Holman/Chapter11.ipynb b/Heat_Transfer_in_SI_units_by_Holman/Chapter11.ipynb new file mode 100644 index 00000000..764a2588 --- /dev/null +++ b/Heat_Transfer_in_SI_units_by_Holman/Chapter11.ipynb @@ -0,0 +1,254 @@ +{ + "cells": [ + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "# Chapter 11 Mass Transfer" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Exa 11.1" + ] + }, + { + "cell_type": "code", + "execution_count": 1, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "value of diffusion coefficient for co2 in air is 0.132 square centimeter/s\n", + "From Table A-8,D=0.164 sq cm/s\n", + " So,they are in fair agreement\n" + ] + } + ], + "source": [ + "#Example Number 11.1\n", + "# diffusion coefficient for co2\n", + "\n", + "# Variable declaration\n", + "\n", + "T =298.0\t\t\t# [K] temperature of air\n", + "Vco2 = 34.0 \t\t\t# molecular volume of co2\n", + "Vair = 29.9 \t\t\t# molecular volume of air\n", + "Mco2 = 44.0 \t\t\t# molecular weight of co2\n", + "Mair = 28.9 \t\t\t# molecular weight of air\n", + "P = 1.0132*10**(5) \t\t# [Pa] atmospheric pressure\n", + "\t# using equation (11-2)\n", + "#Calculation\n", + "D = 435.7*T**(3.0/2.0)*(((1/Mco2)+(1/Mair))**(1.0/2.0))/(P*(Vco2**(1.0/3.0)+Vair**(1.0/3.0))**(2)) \n", + "\n", + "#Result\n", + "print \"value of diffusion coefficient for co2 in air is\",round(D,3),\"square centimeter/s\" \n", + "print \"From Table A-8,D=0.164 sq cm/s\\n So,they are in fair agreement\"\n" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Exa 11.3" + ] + }, + { + "cell_type": "code", + "execution_count": 4, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Temperature of dry air is 53.66 degree celsius\n", + " recalculate the density at the arithmetic-average temperature between wall and free-stream conditions\n", + "With this adjustments these results are RHO = 1.143 kg/m**(3) and Tinf = 55.8 degree celcius\n" + ] + } + ], + "source": [ + "#Example Number 11.3\n", + "# Wet-bulb temperature\n", + "\n", + "#Variable declaration\n", + "\n", + "Pg = 2107.0\t\t\t# [Pa] from steam table at 18.3 degree celcius\n", + "Pw = Pg*18.0 \t\t\t# [Pa]\n", + "Rw = 8315.0 \t\t\t# [J/mol K] gas constant\n", + "Tw = 273+18.3\t \t\t# [K]\n", + "\n", + "RHOw = Pw/(Rw*Tw) \t\t# [kg/cubic meter]\n", + "\n", + "\n", + "Cw = RHOw \t\t\t# [kg/cubic meter]\n", + "RHOinf = 0.0 \t\t\t# since the free stream is dry air\n", + "Cinf = 0.0 \n", + "P = 1.01325*10**(5) \t\t# [Pa]\n", + "R = 287 \t\t\t# [J /kg K]\n", + "T = Tw \t\t\t\t# [K]\n", + "RHO = P/(R*T) \t\t\t# [kg/cubic meter]\n", + "\n", + "Cp = 1004.0 \t\t\t# [J/kg degree celsius]\n", + "Le = 0.845 \n", + "Hfg = 2.456*10**(6) \t\t# [J/kg]\n", + "#Calculations\n", + "# now using equation(11-31)\n", + "\n", + "Tinf = (((Cw-Cinf)*Hfg)/(RHO*Cp*(Le**(2.0/3.0))))+Tw \t# [K]\n", + "Tin = Tinf-273 \t\t\t\t\t# [degree celsius]\n", + "\n", + "print \"Temperature of dry air is\",round(Tin,2),\"degree celsius\" \n", + "print \" recalculate the density at the arithmetic-average temperature between wall and free-stream conditions\" \n", + "print \"With this adjustments these results are RHO = 1.143 kg/m**(3) and Tinf = 55.8 degree celcius\"\n", + "\n" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Exa 11.4" + ] + }, + { + "cell_type": "code", + "execution_count": 5, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Relative humidity is therefore 27.8 percentage\n" + ] + } + ], + "source": [ + "#Example Number 11.4\n", + "# relative humidity of air stream\n", + "\n", + "#Variable declaration\n", + "\n", + "\t\t# these data were taken from previous example\n", + "Rho = 1.212 \t\t\t\t\t# [kg/cubic meter]\n", + "Cp = 1004 \t\t\t\t\t# [J/kg]\n", + "Le = 0.845 \n", + "Tw = 18.3 \t\t\t\t\t# [degree celsius]\n", + "Tinf = 32.2 \t\t\t\t\t# [degree celsius]\n", + "Rhow = 0.015666 \t\t\t\t# [kg/cubic meter]\n", + "Cw = Rhow \t\t\t\t\t# [kg/cubic meter]\n", + "\n", + "#calculation\n", + "\n", + "Hfg = 2.456*10**(6) \t\t\t\t# [J/kg]\n", + "\t\t# we use eqn 11-31\n", + "Cinf = Cw-(Rho*Cp*Le**(2.0/3.0)*(Tinf-Tw)/Hfg) \t# [kg/cubic meter]\n", + "Rhoinf = Cinf \t\t\t\t\t# [kg/cubic meter]\n", + "Rhog = 0.0342 \t\t\t\t\t# [kg/cubic meter]\n", + "RH = (Rhoinf/Rhog)*100 \n", + "\n", + "#Result\n", + "\n", + "print \"Relative humidity is therefore\",round(RH,1),\"percentage\" \n" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Exa 11.5" + ] + }, + { + "cell_type": "code", + "execution_count": 6, + "metadata": { + "collapsed": false + }, + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "Evaporation rate on the land under these conditions is 0.0028 kg/h square meter\n" + ] + } + ], + "source": [ + "#Example Number 11.5\n", + "# water evaporation rate\n", + "\n", + "# Variable declaration\n", + "\n", + "Ta = 38+273 \t\t\t# [K] temperature of atmospheric air\n", + "RH = 0.30 \t\t\t# relative humidity\n", + "u = 10.0\t\t\t# [mi/h] mean wind speed\n", + "R = 0.287 \t\t\t# universal gas constant\n", + "Dw = 0.256*10**(-4) \t\t# [square meter/s] from table A-8(page no.-610)\n", + "rho_w = 1000 \t\t\t# [kg/cubic meter]\n", + "\t# for this calculation we can make use of equation(11-36). from thermodynamic \tsteam tables\n", + "p_g = 6.545 \t\t\t# [kPa] at 38 degree celsius\n", + "p_s = p_g \t\t\t# [kPa]\n", + "p_w = RH*p_s \t\t\t# [kPa]\n", + "p_s = 1.933 \t\t\t# [in Hg]\n", + "p_w = 0.580 \t\t\t# [in Hg]\n", + "\t# also \n", + "u_bar = u*24 \t\t\t# [mi/day]\n", + "\t# equation(11-36) yields, with the application of the 0.7 factor\n", + "\n", + "E_lp = 0.7*(0.37+0.0041*u_bar)*(p_s-p_w)**(0.88) \t\t# [in/day]\n", + "E_lp = E_lp*2.54/100 \t\t\t\t\t\t# [m/day]\n", + "\n", + "\t# noting that standard pan has the diameter of 1.2m, we can use the figure to \t\tcalculate the mass evaporation rate per unit area as\n", + "m_dot_w_by_A = E_lp*rho_w/24 \t\t\t\t# [kg/h square meter]\n", + "\n", + "\n", + "\t# as a matter of interest, we might calculate the molecular-diffusion rate of \t\twater vapour from equation(11-35), taking z1 as the 1.5m dimension above the \t\tstandard pan.\n", + "z1 = 1.5 \t\t\t\t\t\t\t# [m]\n", + "\n", + "\t# since rho = p/(R*T)\n", + "\t# equation(11-35) can be written as \n", + "m_dot_w_by_A1 = 0.622*Dw*p_g*3600/(R*Ta*z1) \t\t\t# [kg/h square meter]\n", + "\n", + "#Result\n", + "\n", + "print \"Evaporation rate on the land under these conditions is\",round(m_dot_w_by_A1,4),\"kg/h square meter\"\n", + "\n", + "\n" + ] + } + ], + "metadata": { + "kernelspec": { + "display_name": "Python 2", + "language": "python", + "name": "python2" + }, + "language_info": { + "codemirror_mode": { + "name": "ipython", + "version": 2 + }, + "file_extension": ".py", + "mimetype": "text/x-python", + "name": "python", + "nbconvert_exporter": "python", + "pygments_lexer": "ipython2", + "version": "2.7.6" + } + }, + "nbformat": 4, + "nbformat_minor": 0 +} |