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parentabb52650288b08a680335531742a7126ad0fb846 (diff)
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Diffstat (limited to 'Thermodynamics_for_Engineers_by_J_S_Doolittle')
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/10-Vapors.ipynb465
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/11-Thermodynamics_of_Fluid_flow.ipynb461
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/12-Heat_Transfer.ipynb477
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/13-Non_reactive_and_reactive_gaseous_mixtures.ipynb518
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/14-Energies_associated_with_chemical_reactions.ipynb329
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/15-Thermodynamics_of_chemical_reactions.ipynb137
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/16-Gas_cycles.ipynb211
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/17-Internal_combustion_engines.ipynb114
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/18-Gas_Compressors.ipynb279
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/19-Gas_turbines.ipynb510
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/20-Vapor_power_cycles.ipynb276
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/21-Steam_turbines.ipynb360
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/22-Refrigeration.ipynb277
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/23-Gas_vapor_mixtures.ipynb319
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/5-Actual_Gases.ipynb167
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/7-Entropy.ipynb67
-rw-r--r--Thermodynamics_for_Engineers_by_J_S_Doolittle/8-Availability_of_Energy.ipynb108
17 files changed, 5075 insertions, 0 deletions
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/10-Vapors.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/10-Vapors.ipynb
new file mode 100644
index 0000000..54358be
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/10-Vapors.ipynb
@@ -0,0 +1,465 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 10: Vapors"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.10: Enthalpy_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 1 of keenan and keynes,')\n",
+"in=440000 //lb/hr\n",
+"out=255000 //lb/hr\n",
+"p1=400 //psia\n",
+"t1=700 //F\n",
+"p2=35 //psia\n",
+"t2=290 //F\n",
+"vel=500 //ft/s\n",
+"hp=44000 //hp\n",
+"ent=1362.7 //Btu/lb\n",
+"//calculations\n",
+"ein=ent*in\n",
+"eout=hp*2544 + out*1183 + 925000\n",
+"h2= (ein-eout)/185000\n",
+"//results\n",
+"printf('Specific enthalpy of exhaust steam = %d Btu/lb',h2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.11: Loss_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 1 of keenan and keynes,')\n",
+"h1=1351.1 //Btu/lb\n",
+"p1=600 //psia\n",
+"t1=700 //F\n",
+"p2=234 //psia\n",
+"h2=1.6865\n",
+"h1=1.5875\n",
+"t3=101.74\n",
+"//calculations\n",
+"t2=660 //F\n",
+"loss= (h2-h1)*(t3+459.69)\n",
+"//results\n",
+"printf('Final state of steam is %d psia and %d F',p2,t2)\n",
+"printf('\n Loss of available energy = %.1f Btu/lb',loss)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.12: State_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 2 of keenan and keynes,')\n",
+"p1=98.87 //psia\n",
+"p2=31.78 //psia\n",
+"t1=80 //F\n",
+"h2=26.365 //btu/lb\n",
+"h1=11.554 //btu/lb\n",
+"hfg=67.203 //btu/lb\n",
+"//calculations\n",
+"x=(h2-h1)/hfg\n",
+"//results\n",
+"printf('The state of vapor leaving is %.2f psia with a quality of %.2f percent',p2,x*100)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.13: Mean_state_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"ps=216 //psig\n",
+"pb=29.12 //in of Hg\n",
+"p2=0.4 //in\n",
+"t2=244 //F\n",
+"//calculations\n",
+"pa=0.491*pb\n",
+"pabs=pa + p2*0.491\n",
+"plb=pa+ ps\n",
+"hcal=1166.5 //Btu/lb\n",
+"h2=1200.1 //Btu/lb\n",
+"h3=831.9 //Btu/lb\n",
+"y=-(hcal-h2)/h3\n",
+"//results\n",
+"printf('Mean state in the line is %.1f psia with a moisture content of %.2f percent',plb,y*100)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.1: Enthalpy_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"p=3000 //psia\n",
+"T=250 //F\n",
+"//calculations\n",
+"disp('From table 1, keenan and keynes,')\n",
+"vf=0.01700\n",
+"disp('From table 4,')\n",
+"dvf=-18.3*10^-5 \n",
+"v=vf+dvf\n",
+"disp('From table 1,')\n",
+"hf=218.48\n",
+"disp('From table 4,')\n",
+"dhf=6.13\n",
+"h=hf+dhf\n",
+"sf=0.3675\n",
+"dsf=-4.34*10^-3\n",
+"s=sf+dsf\n",
+"//results\n",
+"printf('Specific volume = %.5f cu ft/lb',v)\n",
+"printf('\n Enthalpy = %.2f Btu/lb',h)\n",
+"printf('\n Entropy = %.4f Btu/lb per deg R',s)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.2: Moisture_content_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"h=1100 //Btu/lb\n",
+"P=100 //psia\n",
+"//calculations\n",
+"disp('From table 2 of keenan and keynes,')\n",
+"hg=1187.2 //Btu/lb\n",
+"hfg=888.8 //Btu/lb\n",
+"y=-(h-hg)/hfg\n",
+"//results\n",
+"printf('The state is %d psia with a moisture content of %.2f percent',P,y*100)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.3: State_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 1 of keenan and keynes,')\n",
+"v1=0.2688\n",
+"//calculations\n",
+"v2=3.060\n",
+"p2=200 //psia\n",
+"t2=600 //F\n",
+"//results\n",
+"printf('State of steam is %d psia and %d F',p2,t2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.4: State_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 2 of keenan and keynes,')\n",
+"t1=439.60 //F\n",
+"u1=1118.4 //Btu/lb\n",
+"//calculations\n",
+"p2=380 //psia\n",
+"//results\n",
+"printf('The state of steam is saturated at %d psia and %.2f F',p2,t1)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.5: State_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 2 of keenan and keynes,')\n",
+"p1=1 //in of Hg\n",
+"s=1.9812 \n",
+"//calculations\n",
+"sf=2.0387\n",
+"sfg=1.9473\n",
+"y=-(s-sf)/sfg\n",
+"//results\n",
+"printf('The state is %d in of Hg with a moisture content of %.2f percent',p1,y*100)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.6: State_Enthalpy_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 1 of keenan and keynes,')\n",
+"h1=1204.8 //Btu/lb\n",
+"q=174 //Btu/lb\n",
+"//calculations\n",
+"h2=h1+q\n",
+"p2=30 //psia\n",
+"t2=720 //F\n",
+"//results\n",
+"printf('Final state of steam is %d psia and %d F',p2,t2)\n",
+"printf('\n Final enthalpy is %.1f Btu/lb',h2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.7: volume_state_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 1 of keenan and keynes,')\n",
+"p=70 //psia\n",
+"x=0.1\n",
+"p2=198 //psia\n",
+"//calculations\n",
+"v1=6.206\n",
+"v2=0.017\n",
+"vx=v1-x*(v1-v2)\n",
+"t2=1400 //F\n",
+"//results\n",
+"printf('Final specific volume = %.3f cu ft',vx)\n",
+"printf('\n Final state is %d psia and %d F',p2,t2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.8: State_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"disp('From table 1 of keenan and keynes,')\n",
+"p=400 //psia\n",
+"t1=700 //F\n",
+"p2=85 //psia\n",
+"//calculations\n",
+"s2=1.6398 //units/lb\n",
+"t2=350 //F\n",
+"//results\n",
+"printf('Final state of steam is %d psia and %d F',p2,t2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.9: Work_and_heat_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"p1=20 //psia\n",
+"p2=140 //psia\n",
+"J=778\n",
+"t2=150 //F\n",
+"t1=30 //F\n",
+"//calculations\n",
+"disp('From Table A-3,')\n",
+"v1=2.0884 //cu ft/lb\n",
+"v2=0.33350 //cu ft/lb\n",
+"h2=95.709\n",
+"h1=81.842\n",
+"n=log(p2/p1) /log(v1/v2)\n",
+"W=(p2*v2-p1*v1)*144/(1-n)\n",
+"du=h2-h1 + (p1*v1-p2*v2)*144/J\n",
+"Q=du+W/J\n",
+"s2=0.17718\n",
+"s1=0.18126\n",
+"Q2=((t2+t1)/2 +460) *(s2-s1)\n",
+"//results\n",
+"printf('Work of compression = %d ft-lb',W)\n",
+"printf('\n Heat removed per pound of refrigerant = %.3f Btu/lb',Q)\n",
+"printf('\n Heat removed in case 2 = %.4f Btu',Q2)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/11-Thermodynamics_of_Fluid_flow.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/11-Thermodynamics_of_Fluid_flow.ipynb
new file mode 100644
index 0000000..d149fb7
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/11-Thermodynamics_of_Fluid_flow.ipynb
@@ -0,0 +1,461 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 11: Thermodynamics of Fluid flow"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.10: Pressure_and_velocity_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"R=53.35\n",
+"v=300 //ft/s\n",
+"p=100 //psia\n",
+"t1=200 //F\n",
+"q=500 //Btu/s\n",
+"gc=32.2 //ft/s^2\n",
+"J=778\n",
+"//calculations\n",
+"rho1=p*144/(R*(460+t1))\n",
+"x=poly(0,'x')\n",
+"s=x^2 -0.206*x+0.00535\n",
+"vec=roots(s)\n",
+"rho2=vec(1)\n",
+"t2=(236.6 - 0.301/rho2^2)/0.248\n",
+"P2=rho2*R*(t2+462) /144\n",
+"v2=sqrt(2*gc*J*(236.6-0.248*t2))\n",
+"v22=rho1*v/rho2\n",
+"//results\n",
+"printf('Final temperature = %.1f F',t2)\n",
+"printf('\n Final pressure = %.1f psia',P2)\n",
+"printf('\n Exit velocity in case 1 = %.1f ft/s',v2)\n",
+"printf('\n Exit velocity in case 2 = %.1f ft/s',v22)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.1: Reynolds_Number.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"d=2.067 //in\n",
+"P=20 //psia\n",
+"R=53.35 \n",
+"T=600 //R\n",
+"mu=0.0486 //lb /ft.hr\n",
+"v=50 //ft/s\n",
+"//calculations\n",
+"rho=P*144/(R*T)\n",
+"Re=d*v*rho*3600/(12*mu)\n",
+"//results\n",
+"printf('Reynolds number = %d ',Re)\n",
+"disp('The answers are a bit different due to rounding off error in textbook')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.2: Pressure_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"eps=0.00015 \n",
+"D=2.067/12 //ft\n",
+"l=100 //ft\n",
+"P=20 //psia\n",
+"R=53.35 \n",
+"T=600 //R\n",
+"mu=0.0486 //lb /ft.hr\n",
+"v=50 //ft/s\n",
+"g=32.17 //ft/s^2\n",
+"//calculations\n",
+"rho=P*144/(R*T)\n",
+"Re=D*v*rho*3600/(mu)\n",
+"ed=eps/D\n",
+"disp('From figure 11.5')\n",
+"f=0.0235\n",
+"dp=f*l*rho*v^2 /(2*D*g) /144\n",
+"change=dp/P *100\n",
+"//results\n",
+"printf('Change in pressure = %.2f psi',dp)\n",
+"printf('\n Percentage change in pressure = %.2f percent',change)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.3: Final_pressure_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"v1=60 //ft/s\n",
+"d1=10 //in\n",
+"d2=15 //in\n",
+"P=15 //psia\n",
+"R=53.35\n",
+"T=540 //R\n",
+"g=32.17 //ft/s^2\n",
+"v1=60 //ft/s\n",
+"//calculations\n",
+"v2=v1*d1^2 /d2^2\n",
+"rho=P*144/(R*T)\n",
+"dp=rho*(v2^2 -v1^2)/(2*g) /144\n",
+"p2=P-dp\n",
+"//results\n",
+"printf('Final pressure = %.3f psia',p2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.4: Change_in_Entropy.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"J=778 //ft.lb/Btu\n",
+"D=2.067/12 //ft\n",
+"l=100 //ft\n",
+"P=20 //psia\n",
+"R=53.35 \n",
+"T=600 //R\n",
+"mu=0.0486 //lb /ft.hr\n",
+"v=50 //ft/s\n",
+"g=32.17 //ft/s^2\n",
+"//calculations\n",
+"f=0.0235\n",
+"ds=f*v^2 *l /(J*2*D*g*T)\n",
+"//results\n",
+"printf('Change in entropy = %.6f Btu/lbm R',ds)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.5: Enthalpy_and_entropy_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"v=210 //ft/s\n",
+"g=32.17 //ft/s^2\n",
+"p=200 //psia\n",
+"z=5 //ft\n",
+"x=2.361\n",
+"h=1210.3\n",
+"J=778\n",
+"//calculations\n",
+"P0=p + v^2 /(2*g*144*x) + z/(144*x)\n",
+"h0=h + v^2 /(2*J*g) +z/J\n",
+"S=1.5594 //units/lb\n",
+"S0=S\n",
+"t0=401.9 //F\n",
+"v0=2.342 //cu ft/lb\n",
+"rho0=1/v0\n",
+"//results\n",
+"printf('Pressure = %d psia',P0)\n",
+"printf('\n Enthalpy = %.2f Btu/lb',h0)\n",
+"printf('\n Entropy = %.4f units/lb',S0)\n",
+"printf('\n Temperature = %.1f F',t0)\n",
+"printf('\n Density = %.3f lb/cu ft',rho0)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.6: Temperature_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"p1=40 //psia\n",
+"t1=80 //F\n",
+"p2=30 //psia\n",
+"ar=0.5 //sq ft\n",
+"v1=200 //ft/s\n",
+"R=53.35\n",
+"cp=0.24\n",
+"g=32.17\n",
+"J=778\n",
+"//calculations\n",
+"rho1=144*p1/(R*(t1+460))\n",
+"G=rho1*v1\n",
+"h10= cp*t1 + p1^2 /(2*g*rho1^2 *J)\n",
+"t2=78 //F\n",
+"h2=cp*t2\n",
+"g2=h10-h2\n",
+"rho2=sqrt(p1^2 /(2*g*g2*J))\n",
+"P2=rho2*R*(t2+460)/144 \n",
+"ds2=cp*log((t2+460)/(t1+460)) - R/J *log(P2/p1)\n",
+"t3=77 //F\n",
+"h3=cp*t3\n",
+"g3=h10-h3\n",
+"rho3=sqrt(p1^2 /(2*g*g3*J))\n",
+"P3=rho3*R*(t3+460)/144 \n",
+"ds3=cp*log((t3+460)/(t1+460)) - R/J *log(P3/p1)\n",
+"t4=79 //F\n",
+"h4=cp*t4\n",
+"g4=h10-h4\n",
+"rho4=sqrt(p1^2 /(2*g*g4*J))\n",
+"P4=rho4*R*(t4+460)/144 \n",
+"ds4=cp*log((t4+460)/(t1+460)) - R/J *log(P4/p1)\n",
+"h5=18.62\n",
+"t5=h5/cp\n",
+"Gv=[h4 h2 h3]\n",
+"Pv=[P4 P2 P3]\n",
+"Sv=[ds4 ds2 ds3]\n",
+"scf(1)\n",
+"xtitle('Fanno line diagram , Enthalpy vs Entropy','Entropy','Enthalpy Btu/lb')\n",
+"plot(Sv,Gv)\n",
+"scf(2)\n",
+"xtitle('Fanno line diagram , Pressure vs Entropy','Entropy','Pressure psia')\n",
+"plot(Sv,Pv)\n",
+"//results\n",
+"printf('Temperature at exit = %.1f F',t5)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.7: Velocity_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"p1=40 //psia\n",
+"t1=80 //F\n",
+"p2=30 //psia\n",
+"ar=0.5 //sq ft\n",
+"v1=200 //ft/s\n",
+"R=53.35\n",
+"cp=0.24\n",
+"g=32.17\n",
+"J=778\n",
+"t2=78 //F\n",
+"//calculations\n",
+"G=40 //lb/sq ft/sec\n",
+"rho2=144*p2/(R*(t2+460))\n",
+"v2=p1/rho2\n",
+"//results\n",
+"printf('Velocity = %d ft/s',v2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.8: velocity_and_density_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"P2=[180 160 140 120 100 80 60 40 20]\n",
+"k=1.4\n",
+"p1=200 //psia\n",
+"t1=240+460 //R\n",
+"cp=0.24\n",
+"J=778\n",
+"gc=32.2\n",
+"R=53.35\n",
+"m=4 //lb/sec\n",
+"//calculations\n",
+"pr=p1./ P2\n",
+"prr=pr^((k-1)/k)\n",
+"T2=t1 ./prr\n",
+"dt=t1 -T2\n",
+"dh=dt*cp\n",
+"v2=sqrt(2*gc*J*dh)\n",
+"vol=(R*T2) ./(P2*144)\n",
+"A2=m*vol*144 ./v2\n",
+"dia=sqrt(4/ %pi *A2)\n",
+"rad=dia/2\n",
+"den=1 ./vol\n",
+"scf(1)\n",
+"xtitle ('Velocity vs pressure','Pressure in psia','velocity in ft/s')\n",
+"plot(P2,v2)\n",
+"scf(2)\n",
+"xtitle('specific volume vs pressure','Pressure in psia','specific volume in cu ft/lb')\n",
+"plot(P2,vol)\n",
+"scf(3)\n",
+"xtitle('Radius vs Pressure' ,'Pressure in psia','Radius in in')\n",
+"plot(P2,rad)\n",
+"//results\n",
+"disp('Velocity in ft/s')\n",
+"disp(v2)\n",
+"disp('Specific volume in cu ft/lb')\n",
+"disp(vol)\n",
+"disp('Density in lb/cu ft')\n",
+"disp(den)\n",
+"disp('Diameter of nozzle in in')\n",
+"disp(dia)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 11.9: Exit_area_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"p1=200 //psia\n",
+"t1=480 //F\n",
+"eff=0.95\n",
+"g=32.2 //ft/s^2\n",
+"J=778\n",
+"mf=3.4 //lb/s\n",
+"//calculations\n",
+"disp('From steam tables,')\n",
+"h1=1257.8 \n",
+"h2=1210.5 \n",
+"dh=eff*(h1-h2)\n",
+"ve=sqrt(2*g*J*dh)\n",
+"h3=h1-dh\n",
+"vs=3.961\n",
+"Ae=mf*vs/ve *144\n",
+"//results\n",
+"printf('Nozzle exit area = %.3f sq.in',Ae)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/12-Heat_Transfer.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/12-Heat_Transfer.ipynb
new file mode 100644
index 0000000..412a303
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/12-Heat_Transfer.ipynb
@@ -0,0 +1,477 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 12: Heat Transfer"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.10: Heat_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"Do=2.375 //in\n",
+"hi=1200\n",
+"Di=2.067 //in\n",
+"km=29.2\n",
+"h0=1500\n",
+"L=2.375 //in\n",
+"t1=220 //F\n",
+"t4=140 //F\n",
+"//calculations\n",
+"U0= 1/(Do/(Di*hi) + (Do/12 *log(Do/Di) /(2*km)) + 1/h0)\n",
+"Q=U0*L*%pi*(t1-t4)/12\n",
+"//results\n",
+"printf('Heat transferred per foot length of pipe = %d btu/hr',Q)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.11: Temperature_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"Do=2.375 //in\n",
+"hi=1200\n",
+"Di=2.067 //in\n",
+"km=29.2\n",
+"h0=1500\n",
+"L=2.375 //in\n",
+"t1=220 //F\n",
+"t4=140 //F\n",
+"//calculations\n",
+"Re=Do/(Di*hi)\n",
+"R0=Do/(Di*hi) + (Do/12 *log(Do/Di) /(2*km)) + 1/h0\n",
+"td=Re/R0 *(t1-t4)\n",
+"ti=t4+td\n",
+"Req=1/h0\n",
+"td2=Req/R0 *(t1-t4)\n",
+"to=t1-td2\n",
+"//results\n",
+"printf('The temperature of the inner surface of pipe = %.1f F',ti)\n",
+"printf('\n The temperature of the outer surface of pipe = %.1f F',to)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.12: LMTD_Calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"th1=800 //F\n",
+"th2=300 //F\n",
+"tc1=100 //F\n",
+"tc2=400 //F\n",
+"//calculations\n",
+"lmtd= ((th1-tc2) - (th2-tc1) )/(log((th1-tc2)/(th2-tc1)))\n",
+"//results\n",
+"printf('Logarithmic Mean temperature difference = %d F',lmtd)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.13: True_MTD_Calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"th1=200 //F\n",
+"th2=100 //F\n",
+"tc1=80 //F\n",
+"tc2=110 //F\n",
+"//calculations\n",
+"disp('From the lmtd graph,')\n",
+"R=(tc1-tc2)/(th2-th1)\n",
+"P=(th2-th1)/(tc1-th1)\n",
+"F=0.62\n",
+"lmtd= F* ((th1-tc2) - (th2-tc1) )/(log((th1-tc2)/(th2-tc1)))\n",
+"//results\n",
+"printf('True Mean temperature difference = %.1f F',lmtd)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.1: Temperature_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"km1=0.62\n",
+"km2=0.16\n",
+"km3=0.4\n",
+"l1=8 //in\n",
+"l2=4 //in\n",
+"l3=4 //in\n",
+"Tf=1600 //F\n",
+"Tc=100 //F\n",
+"//calculations\n",
+"Rw=l1/12/km1 +l2/12/km2 +l3/12/km3\n",
+"Rb=l1/12/km1\n",
+"Ti=Tf-Rb/Rw *(Tf-Tc)\n",
+"//results\n",
+"printf('Interface temperature = %.1f F',Ti)\n",
+"disp('The answers might differ a bit from textbook due to rounding off error.')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.2: Heat_flow_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"th=350 //F\n",
+"tc=150 //F\n",
+"od1=4.5\n",
+"id1=4.026\n",
+"od2=6.5\n",
+"id2=4.5\n",
+"k1=32\n",
+"k2=0.042\n",
+"//calculations\n",
+"Q=2*%pi*(th-tc)/(log(od1/id1) /k1 + log(od2/id2) /k2)\n",
+"r1=log(od1/id1) /k1\n",
+"rt=log(od1/id1) /k1 + log(od2/id2) /k2\n",
+"ti=th-r1/rt*(th-tc)\n",
+"//results\n",
+"printf('Heat flow = %.1f Btu/hr',Q)\n",
+"printf('\n Interface temperature = %.2f F',ti)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.3: Energy_exchange_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"Fa=0.045\n",
+"l=4 //m\n",
+"b=4 //m\n",
+"Fe=1\n",
+"Ta=540+460 //R\n",
+"Tb=1540+460 //R\n",
+"//calculations\n",
+"A=l*b\n",
+"Q=0.173*A*Fa*Fe*((Tb/100)^4 -(Ta/100)^4)\n",
+"Q2=416000\n",
+"//results\n",
+"printf('In case 1, Net energy exchange = %d Btu/hr',Q)\n",
+"printf('\n In case 2, Net energy exchange = %d Btu/hr',Q2)\n",
+"disp('The answers are a bit different due to rounding off error in textbook')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.4: Energy_Exchange_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"ea=0.8\n",
+"eb=0.7\n",
+"Fa=0.045\n",
+"l=4 //m\n",
+"b=4 //m\n",
+"Fe=1\n",
+"Ta=540+460 //R\n",
+"Tb=1540+460 //R\n",
+"//calculations\n",
+"A=l*b\n",
+"ef=ea*eb\n",
+"Q=0.173*A*Fa*Fe*ef*((Tb/100)^4 -(Ta/100)^4)\n",
+"//results\n",
+"printf('Net energy exchange = %d Btu/hr',Q)\n",
+"disp('The answers are a bit different due to rounding off error in textbook')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.5: Inside_film_coefficient_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"den=61.995 //lb/cu ft\n",
+"vel=6 //ft/s\n",
+"t1=100 //F\n",
+"t2=160 //F\n",
+"de=2.067 //in\n",
+"mu=1.238\n",
+"pr=3.3\n",
+"//calculations\n",
+"G=den*vel*3600\n",
+"tm=(t1+t2)/2\n",
+"hc=0.023*0.377/(de/12) *(de/12 *G/mu)^0.8 *(pr)^0.4\n",
+"//results\n",
+"printf('Inside film coefficient = %d Btu/sq ft hr F',hc)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.6: Inside_film_coefficient_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"d=0.5 //in\n",
+"tm=1000 //F\n",
+"v=5//ft/s\n",
+"k=38.2\n",
+"den=51.2\n",
+"mu=0.3\n",
+"//calculations\n",
+"Nu=7+ 0.025*(d/12 *v*den*mu/k*3600)^0.8\n",
+"h=Nu*k/(d/12)\n",
+"//results\n",
+"printf('Inside film coefficient = %d Btu/sq ft hr F',h)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.7: convective_film_coefficient_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variablesdo=2 //in\n",
+"tf=120 //F\n",
+"ti=80 //F\n",
+"rho=0.0709\n",
+"g=32.17\n",
+"bet=1/560\n",
+"cp=0.24\n",
+"mu=0.0461\n",
+"k=0.0157\n",
+"d=2 //in\n",
+"Cd=0.45\n",
+"//calculations\n",
+"GrPr=(d/12)^3 *rho^2 *g*3600^2 *bet*(tf-ti)*cp/(mu*k)\n",
+"hc=Cd*k/(d/12)^(1/4) *GrPr^(1/4)\n",
+"//results\n",
+"printf('Convective film coefficient = %.3f Btu/sq ft hr F',hc)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.8: Outer_film_coefficient_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"tf=220 //F\n",
+"ti=200 //F\n",
+"d=2 //in\n",
+"C=103.7\n",
+"k=0.394\n",
+"rho=59.37\n",
+"hfg=965.2\n",
+"mu=0.70\n",
+"//calculations\n",
+"h=C*(k^3 *rho^2 *hfg/((d/12) *mu*(tf-ti)))^(1/4)\n",
+"//results\n",
+"printf('Outer film coefficient = %d Btu/sq ft hr F',h)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 12.9: Boiling_film_coefficient_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"tf=225 //F\n",
+"a=190\n",
+"b=0.043\n",
+"ti=212 //F\n",
+"//calculations\n",
+"hc=a/(1-b*(tf-ti))\n",
+"hcti=hc*1.25\n",
+"//results\n",
+"printf('For a flat copper plate, boiling film coefficient = %.1f Btu/sq ft hr F',hc)\n",
+"printf('\n For an inclined copper plate, boiling film coefficient = %d Btu/sq ft hr F',hcti)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/13-Non_reactive_and_reactive_gaseous_mixtures.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/13-Non_reactive_and_reactive_gaseous_mixtures.ipynb
new file mode 100644
index 0000000..54eb380
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/13-Non_reactive_and_reactive_gaseous_mixtures.ipynb
@@ -0,0 +1,518 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 13: Non reactive and reactive gaseous mixtures"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.10: volumetric_analysis.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"A=[1 1; 0.5 1]\n",
+"B=[1; 0.9]\n",
+"x=0.9\n",
+"//calculations\n",
+"N2=x*79/21\n",
+"C=A\B\n",
+"vec= [ C(1) C(2) N2]\n",
+"su=sum(vec)\n",
+"vec2=vec/su *100\n",
+"//results\n",
+"printf('Volumetric analysis')\n",
+"disp('CO CO2 N2')\n",
+"disp(vec2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.11: Moles_of_dry_products_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"c=0.74\n",
+"ref=0.02\n",
+"co2=0.12\n",
+"co=0.1/100\n",
+"M=12\n",
+"//calcualtions\n",
+"carbon=c-ref\n",
+"car2=co2+co\n",
+"wt=car2*M\n",
+"amount=carbon/wt\n",
+"//results\n",
+"printf('Moles of dry products per pound of coal = %.3f mole',amount)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.12: Moles_of_dry_products_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"x1=0.128\n",
+"x2=0.035\n",
+"x3=0.002\n",
+"M=12\n",
+"N=26\n",
+"//calculations\n",
+"c=x1+x3\n",
+"mole=12/c\n",
+"wt=M*M+N\n",
+"num=mole/wt\n",
+"//results\n",
+"printf('Number of moles of dry products per pound of fuel = %.3f mole',num)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.13: Weight_of_dry_air_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"c=0.74\n",
+"ref=0.02\n",
+"co2=0.12\n",
+"co=0.1/100\n",
+"o2=0.065\n",
+"M=12\n",
+"x=0.79\n",
+"M=28.97\n",
+"//calcualtions\n",
+"n2=1-(co2+co+o2)\n",
+"mol=n2/x\n",
+"wt=mol*M\n",
+"wt2=0.496\n",
+"pou=wt2*wt\n",
+"ta=10.27\n",
+"EA=(pou-ta)/ta *100\n",
+"//results\n",
+"printf('Weight of air per pound of fuel = %.2f lb',pou)\n",
+"printf('\n Excess air percentage = %.1f percent',EA)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.1: Mass_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"P=70 //psia\n",
+"Pt=110 //psia\n",
+"V=20 //cu ft\n",
+"R0=1545 //Universal gas constant\n",
+"T=540 //R\n",
+"M=32 //Molecular weight of Oxygen\n",
+"M2=28 //Molecular weight of Nitrgoen\n",
+"//calculations\n",
+"N=P*V*144/(R0*T)\n",
+"mo=M*N\n",
+"Pn=Pt-P\n",
+"N2=Pn*V*144/(R0*T)\n",
+"mn=N2*M2\n",
+"Vo=N*R0*T/(144*Pt)\n",
+"Vn=N2*R0*T/(144*Pt)\n",
+"Vn2=V-Vo\n",
+"//results\n",
+"printf('Mass of oxygen = %.2f lb',mo)\n",
+"printf('\n Mass of nitrogen = %.2f lb',mn)\n",
+"printf('\n Partial volume of oxygen = %.2f cu ft',Vo)\n",
+"printf('\n Partial volume of nitrogen = %.2f cu ft',Vn)\n",
+"printf('\n In case 2, Partial volume of nitrogen = %.2f cu ft',Vn2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.2: Change_in_Entropy_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"P=50 //psia\n",
+"V=4 //cu ft\n",
+"dv=3 //cu ft\n",
+"J=778\n",
+"T=560 //R\n",
+"//calculation\n",
+"ds= 144*P*V*log((V+dv)/V) /(J*T)\n",
+"//results\n",
+"printf('Change in entropy = %.3f unit',ds)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.3: Change_in_Entropy_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"p1=50 //psia\n",
+"t1=100+460 //R\n",
+"R1=48.3\n",
+"R2=55.2\n",
+"v1=4 //cu ft\n",
+"p2=100 //psia\n",
+"v2=3 //cu ft\n",
+"t2=200+460 //R\n",
+"cv1=0.157\n",
+"cv2=0.177\n",
+"cpm=0.219\n",
+"J=778\n",
+"//calculations\n",
+"m1=144*p1*v1/(R1*t1)\n",
+"m2=144*p2*v2/(R2*t2)\n",
+"tf=(m1*cv1*(t1-460) + m2*cv2*(t2-460))/(m1*cv1+m2*cv2)\n",
+"Po2=v1/(v1+v2) *(tf+460)/t1 *p1\n",
+"ds=cpm*log((tf+460)/t1) - R1/J *log(Po2/p1)\n",
+"dss=ds*m1\n",
+"//results\n",
+"printf('Change in entropy = %.4f unit',dss)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.4: Change_in_Entropy_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"p1=30 //psia\n",
+"t1=80+460 //R\n",
+"R1=48.3\n",
+"R2=55.2\n",
+"m1=20 //lb/min\n",
+"p2=50 //psia\n",
+"m2=35 //lb/min\n",
+"t2=160+460 //R\n",
+"cp1=0.219\n",
+"cp2=0.248\n",
+"J=778\n",
+"//calculations\n",
+"tf=(m1*cp1*(t1-460) + m2*cp2*(t2-460))/(m1*cp1+m2*cp2)\n",
+"Po2=m1/32/(m1/32+m2/28) *p1\n",
+"ds=cp1*log((tf+460)/t1) - R1/J *log(Po2/p1)\n",
+"dss=ds*m1\n",
+"//results\n",
+"printf('Change in entropy = %.4f units/min',dss)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.5: Weight_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"x=[0.15 0.08 0.77]\n",
+"M=[44 32 28]\n",
+"//calculations\n",
+"y=x ./M\n",
+"yt=sum(y)\n",
+"mt=y/yt\n",
+"per=mt*100\n",
+"wt=1/yt\n",
+"R=1545/wt\n",
+"//results\n",
+"printf('Volumetric analysis')\n",
+"disp('percent by volume')\n",
+"format('v',6);per\n",
+"disp(per)\n",
+"printf('Weight per mole = %.1f lb',wt)\n",
+"printf('\n Gas constant = %.1f ',R)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.6: Dry_analysis_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"x1=0.885 //mole fraction of Ch4\n",
+"x2=0.115 //mole fraction of c2h6\n",
+"x3=0.4/100 //mole fraction of N2\n",
+"n1=2 //Moles of Ch4\n",
+"n2=3.5 //Moles of c2h6\n",
+"n3=1 //moles of ch4 in case 2\n",
+"n4=2 //moles of c2h6 in case 2\n",
+"//calculations\n",
+"y1=n1*x1\n",
+"y2=n2*x2\n",
+"y=y1+y2\n",
+"vec2=[y1 y2]\n",
+"air=y/0.21\n",
+"y3=n3*x1\n",
+"y4=n4*x2\n",
+"yy=y3+y4\n",
+"vec3=[y3 y4]\n",
+"air2=y/0.21 *0.79\n",
+"//results\n",
+"printf('Theoretical air = %.2f moles of air per mole of fuel',air)\n",
+"disp('Oxygen analysis')\n",
+"disp(vec2)\n",
+"printf('\n Amount of nitrogen = %.2f moles of nitrogen per mole of fuel',air2)\n",
+"disp('Dry analysis')\n",
+"disp(vec3)\n",
+"printf('total = %.3f moles',yy)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.7: Air_fuel_ratio_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"x=[0.74 0.06 0.01] //mole fraction of C, H and S respectively\n",
+"y=[8/3 8 1] //Pounds O2 per pound substance of C,H and S respectively\n",
+"oxy=0.08 //Oxygen in coal\n",
+"z=0.232 //mass of coal\n",
+"//calculations\n",
+"pou=x.*y\n",
+"tot=sum(pou)\n",
+"oxy2=tot-oxy\n",
+"air=oxy2/z\n",
+"//results\n",
+"printf('Theoretical air fuel ratio = %.2f lb of air per pound of coal',air)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.8: Air_fuel_ratio_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"o2=12.5 //moles of O2\n",
+"h20=9 //moles of H2O\n",
+"x=0.21 //Mole fraction of Oxygen in air\n",
+"M=28.97 //Molar mass of air\n",
+"M2=56 //molar mass of C4H8\n",
+"M1=8*12+18 //molecular mass of c8h18\n",
+"//calculations\n",
+"air=o2/x\n",
+"pound=air*M\n",
+"AR=pound/M1\n",
+"y1=h20/M2 *100\n",
+"y2=o2*(79/21) /M2 *100\n",
+"//results\n",
+"printf('Air fuel ratio = %.2f lb of air per pound of fuel',AR)\n",
+"printf('\n Molal or volumetric analysis is %.2f percent of CO2 and %.2f percent N2',y1,y2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 13.9: volumetric_analysis.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"x=18.5 //Moles of O2\n",
+"c=12 //Moles of CO2\n",
+"vap=13 //moles of H2O\n",
+"P=15 //psia\n",
+"R=1545 //Universal gas constant\n",
+"//calculations\n",
+"excess=x*0.5\n",
+"M=12*12+2*vap\n",
+"n2=(x+excess)*79/21\n",
+"nt=n2+excess+c\n",
+"dry=[c x/2 n2]/nt *100\n",
+"wet=nt+vap\n",
+"fue=100/(M)\n",
+"mol=wet*fue\n",
+"vol=mol*R*1460/(144*P)\n",
+"//results\n",
+"disp('Volumetric analysis in percentage')\n",
+"disp(' CO2 O2 N2')\n",
+"disp(dry)\n",
+"printf('Volume of wet products = %d cfm',vol)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/14-Energies_associated_with_chemical_reactions.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/14-Energies_associated_with_chemical_reactions.ipynb
new file mode 100644
index 0000000..006509e
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/14-Energies_associated_with_chemical_reactions.ipynb
@@ -0,0 +1,329 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 14: Energies associated with chemical reactions"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 14.1: Heating_value_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"lhs=8.5 //moles of reactants\n",
+"rhs=6 //moles of CO2\n",
+"n=3 //moles of H2O\n",
+"R=1545 //Universal gas constant\n",
+"R2=18.016 //molar mass of water\n",
+"J=778 //Work conversion constant\n",
+"T=537 //R\n",
+"T2=1050.4 //R\n",
+"T3=991.3 //R\n",
+"Qhp=1417041 //Btu/mol\n",
+"//calculations\n",
+"Qhpv=(lhs-rhs)*R*T/J\n",
+"Qhv=Qhp-Qhpv\n",
+"hfg=(rhs-n)*R2*T2\n",
+"Qlp=Qhp-hfg\n",
+"Qlpv=(lhs-rhs-n)*R/J *T\n",
+"Qlv=Qlp-Qlpv\n",
+"Qhlv=(rhs-n)*R2*T3\n",
+"Qlv3=Qhv-Qhlv\n",
+"//results\n",
+"printf('Higher heating value at constant volume = %d Btu/mol',Qhv)\n",
+"printf('\n Lower heating value at constant pressure = %d Btu/mol',Qlp)\n",
+"printf('\n In case 1,Lower heating value at constant volume = %d Btu/mol',Qlv)\n",
+"printf('\n In case 2,Lower heating value at constant volume = %d Btu/mol',Qlv3)\n",
+"disp('The answers might differ a bit from textbook due to rounding off error.')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 14.2: Heating_value_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"disp('From table 5-4,')\n",
+"no=7.5\n",
+"n1=3\n",
+"n2=6\n",
+"Q=1360805 //Btu/mol\n",
+"//calculations\n",
+"Uo=337+no*85\n",
+"Uf=n1*104+n2*118\n",
+"del= Q-(Uo-Uf)\n",
+"Uo2=1656+no*402\n",
+"Uf2=n1*490+n2*570\n",
+"Qv=Uo2-Uf2+del\n",
+"//results\n",
+"printf('Change in chemical energy during complete combustion = %d Btu/mol',del)\n",
+"printf('\n Lower heating value at constant volume = %d Btu/mol',Qv)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 14.3: Heat_removed_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"disp('From table 5-4,')\n",
+"a=1 //moles of C6H6\n",
+"b=7.5 //moles of O2 in reactant\n",
+"c=1.875 //moles of excess O2\n",
+"d=35.27 //moles of N2\n",
+"e=3 //moles of H2O\n",
+"flow=40 //lb/min\n",
+"w=1360850 //Btu/mol\n",
+"//calculations\n",
+"U11=a*337\n",
+"U12=(b+c)*85\n",
+"U13=d*82\n",
+"U14=(a+b+c+d)*1066\n",
+"Ua1=U11+U12+U13+U14\n",
+"U21=c*2539\n",
+"U22=d*2416\n",
+"U23=e*3009\n",
+"U24=2*e*3852\n",
+"U25=(c+d+e+2*e)*1985\n",
+"Ua2=U21+U22+U23+U24+U25\n",
+"Q=Ua1+w-Ua2\n",
+"fuel=flow/(6*12+2*e)\n",
+"Q2=Q*fuel\n",
+"//results\n",
+"printf('Heat removed = %d Btu/min',Q2)\n",
+"disp('The answers might differ a bit from textbook due to rounding off error.')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 14.4: Furnace_efficiency_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"rate=10700 //lb/min\n",
+"t2=97.90 \n",
+"t1=33.05 \n",
+"r1=46 //lb/min\n",
+"//calculations\n",
+"disp('From steam tables,')\n",
+"Hv=1417041\n",
+"Qw=rate*(t2-t1)\n",
+"Q=r1/(12*6+6) *Hv\n",
+"eff=Qw/Q*100\n",
+"//results\n",
+"printf('Furnace efficiency = %.1f percent',eff)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 14.5: Thermal_efficiency_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"rate=94 //lb/hr\n",
+"hp=197 //hp\n",
+"c=8\n",
+"h=18\n",
+"Lv=17730 //Btu/hr\n",
+"H=2368089 //Btu/hr\n",
+"//calculations\n",
+"amount=rate*c/12 +h\n",
+"amount=0.824\n",
+"Lvv=H-Lv\n",
+"eff=hp*2544/(amount*Lvv) *100\n",
+"//results\n",
+"printf('Thermal efficiency = %.2f percent',eff)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 14.6: Thermal_efficiency_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"rate=94 //lb/hr\n",
+"hp=197 //hp\n",
+"c=8\n",
+"h=18\n",
+"mole=9\n",
+"H=2350359 //Btu/hr\n",
+"//calculations\n",
+"amount=rate*c/12 +h\n",
+"amount=0.824\n",
+"Lvv=H-mole*18.016*1050.4\n",
+"eff=hp*2544/(amount*Lvv) *100\n",
+"//results\n",
+"printf('Thermal efficiency = %.2f percent',eff)\n",
+"disp('The answer in the textbook is a different due to rounding off error')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 14.7: Total_available_energy_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"hv=14000 //Btu/lb\n",
+"ef=0.4\n",
+"tmin=80 //F\n",
+"tmid=300 //F\n",
+"m=13 //lb\n",
+"c=0.27\n",
+"tmean=2300 //F\n",
+"//calculations\n",
+"heat=ef*hv\n",
+"Qavail=heat*(tmean-tmin)/(tmean+460)\n",
+"Q=m*c*(tmean-tmid)\n",
+"Q2=Q- (tmin+460)*m*c*log((tmean+460)/(tmid+460))\n",
+"tot=Qavail+Q2\n",
+"//results\n",
+"printf('Total available energy = %d Btu/lb of fuel',tot)\n",
+"disp('The answer is a bit different due to rounding off error in textbook')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 14.8: Max_amount_of_work_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"disp('From table 14-2,')\n",
+"G1=55750 //Btu/mol\n",
+"co2=-169580 //Btu/mol\n",
+"h2o=-98290 //Btu/mol\n",
+"//calculations\n",
+"G2=6*co2+3*h2o\n",
+"avail=G1-G2\n",
+"//results\n",
+"printf('Max. amount of work = %d Btu/mol',avail)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/15-Thermodynamics_of_chemical_reactions.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/15-Thermodynamics_of_chemical_reactions.ipynb
new file mode 100644
index 0000000..c741824
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/15-Thermodynamics_of_chemical_reactions.ipynb
@@ -0,0 +1,137 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 15: Thermodynamics of chemical reactions"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 15.1: Dissociation_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"kp=10^(1.45)\n",
+"//calculations\n",
+"x=poly(0,'x')\n",
+"s=(1-x)^2 *(2+x) -kp^2 *x^(3)\n",
+"vec=roots(s)\n",
+"X=vec(3)\n",
+"xper=X*100\n",
+"//results\n",
+"printf('Amount of dissociaton = %.1f percent',xper)\n",
+"printf('\n Of each original mole of CO2, there will be %.3f mole of CO , %.3f mol of Oxygen and %.3f mol of CO2',X,X/2,(1-X))"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 15.2: Max_temperature_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"U=121200 //Btu/mol\n",
+"Uco2=51635 //Btu/mol\n",
+"Un2=27589 //Btu/mol\n",
+"Uco22=57875 //Btu/mol\n",
+"Un22=21036 //Btu/mol\n",
+"T1=5000 //R\n",
+"T2=5500 //R\n",
+"//calculations\n",
+"Ut1=Uco2+1.88*Un2\n",
+"Ut2=Uco22 + 1.88*Un22\n",
+"disp('By extrapolation,')\n",
+"Tx=5710 //R\n",
+"//results\n",
+"printf('Max. Temperature reached = %d R',Tx)\n",
+"disp('The calculation for Ut2 is wrong in textbook. Please use a calculator.')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 15.3: Max_temperature_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"disp('By trial and error,')\n",
+"X=0.201\n",
+"X1=0.2\n",
+"R=59.3 //universal gas constant\n",
+"T=5000 //R\n",
+"U=121200 //Btu/mol\n",
+"Uco2=51635 //Btu/mol\n",
+"Un2=27907 //Btu/mol\n",
+"U3=29616 //Btu/mol\n",
+"U4=27589 //Btu/mol\n",
+"//calculations\n",
+"kp1=R*(1-X1)/X1^1.5 /T^0.5\n",
+"kp2=R*(1-X)/X^1.5 /T^0.5\n",
+"q=(1-X)*Uco2 + X*Un2+ X/2 *U3 +1.88*U4 + X*U\n",
+"disp('Interpolating between T=4500 R and T=5000 R, we get')\n",
+"T2=4907 //R\n",
+"//results\n",
+"printf('Max. obtainable temperature = %d R',T2)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/16-Gas_cycles.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/16-Gas_cycles.ipynb
new file mode 100644
index 0000000..bb7a4c4
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/16-Gas_cycles.ipynb
@@ -0,0 +1,211 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 16: Gas cycles"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 16.1: Temperature_and_pressure_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"cr=9\n",
+"p1=14 //psia\n",
+"t1=80+460 //R\n",
+"n=1.4\n",
+"heat=800 //Btu\n",
+"c=0.1715\n",
+"R=53.35\n",
+"J=778\n",
+"//calculations\n",
+"p2=p1*(cr)^n\n",
+"t2=t1*cr^(n-1)\n",
+"t3=heat/c +t2\n",
+"p3=p2*t3/t2\n",
+"eff=(1-1/cr^(n-1))*100\n",
+"t4=t3/cr^(n-1)\n",
+"Qr=c*(t4-t1)\n",
+"cyclework=heat-Qr\n",
+"eff2= cyclework/heat *100\n",
+"V1=R*t1/(144*p1)\n",
+"pd=(1-1/cr)*V1\n",
+"mep=cyclework*J/(pd*144)\n",
+"//results\n",
+"printf('Max. temperature = %d R',t3)\n",
+"printf('\n Max. pressure = %d psia',p3)\n",
+"printf('\n In method 1,Thermal efficiency = %.1f percent',eff)\n",
+"printf('\n In method 2,Thermal efficiency = %.1f percent',eff2)\n",
+"printf('\n Mean effective pressure mep = %.1f psia',mep)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 16.2: Temperature_and_pressure_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"t1=80+460 //R\n",
+"p1=14 //psia\n",
+"n=1.4\n",
+"cr=16\n",
+"heat=800 //Btu\n",
+"cp=0.24\n",
+"c=0.1715\n",
+"//calculations\n",
+"t2=t1*cr^(n-1)\n",
+"p2=p1*(cr)^n\n",
+"t3=t2 +heat/cp\n",
+"v32=t3/t2\n",
+"v43=cr/v32\n",
+"t4=t3/v43^(n-1)\n",
+"Qr=c*(t4-t1)\n",
+"etat=(heat-Qr)/heat *100\n",
+"//results\n",
+"printf('Max. Temperature = %d R',t3)\n",
+"printf('\n Max. Pressure = %d psia',p2)\n",
+"printf('\n Thermal efficiency = %.1f percent',etat)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 16.3: mep_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"eff=0.585\n",
+"heat=800 //Btu\n",
+"t1=80+460 //R\n",
+"p1=14 //psia\n",
+"n=1.4\n",
+"R=53.35\n",
+"cr=9\n",
+"cp=0.24\n",
+"J=778\n",
+"//calculations\n",
+"W=eff*heat\n",
+"v1=R*t1/(144*p1)\n",
+"v2=v1/cr\n",
+"t2=1301 //R\n",
+"t3=t2+ heat/cp\n",
+"v3=v2*t3/t2\n",
+"v4=cr*v3\n",
+"mep=W*J/(144*(v4-v2))\n",
+"//results\n",
+"printf('Mean effective pressure = %.1f psia',mep)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 16.4: mep_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"eff=0.585\n",
+"heat=500 //Btu\n",
+"heat1=300 //Btu\n",
+"t1=80+460 //R\n",
+"p1=14 //psia\n",
+"n=1.4\n",
+"R=53.35\n",
+"cr=9\n",
+"J=778\n",
+"c=0.1715\n",
+"cp=0.24\n",
+"t2=1301 //R\n",
+"p2=308 //psia\n",
+"//calculations\n",
+"t3=t2+ heat/c\n",
+"p3=p2*t3/t2\n",
+"t4=t3+ heat1/cp\n",
+"v43=t4/t3\n",
+"v54=cr/v43\n",
+"t5=t4/(v54)^(n-1)\n",
+"Qr=c*(t5-t1)\n",
+"etat=(heat+heat1-Qr)/(heat+heat1) *100\n",
+"mep=(heat+heat1-Qr)*J/(12.69*144)\n",
+"//results\n",
+"printf('Max. Temperature = %d R',t4)\n",
+"printf('\n Max. Pressure = %d psia',p3)\n",
+"printf('\n Thermal efficiency = %.1f percent',etat)\n",
+"printf('\n Mean effective pressure = %.1f psia',mep)\n",
+"disp('The calculations are a bit different due to rounding off error in textbook')"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/17-Internal_combustion_engines.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/17-Internal_combustion_engines.ipynb
new file mode 100644
index 0000000..a2e733e
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/17-Internal_combustion_engines.ipynb
@@ -0,0 +1,114 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 17: Internal combustion engines"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 17.1: Indicated_efficiency_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"hp1=2000 //bhp\n",
+"m=792 //lb/hr\n",
+"ex=0.5\n",
+"hp2=210\n",
+"hv=18900 //Btu/lb\n",
+"etth=51.3\n",
+"//calculations\n",
+"ihp=hp1+hp2\n",
+"ietat= ihp*2544/(m*hv) *100\n",
+"betat=ietat*hp1/ihp\n",
+"betat2=hp1*2544/(m*hv) *100\n",
+"ietae=ietat/etth *100\n",
+"betae=betat/etth *100\n",
+"brake= ietae*hp1/ihp\n",
+"//results\n",
+"printf('Indicated efficiency = %.1f percent',ietat)\n",
+"printf('\n Brake thermal efficiency = %.1f percent',betat)\n",
+"printf('\n In case 2, Brake thermal efficiency = %.1f percent',betat2)\n",
+"printf('\n Indicated thermal efficiency = %.1f percent',ietae)\n",
+"printf('\n Brake engine efficiency = %.1f percent',betae)\n",
+"printf('\n In case 2, Brake engine efficiency = %.1f percent',brake)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 17.2: Indicated_mep_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"J=778\n",
+"o2=12.5\n",
+"theo=0.95\n",
+"N=56.5\n",
+"R0=1545\n",
+"T=540 //R\n",
+"p=14 //psia\n",
+"LHV=2368089 //Btu/lb\n",
+"ther=39.4\n",
+"iep=0.78\n",
+"ve=0.8\n",
+"//calculations\n",
+"Ar=o2/0.21 *theo\n",
+"vol=N*R0*T/(144*p)\n",
+"hv=(LHV -17730)/LHV\n",
+"ithep=iep*ther\n",
+"pd=ithep/100 *ve *100.5\n",
+"mep=J*pd\n",
+"//results\n",
+"printf('Indicated mep = %d lb/sq ft',mep)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/18-Gas_Compressors.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/18-Gas_Compressors.ipynb
new file mode 100644
index 0000000..dc79078
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/18-Gas_Compressors.ipynb
@@ -0,0 +1,279 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 18: Gas Compressors"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 18.1: Horsepower_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"q=200 //cfm\n",
+"p2=90 //psia\n",
+"p1=14.5 //psia\n",
+"n=1.36\n",
+"//calculations\n",
+"hpp=n/(n-1) *144*p1*q/33000 *(1- (p2/p1))^((n-1)/n)\n",
+"//results\n",
+"printf('Theoretical horse power required = %.1f hp',hpp)\n",
+"disp('The answer given in textbook is wrong. Please verify with a calculator')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 18.2: Horsepower_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"q=350 //cfm\n",
+"eff=0.78\n",
+"x=0.95\n",
+"p2=120 //psia\n",
+"p1=14.3 //psia\n",
+"//calculations\n",
+"cal=p1*144*q/550 *log(p2/p1) /100\n",
+"ihp= cal/eff\n",
+"shp=ihp/x\n",
+"//results\n",
+"printf('Indicated hp = %.1f hp',ihp)\n",
+"printf('\n Shaft hp = %.1f hp',shp)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 18.3: Piston_displacement_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"n=1.35\n",
+"p1=14.2\n",
+"q=400 //cfm\n",
+"p2=200 //psia\n",
+"p1=14.2 //psia\n",
+"ve=0.75\n",
+"t1=530 //R\n",
+"//calculations\n",
+"thp=-n/(n-1) *144 *p1*q/33000 *(1- (p2/p1)^((n-1)/n))\n",
+"pd=q/ve\n",
+"Tmax=t1*(p2/p1)^((n-1)/n)\n",
+"//results\n",
+"printf('Theoretical hp = %.1f hp',thp)\n",
+"printf('\n Piston displacement = %d cfm',pd)\n",
+"printf('\n Max. Temperature = %d R',Tmax)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 18.4: Piston_displacement_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"n=1.35\n",
+"p1=14.2 //psia\n",
+"p3=200 //psia\n",
+"q=400 //cfm\n",
+"ve=0.78\n",
+"t1=530 //R\n",
+"//calculations\n",
+"p2=sqrt(p3*p1) //psia\n",
+"thp=-2*n/(n-1) *144 *p1*q/33000 *(1- (p2/p1)^((n-1)/n))\n",
+"pd=q/ve\n",
+"pd2=q*p1/p2 /ve\n",
+"Tmax=t1*(p2/p1)^((n-1)/n)\n",
+"//results\n",
+"printf('Theoretical hp = %.1f hp',thp)\n",
+"printf('\n For low pressure case, Piston displacement = %.1f cfm',pd)\n",
+"printf('\n For high pressure case, Piston displacement = %.1f cfm',pd2)\n",
+"printf('\n Max. Temperature = %.1f R',Tmax)\n",
+"disp('The answers are a bit different due to rounding off error')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 18.5: Pressure_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"dia=2 //ft\n",
+"rpm=6000 //rpm\n",
+"p=14.2 //psia\n",
+"t=75 //F\n",
+"g=32.17\n",
+"n=1.4\n",
+"R=53.35\n",
+"//calculations\n",
+"v=2*%pi*rpm/60\n",
+"wbym=v^2 /g\n",
+"T=t+460\n",
+"pr=1+ wbym*(n-1)/n /(R*T) \n",
+"pr2=pr^(n/(n-1))\n",
+"p2=pr2*p\n",
+"//results\n",
+"printf('Theoretical pressure at exit = %.1f psia',p2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 18.6: Pressure_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"pa=14.7 //psia\n",
+"p1=12 //psia\n",
+"t1=560 //R\n",
+"n=1.4 //gamma\n",
+"J=778 //constant conversion\n",
+"g=32.2 //ft/s^2\n",
+"cp=0.24 //heat capacity\n",
+"eff=0.7 //efficiency\n",
+"m1=1.8 \n",
+"m3=1 \n",
+"//calculations\n",
+"t5=t1*(pa/p1)^((n-1)/n)\n",
+"v4=sqrt(2*g*J*cp*(t5-t1)/eff) \n",
+"v3=(m1+m3)/m1 *v4\n",
+"//results\n",
+"printf('Velocity of air = %.1f ft/s',v3)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 18.7: Pressure_required.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"v2=1180 //ft/s\n",
+"etan=0.95\n",
+"cp=0.24\n",
+"n=1.4\n",
+"p2=12\n",
+"//calculations\n",
+"dh=v2^2 /(etan*223.8^2)\n",
+"dt=dh/cp\n",
+"t2d=560 //R\n",
+"t1=t2d+ etan*dt\n",
+"t2=554 //R\n",
+"pr=(t1/t2)^(n/(n-1))\n",
+"p1=p2*pr\n",
+"//results\n",
+"printf('Pressure required = %.2f psia',p1)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/19-Gas_turbines.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/19-Gas_turbines.ipynb
new file mode 100644
index 0000000..bd042a0
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/19-Gas_turbines.ipynb
@@ -0,0 +1,510 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 19: Gas turbines"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.10: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"cp=0.24\n",
+"h=138.8\n",
+"t3=1960 //R\n",
+"//calculations\n",
+"t4d=t3-h/cp\n",
+"Qs=cp*(t3-t4d)\n",
+"work=43.9 //Btu/lb\n",
+"etat=work/Qs *100\n",
+"//results\n",
+"printf('Thermal efficiency of the unit = %.1f percent',etat)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.11: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"n=1.4\n",
+"t1=540 //R\n",
+"tmax=1500 //F\n",
+"pr=5\n",
+"cp=0.24\n",
+"p1=14 //psia\n",
+"p3=70 //psia\n",
+"//calculations\n",
+"pint=p1*sqrt(pr)\n",
+"t2=t1*(pint/p1)^((n-1)/n)\n",
+"t4=t1*(p3/pint)^((n-1)/n)\n",
+"w=cp*(t4-t1)\n",
+"w2=2*w\n",
+"t6=(tmax+460)/(p3/pint)^((n-1)/n)\n",
+"t8=(tmax+460)/(pint/p1)^((n-1)/n)\n",
+"work=cp*(tmax+460-t6)\n",
+"w22=2*work\n",
+"net=w22-w2\n",
+"Qa=cp*(tmax+460-t2)\n",
+"Qb=cp*(tmax+460-t6)\n",
+"Qt=Qa+Qb\n",
+"eta=net/Qt*100\n",
+"//results\n",
+"printf('Thermal efficiency = %.2f percent',eta)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.12: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"n=1.4\n",
+"t1=540 //R\n",
+"tmax=1500 //F\n",
+"pr=5\n",
+"cp=0.24\n",
+"p1=14 //psia\n",
+"p3=70 //psia\n",
+"w2=75.9 //Btu/lb\n",
+"Qa=265 //Btu/lb\n",
+"//calculations\n",
+"pint=p1*sqrt(pr)\n",
+"t6=(tmax+460)/(p3/pint)^((n-1)/n)\n",
+"t8=(tmax+460)/(pint/p1)^((n-1)/n)\n",
+"work=cp*(tmax+460-t6)\n",
+"w22=2*work\n",
+"net=w22-w2\n",
+"Qb=cp*(tmax+460-t6)\n",
+"Qt=Qa+Qb\n",
+"eta=net/Qt*100\n",
+"//results\n",
+"printf('Thermal efficiency = %.1f percent',eta)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.13: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"n=1.4\n",
+"t1=540 //R\n",
+"tmax=1500 //F\n",
+"pr=5\n",
+"cp=0.24\n",
+"t3=1558 //R\n",
+"net=125.8 //Btu/lb\n",
+"//calculations\n",
+"Q=cp*(tmax+460-t3)\n",
+"Qt=2*Q\n",
+"eta=net/Qt*100\n",
+"//results \n",
+"printf('Thermal efficiency = %.1f percent',eta)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.1: Efficiency_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"n=1.4\n",
+"t1=540 //R\n",
+"tmax=1200 //F\n",
+"tmax2=1500 //F\n",
+"pr=5\n",
+"cp=0.24\n",
+"//calculations\n",
+"t2=t1*(pr)^((n-1)/n)\n",
+"work=cp*(t2-t1)\n",
+"t4=(tmax+460) /pr^((n-1)/n)\n",
+"twork=cp*(tmax+460-t4)\n",
+"net=twork-work\n",
+"eff=1- 1/pr^((n-1)/n)\n",
+"Qs=cp*(tmax+460-t2)\n",
+"ett=net/Qs *100\n",
+"t42=(tmax2+460)/pr^((n-1)/n)\n",
+"twork2=cp*(tmax2+460-t42)\n",
+"net2=twork2-work\n",
+"Qs2=cp*(tmax2+460-t2)\n",
+"eff3=net2/Qs2 *100\n",
+"//results\n",
+"printf('Compressor work = %.1f Btu/lb',work)\n",
+"printf('\n Turbine work = %.1f Btu/lb',twork)\n",
+"printf('\n Net work = %.1f Btu/lb',net)\n",
+"printf('\n Thermal efficiency = %.1f percent',eff*100)\n",
+"printf('\n In case 2, Thermal efficiency = %.1f percent',ett)\n",
+"printf('\n In case 2, Turbine work = %.1f Btu/lb',twork2)\n",
+"printf('\n In case 2, Net work = %.1f Btu/lb',net2)\n",
+"printf('\n In case 3, Thermal efficiency = %.1f percent,',eff3)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.2: Work_and_efficiency_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"work=75.9 //Btu/lb\n",
+"twork=173.5 //Btu/lb\n",
+"eta=0.8\n",
+"t2=856 //R\n",
+"t1=540 //R\n",
+"t4=1960 //R\n",
+"cp=0.24\n",
+"//calculations\n",
+"cwork=work/eta\n",
+"internal=twork*eta\n",
+"net=-cwork+internal\n",
+"t2d=(t2-t1)/eta + t1\n",
+"Qs=cp*(t4-t2d)\n",
+"eff=net/Qs *100\n",
+"//results\n",
+"printf('Indicated compressor work = %.1f Btu/lb',cwork)\n",
+"printf('\n Internal work = %.1f Btu/lb',internal)\n",
+"printf('\n Net work = %.1f Btu/lb',net)\n",
+"printf('\n Thermal efficiency = %.2f percent',eff)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.3: Work_and_efficiency_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"eff=0.97\n",
+"c1=94.9 //Btu/lb\n",
+"c2=138.8 //Btu/lb\n",
+"ntee=246 //Btu/lb\n",
+"//calculations\n",
+"cwork=c1/eff\n",
+"twork=c2*eff\n",
+"net=twork-cwork\n",
+"etat=net/ntee *100\n",
+"//results\n",
+"printf('Compressor work = %.1f Btu/lb',cwork)\n",
+"printf('\n Turbine work = %.1f Btu/lb',twork)\n",
+"printf('\n Net work = %.1f Btu/lb',net)\n",
+"printf('\n Thermal efficiency = %.1f percent',etat)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.4: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"pr=5\n",
+"p1=14 //psia\n",
+"pd=3 //psi\n",
+"pen=70 //psia\n",
+"tin=1960 //R\n",
+"n=1.4\n",
+"cp=0.24\n",
+"Qs=265 //Btu/lb\n",
+"//calculations\n",
+"p2=p1*pr\n",
+"pe=pen-pd\n",
+"prt=pe/p1\n",
+"tex=tin/prt^((n-1)/n)\n",
+"twork=cp*(tin-tex)\n",
+"net=twork-75.9\n",
+"eff=net/Qs *100\n",
+"//results\n",
+"printf('Thermal efficiency = %.1f percent',eff)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.5: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"pr=5\n",
+"p1=14 //psia\n",
+"pd=3 //psi\n",
+"pen=70 //psia\n",
+"tin=1960 //R\n",
+"n=1.4\n",
+"cp=0.24\n",
+"Qs=265\n",
+"ef=0.95\n",
+"//calculations\n",
+"p2=p1*pr\n",
+"pe=pen-pd\n",
+"prt=pe/p1\n",
+"tex=tin/prt^((n-1)/n)\n",
+"twork=cp*(tin-tex)\n",
+"net=twork-75.9\n",
+"Qs2=Qs/ef\n",
+"eff=net/Qs2 *100\n",
+"//results\n",
+"printf('Thermal efficiency = %.1f percent',eff)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.6: Pressure_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"pr1=1.0590\n",
+"pr2=4.396\n",
+"p1=14 //psia\n",
+"//calculations\n",
+"prr=pr2/pr1\n",
+"p2=p1*prr\n",
+"//results\n",
+"printf('Final pressure = %.1f psia',p2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.7: Compressor_work.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"t1=540 //R\n",
+"h1=129.06\n",
+"pr1=1.386\n",
+"cr=5\n",
+"//calculations\n",
+"pr2=pr1*cr\n",
+"disp('From air tables,')\n",
+"h2=204.63\n",
+"cwork=h2-h1\n",
+"//results\n",
+"printf('Compressor work = %.2f Btu/lb',cwork)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.8: Turbine_work.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"cr=5\n",
+"pr3=176.73 //psia\n",
+"h3=14580.3 //Btu/mol\n",
+"M=28.9\n",
+"//calculations\n",
+"pr4=pr3/cr\n",
+"h4=9409\n",
+"twork=h3-h4\n",
+"turb=twork/M\n",
+"//results\n",
+"printf('Turbine work = %.1f Btu/lb',turb)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 19.9: Air_fuel_ratio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"chem=19000 //Btu/lb\n",
+"m1=204.63 //Btu/lb\n",
+"M=28.9\n",
+"w=14580.3\n",
+"//calculations\n",
+"ma=(chem-w/M)/(w/M -m1)\n",
+"//results\n",
+"printf('Air fuel ratio = %.1f lb air/lb fuel',ma)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/20-Vapor_power_cycles.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/20-Vapor_power_cycles.ipynb
new file mode 100644
index 0000000..5369d94
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/20-Vapor_power_cycles.ipynb
@@ -0,0 +1,276 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 20: Vapor power cycles"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 20.1: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"Qs=825.1 //Btu/lb\n",
+"ds=0.9588\n",
+"t1=101.74 //F\n",
+"th=400.95 //F\n",
+"//calculations\n",
+"Qr=ds*(t1+459.69)\n",
+"work=Qs-Qr\n",
+"eta=work/Qs*100\n",
+"eta2=(th-t1)/(th+459.69) *100\n",
+"//results\n",
+"printf('In case 1, Thermal efficiency = %.2f percent',eta)\n",
+"printf('\n In case 2, Thermal efficiency = %.2f percent',eta2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 20.2: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"s2=1.5263\n",
+"sfg=1.8456\n",
+"sf=1.9782 \n",
+"h2=1201.1 //Btu/lb\n",
+"hf=1106 //Btu/lb\n",
+"hfg=1036.3 //Btu/lb\n",
+"v=0.01616 //m^3/kg\n",
+"p2=250 //psia\n",
+"p1=1//psia\n",
+"J=778\n",
+"//calculations\n",
+"x3=1+ (s2-sf)/sfg\n",
+"h3=hf-(1-x3)*hfg\n",
+"h4=69.7\n",
+"Wp=v*144*(p2-p1)/J\n",
+"h1=h4+Wp\n",
+"etat=((h2-h3)-Wp)/(h2-h1) *100\n",
+"eta2=(h2-h3)/(h2-h4)*100\n",
+"//results\n",
+"printf('\n In case 1, Efficieny = %.2f percent',etat)\n",
+"printf('\n In case 2, Efficieny = %.2f percent',eta2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 20.3: Enthalpy_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"p=40000 //kW\n",
+"ef=0.98\n",
+"rate=302000 //lb\n",
+"s3=1.6001\n",
+"h2=1490.1\n",
+"loss=600\n",
+"v=400 //ft/s\n",
+"g=32.2 //ft/s^2\n",
+"J=778\n",
+"//calculations\n",
+"out=p/(0.746*ef)\n",
+"srate=rate/out\n",
+"X=-(s3-1.9782)/1.8456\n",
+"h3=1106 - X*1036.3\n",
+"theoturb=h2-h3\n",
+"intturb=(out+loss)*2544/rate\n",
+"Ie=intturb/theoturb *100\n",
+"h3d=h2-intturb-v^2 /(2*g*J)\n",
+"hex=h3d+ v^2 /(2*g*J)\n",
+"excess=rate*(hex-h3)\n",
+"//results\n",
+"printf('Steam rate = %.2f lb/shaft hp-hr',srate)\n",
+"printf('\n Internal engine efficiency = %.1f percent',Ie)\n",
+"printf('\n Enthalpy of exhaust steam = %.1f Btu/lb',h3d)\n",
+"printf('\n Excess heat to be removed = %d Btu/hr',excess)\n",
+"disp('The answers are a bit different due to rounding off error in textbook')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 20.4: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"s2=1.5263\n",
+"sf=1.6993\n",
+"sfg=1.3313\n",
+"hf=1164.1 //Btu/lb\n",
+"hfg=945.3 //Btu/lb\n",
+"h2=1201.1 //Btu/lb\n",
+"h1=852.3 //Btu/lb\n",
+"//calculations\n",
+"X3=-(s2-sf)/sfg\n",
+"h3=hf-X3*hfg\n",
+"h4=218.82\n",
+"h6=h4\n",
+"h5=69.7\n",
+"x=(h4-h5)/(h3-h5)\n",
+"W= h2-h3+ (1-x)*(h3-h1)\n",
+"Qs=h2-h4\n",
+"eff=W/Qs *100\n",
+"//results\n",
+"printf('Thermal efficiency = %.2f percent',eff)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 20.5: Thermal_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"h6=157.933 //Btu/lb\n",
+"s2=0.11626\n",
+"sf=0.16594\n",
+"sfg=0.14755\n",
+"hf=139.095 //Btu/lb\n",
+"hfg=126.98 //Btu/lb\n",
+"h5=12.016 //Btu/lb\n",
+"h2=1201.1 //Btu/lb\n",
+"h1=69.7 //Btu/lb\n",
+"w=348.8 //Btu/lb\n",
+"m=0.0745 //lb\n",
+"//calculations\n",
+"x7=-(s2-sf)/sfg\n",
+"h7=hf-x7*hfg\n",
+"dh6=h6-h7\n",
+"mr=(h7-h5)/(h2-h1)\n",
+"work=w*m\n",
+"tw=work+dh6\n",
+"dh65=h6-h5\n",
+"eff=tw/dh65 *100\n",
+"//results\n",
+"printf('Thermal efficiency = %.2f percent',eff)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 20.6: Heat_transferred.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"m=1 //lb\n",
+"cp=0.26\n",
+"t2=1800+460 //R\n",
+"t1=400.95+460 //R\n",
+"x=0.6\n",
+"sink=100+460 //R\n",
+"tm=2600+460 //R\n",
+"//calculations\n",
+"Q=m*cp*(t2-t1)\n",
+"ds=m*cp*log((t2/t1))\n",
+"tds=ds*(sink)\n",
+"avail=Q-tds\n",
+"hf=Q*x/(1-x)\n",
+"av2=hf*(tm-sink)/(tm)\n",
+"Qt=Q+hf\n",
+"av=avail+av2\n",
+"per=av/Qt *100\n",
+"//results\n",
+"printf('Available portion of heat transferred = %.1f percent',per)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/21-Steam_turbines.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/21-Steam_turbines.ipynb
new file mode 100644
index 0000000..90462d6
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/21-Steam_turbines.ipynb
@@ -0,0 +1,360 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 21: Steam turbines"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.1: Rate_of_flow_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"p2=190 //psia\n",
+"p1=110 //psia\n",
+"v1=2.456 \n",
+"k=1.3\n",
+"J=778\n",
+"A2=1.2 //in^2\n",
+"//calculations\n",
+"v2=v1*(p2/p1)^(1/k)\n",
+"dh=k/(k-1) *144/J *(p2*v1-p1*v2)\n",
+"Vex=223.8*sqrt(dh)\n",
+"m=A2*Vex/(144*v2)\n",
+"//results\n",
+"printf('Rate of flow = %.2f lb/sec',m)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.2: Rate_of_flow_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"h1=1205.8 //Btu/lb\n",
+"s2=1.5594\n",
+"sf=1.5948\n",
+"sfg=1.1117\n",
+"hf=1188.9 //Btu/lb\n",
+"hfg=883.2 //Btu/lb\n",
+"vf=4.049\n",
+"vfg=vf-0.018\n",
+"k=1.3\n",
+"J=778\n",
+"A2=1.2 //in^2\n",
+"//calculations\n",
+"x2=-(s2-sf)/sfg\n",
+"h2=hf-x2*hfg\n",
+"v2=vf-x2*vfg\n",
+"dh=h1-h2\n",
+"Vex=223.8*sqrt(dh)\n",
+"m=A2*Vex/(144*v2)\n",
+"//results\n",
+"printf('Rate of flow = %.2f lb/sec',m)\n",
+""
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.3: Blade_work_and_efficiency.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"alp=14 //degrees\n",
+"vb=900 //ft/s\n",
+"v1=2200 //ft/s\n",
+"g=32.17 //ft/s^2\n",
+"//calculations\n",
+"vrc=v1*cosd(alp) - vb\n",
+"W=(2*vrc)/g *vb\n",
+"eta=W/(v1^2/ (2*g)) *100\n",
+"bet=atand(v1*sind(alp) /vrc)\n",
+"//results\n",
+"printf('Blade work = %d ft-lb/lb',W)\n",
+"printf('\n Efficiency = %.1f percent',eta)\n",
+"printf('\n Blade angle = %.1f degrees',bet)\n",
+"disp('The answers are a bit different due to rounding off error')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.4: Blade_work_and_efficiency.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"v1=1234 //ft/s\n",
+"v2=532 //ft/s \n",
+"kb=0.92\n",
+"alp=20 //degrees\n",
+"ve=900 //ft/s\n",
+"r=2200 //ft/s\n",
+"g=32.17 //ft/s^2\n",
+"//calculations\n",
+"vr=sqrt(v1^2 +v2^2)\n",
+"vr2=vr*kb\n",
+"vrc=vr2*cosd(alp)\n",
+"W=(v1+vrc)*ve/g\n",
+"eta=W/(r^2 /(2*g)) *100\n",
+"//results\n",
+"printf('Blade work = %d ft-lb/lb',W)\n",
+"printf('\n Efficiency = %.1f percent',eta)\n",
+"disp('The answers are a bit different due to rounding off error')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.5: Blade_reheat_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"v1=1234\n",
+"v2=532\n",
+"kb=0.92\n",
+"alp=20 //degrees\n",
+"ve=900\n",
+"r=2200 //ft/s\n",
+"g=32.17 //ft/s^2\n",
+"J=778\n",
+"w=67000\n",
+"//calculations\n",
+"vr=sqrt(v1^2 +v2^2)\n",
+"vr2=vr*kb\n",
+"vrc=vr2*cosd(alp)\n",
+"reheat=(vr^2 - vr2^2 )/(2*g*J)\n",
+"v22=sqrt((vrc-ve)^2 +(vr2*sind(alp))^2)\n",
+"ein=r^2 /(2*g*J)\n",
+"eout=w/J + v22^2 /(2*g*J)\n",
+"re2=ein-eout\n",
+"//results\n",
+"printf('\n In case 1, Blade reheat = %.2f Btu/lb',reheat)\n",
+"printf('\n In case 2, Blade reheat = %.1f Btu/lb',re2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.6: Pressure_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"h1=1416.4\n",
+"s1=1.6842\n",
+"sf=1.7319\n",
+"sfg=1.3962\n",
+"fac=1.05\n",
+"x2=0.7\n",
+"//calculations\n",
+"x6=-(s1-sf)/sfg\n",
+"h6=1156.3 - x6*960.1\n",
+"dh6=h1-h6\n",
+"drop= fac*h6/2\n",
+"h2=h1-drop\n",
+"first=(1-x2)*drop\n",
+"h3=1264.1 +first\n",
+"h4=1157 //Btu/lb\n",
+"fac2=(drop+153)/dh6\n",
+"disp('From air charts,')\n",
+"p2=107 //psia\n",
+"//results\n",
+"printf('Intermediate pressure = %d psia',p2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.7: Shaft_output_and_efficiency_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"reh=1.047\n",
+"dh6=292.8\n",
+"x2=0.7\n",
+"flow=98000 //lb/hr\n",
+"loss=200 //hp\n",
+"//calculations\n",
+"intwork=reh*dh6*x2\n",
+"inthp=intwork*flow/2544\n",
+"sout=inthp-loss\n",
+"swork=sout*2544/flow\n",
+"seff=swork/290.1 *100\n",
+"//results\n",
+"printf('Shaft output = %d hp',sout)\n",
+"printf('\n Shaft engine efficiency = %.1f percent',seff)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.8: Pressure_at_Exit_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"h1=1416.4 //Btu/lb\n",
+"h2=214.5 //Btu/lb\n",
+"//calculations\n",
+"hex=h1-h2\n",
+"disp('From Air tables,')\n",
+"pe=20 //psia\n",
+"te=321.5 //F\n",
+"//results\n",
+"printf('Exit Pressure = %d psia',pe)\n",
+"printf('\n Exit temperature = %.1f F',te)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 21.9: Steam_rate_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"flow=98000 //lb/hr\n",
+"loss=200 //hp\n",
+"x= 0.11 //percent\n",
+"shp=3000 //hp\n",
+"//calculations\n",
+"sflow = x*flow\n",
+"sflow2= sflow + (flow-sflow)*shp/8060\n",
+"srate=sflow2/shp\n",
+"//results\n",
+"printf('Steam rate required = %.2f lb/hp-hr',srate)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/22-Refrigeration.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/22-Refrigeration.ipynb
new file mode 100644
index 0000000..9b4e86d
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/22-Refrigeration.ipynb
@@ -0,0 +1,277 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 22: Refrigeration"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 22.1: cop_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"t1=45+460 //R\n",
+"th=70+460 //R\n",
+"t2=-200+460 //R\n",
+"th2=100+460 //R\n",
+"//calculations\n",
+"cp1=t1/(th-t1)\n",
+"cp2=th/(th-t1)\n",
+"cp3=t2/(th2-t2)\n",
+"cp4=th2/(th2-t2)\n",
+"//results\n",
+"printf('In case 1, Refrigerator cp = %.1f',cp1)\n",
+"printf('\n In case 1, Heat pump cp = %.1f',cp2)\n",
+"printf('\n In case 2, Refrigerator cp = %.3f',cp3)\n",
+"printf('\n In case 2, Heat pump cp = %.3f',cp4)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 22.2: cop_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"h3=85.282 //Btu/lb\n",
+"s2=0.16392\n",
+"sf=0.16798\n",
+"//calculations\n",
+"sfg=sf-0.023954\n",
+"x3=-(s2-sf)/sfg\n",
+"h2=78.335 - x3*67.651\n",
+"h4=26.365 //Btu/lb\n",
+"h1=h4\n",
+"ref=h2-h1\n",
+"work=h3-h2\n",
+"cp1=ref/work\n",
+"h2d=78.355\n",
+"h1d=26.365 //Btu/lb\n",
+"h3d=87.495 //Btu/lb\n",
+"ref2=h2d-h1d\n",
+"work2=h3d-h2d\n",
+"cp2=ref2/work2\n",
+"//results\n",
+"printf('\n Coefficient of performance in wet compression = %.3f',cp1)\n",
+"printf('\n Coefficient of performance in dry compression = %.3f',cp2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 22.3: Tonnage_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"h1=24.973 //Btu/lb\n",
+"h2=81.436 //Btu/lb\n",
+"cfm=200 //cfm\n",
+"v2=0.77357\n",
+"v3=3.8750\n",
+"h4=72.913\n",
+"//calculations\n",
+"mass=cfm/v2\n",
+"ref=h2-h1\n",
+"tonnage=mass*ref/cfm\n",
+"mass2=cfm/v3\n",
+"ref2=h4-h1\n",
+"tonnage2=mass2*ref2/cfm\n",
+"//results\n",
+"printf('In case 1,Tonnage = %.1f tons',tonnage)\n",
+"printf('\n In case 2,Tonnage = %.2f tons',tonnage2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 22.4: Refrigeration_and_cop_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"h2d=93.410 //Btu/lb\n",
+"h1=80.740 //Btu/lb\n",
+"x=0.75\n",
+"PD=160\n",
+"vol=0.82\n",
+"v1=1.7213\n",
+"w2=80.156\n",
+"w1=27.3\n",
+"//calculations\n",
+"twork=h2d-h1\n",
+"swork=twork/x\n",
+"flow=PD*vol/v1\n",
+"ref=flow*(w2-w1)/200\n",
+"shp= flow*swork/42.4\n",
+"cop=(w2-w1)/swork\n",
+"//results\n",
+"printf('Refrigeration = %.1f tons',ref)\n",
+"printf('\n Shaft hp= %.1f hp',shp)\n",
+"printf('\n Coefficient of performance = %.2f ',cop)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 22.5: cop_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"mc=3000 //lb\n",
+"hv=1080.2 //Btu/lb\n",
+"hfe=26.06 //Btu/lb\n",
+"hfp=10.05 //Btu/lb\n",
+"x=0.7\n",
+"//calculations\n",
+"mv=(mc*hfp-mc*hfe)/(hfe-hv)\n",
+"dh=145.4 //Btu/lb\n",
+"chp=dh*mv/(x*42.4)\n",
+"cop=mc*(hfe-hfp)/(chp*42.4)\n",
+"//results\n",
+"printf('Coefficient of performace = %.2f ',cop)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 22.6: Power_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"loss=80000 //Btu/lb\n",
+"t=560 //R\n",
+"//calculations\n",
+"ratio=t/68\n",
+"power=loss/(ratio*2544)\n",
+"//results\n",
+"printf('Power = %.2f hp',power)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 22.7: Power_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"loss=2*80000 //Btu/lb\n",
+"tb=72 //F\n",
+"to=12 //F\n",
+"to2=42 //F\n",
+"tf=104+460 //R\n",
+"//calculations\n",
+"ratio=tf/(tf-460)\n",
+"power=loss/(2544*ratio)\n",
+"//results\n",
+"printf('Power = %.1f hp',power)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/23-Gas_vapor_mixtures.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/23-Gas_vapor_mixtures.ipynb
new file mode 100644
index 0000000..5571515
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/23-Gas_vapor_mixtures.ipynb
@@ -0,0 +1,319 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 23: Gas vapor mixtures"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 23.1: Specific_humidity_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"pv=0.3631 //psia\n",
+"pa=14.7 //psia\n",
+"cp=0.24\n",
+"tw=70 //F\n",
+"td=80 //F\n",
+"hv1=1096.6 //Btu/lb\n",
+"hfb=38.06 //Btu/lb\n",
+"//calculations\n",
+"sh=0.622*pv/(pa-pv)\n",
+"sh1=(cp*tw -cp*td + sh*1054.3)/(hv1-hfb)\n",
+"//results\n",
+"printf('Specific humidity = %.5f lb/lb',sh1)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 23.2: RH_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"rel=0.9\n",
+"p1=0.0396 //psia\n",
+"p2=0.3631 //psia\n",
+"//calculations\n",
+"act=rel*p1\n",
+"RH=act/p2 *100\n",
+"//results\n",
+"printf('Relative humidity = %.1f percent',RH)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 23.3: Temperature_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"pa=14.2\n",
+"rel=0.9\n",
+"sh=0.012 //lb/lb\n",
+"//calculations\n",
+"pv=(pa*sh)/(0.622-sh)\n",
+"sat=pv/rel\n",
+"tf=64.34 //F\n",
+"//results\n",
+"printf('From steam tables, by interpolation, Final temperature = %.2f F',tf)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 23.4: Heat_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"pa=14.7\n",
+"pv=0.0356\n",
+"pv2=0.04\n",
+"cp=0.24\n",
+"t1=70 //F\n",
+"t2=15 //F\n",
+"R=53.35\n",
+"V=8000 //ft^3\n",
+"//calculations\n",
+"sh=0.622*pv/(pa-pv2)\n",
+"hm2=cp*t1+ sh*1092.3\n",
+"hm1=cp*t2+sh*1068.4\n",
+"Q=hm2-hm1\n",
+"m=144*(pa-pv2)*V/(R*(t2+460))\n",
+"Q2=Q*m\n",
+"//results\n",
+"printf('Heat added per min = %d Btu/min',Q2)\n",
+"disp('The answer is a bit different due to rounding off error in the textbook')"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 23.5: Temperature_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"rel=0.45\n",
+"p1=0.4747 //psia\n",
+"disp('From steam table data,')\n",
+"//calculations\n",
+"act=rel*p1\n",
+"t2=54.94 //F\n",
+"//results\n",
+"printf('Temperature = %.2f F',t2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 23.6: Tonnage_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"rel=0.6\n",
+"p1=0.6982 //psia\n",
+"pa=14.7 //psia\n",
+"t1=90 //F\n",
+"t2=54.94 //F\n",
+"cp=0.24\n",
+"p2=0.2136 //psia\n",
+"vol=4000 //ft\n",
+"t3=538 //R\n",
+"R=53.35\n",
+"//calculations\n",
+"act1=rel*p1\n",
+"sh1=0.622*act1/(pa-act1)\n",
+"hm1=cp*t1+sh1*1100.9\n",
+"sh2=0.622*p2/(pa-p2)\n",
+"hm2=cp*t2+sh2*1085.8\n",
+"con=sh1-sh2\n",
+"enth=con*23.01\n",
+"heat=hm1-hm2-enth\n",
+"mass=144*(pa-p2)*vol/(R*(t3))\n",
+"tonnage=mass*heat/200\n",
+"//results\n",
+"printf('Tonnage = %.1f tons ',tonnage)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 23.7: Tonnage_calculation.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"p1=0.541 //psia\n",
+"rel=0.48\n",
+"pa=14.7 //psia\n",
+"t1=82 //F\n",
+"cp=0.24\n",
+"m1=0.75 //lb\n",
+"m2=0.25 //lb\n",
+"hm4=23.15 //Btu/lb\n",
+"mass=291 //lb\n",
+"//calculations\n",
+"p2=rel*p1\n",
+"sh=0.622*p2/(pa-p2)\n",
+"hm1=cp*t1 + sh*1097.5\n",
+"hm2=m1*hm1\n",
+"hm3=m2*41.67\n",
+"heat=hm2+hm3-hm4\n",
+"tonnage=heat*mass/200\n",
+"//results\n",
+"printf('Tonnage = %.2f tons',tonnage)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 23.8: Volume_calculatio.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initalization of variables\n",
+"ce=0.8\n",
+"t1=115 //F\n",
+"tc=75 //F\n",
+"td=85 //F\n",
+"pa=14.7 //psia\n",
+"p1=0.43 //psia\n",
+"p2=0.9492 //psia\n",
+"m1=159600\n",
+"m2=31.65\n",
+"R=53.35\n",
+"T=545 //R\n",
+"//calculations\n",
+"t2=t1-ce*(t1-tc)\n",
+"Pv=0.4298- (pa-p1)*(td-tc)/(2800- 1.3*tc) \n",
+"sh1=0.622*Pv/(pa-Pv)\n",
+"sh2=0.622 *p2/(pa-p2)\n",
+"mda=m1/m2\n",
+"V=mda*R*T/(144*(pa-Pv))\n",
+"amount=mda*(sh2-sh1)\n",
+"//results\n",
+"printf('Volume of entering air = %d cfm',V)\n",
+"printf('\n Amount of make up water = %.1f lb/min',amount)\n",
+"disp('The answers are a bit different due to rounding off error in textbook')"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/5-Actual_Gases.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/5-Actual_Gases.ipynb
new file mode 100644
index 0000000..32085c9
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/5-Actual_Gases.ipynb
@@ -0,0 +1,167 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 5: Actual Gases"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 5.1: Volume_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"m=20 //lbm\n",
+"P=1000 //psia\n",
+"T=580 //R\n",
+"R=35.12\n",
+"//calculations\n",
+"disp('From table 5-2,')\n",
+"z=0.667\n",
+"V=z*m*R*T/(P*144)\n",
+"vt=0.0935\n",
+"vtt=vt*m\n",
+"//results\n",
+"printf('Volume occupied = %.3f cu ft',V)\n",
+"printf('\n Tablulated value for volume = %.2f cu ft',vtt)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 5.2: Pressure_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"m=90 //lbm\n",
+"T=200+459.7 //R\n",
+"Tc=232.7+459.7 //R\n",
+"R0=1545\n",
+"M=120.9\n",
+"V=30 //cu ft\n",
+"//calculations\n",
+"R=R0/M\n",
+"disp('From fig 5.5')\n",
+"z=0.883\n",
+"P=z*R*m*T/V/144\n",
+"vc=V/m\n",
+"P2=156.1 //psia\n",
+"//results\n",
+"printf('Pressure obtained = %.2f psia',P)\n",
+"printf('\n Theoretical pressure = %.1f psia',P2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 5.3: Heat_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"T1=140+460 //R\n",
+"T2=240 +460 //R\n",
+"N=1\n",
+"//calculations\n",
+"Q=N*(9.47*(T2-T1)-3.47*10^3 *log(T2/T1) -1.16*10^6 *(1/T2-1/T1))\n",
+"Tm=(T1+T2)/2\n",
+"Cp=9.47-3.47*10^3 /Tm +1.16*10^6 /Tm^2\n",
+"Q2=N*Cp*(T2-T1)\n",
+"//results\n",
+"printf('Heat added in case 1 = %d Btu',Q)\n",
+"printf('\n Heat added in case 2 = %.1f Btu',Q2)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 5.4: Heat_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"Rj=1.985\n",
+"N=1\n",
+"T1=540+460 //R\n",
+"T2=3540+460 //R\n",
+"//calculations\n",
+"Q=N*(14.215*(T2-T1)-6.53*10^3 *log(T2/T1) -1.41*10^6 *(1/T2-1/T1))\n",
+"Tm=(T1+T2)/2\n",
+"Cv=14.215-6.53*10^3 /Tm +1.41*10^6 /Tm^2\n",
+"Q2=N*Cv*(T2-T1)\n",
+"//results\n",
+"printf('Heat added in case 1 = %.1f Btu',Q)\n",
+"printf('\n Heat added in case 2 = %.1f Btu',Q2)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/7-Entropy.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/7-Entropy.ipynb
new file mode 100644
index 0000000..4958a29
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/7-Entropy.ipynb
@@ -0,0 +1,67 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 7: Entropy"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 7.1: Change_in_Entropy.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"T2=920 //R\n",
+"T1=520 //R\n",
+"P1=14 //psia\n",
+"P2=84 //psia\n",
+"J=778\n",
+"R=53.35\n",
+"cv=0.1715\n",
+"N=1\n",
+"//calculations\n",
+"k= log(T2/T1) /log(P2/P1)\n",
+"n=1/(1-k)\n",
+"cx=cv+R/(J*(1-n))\n",
+"dS=N*cx*log(T2/T1)\n",
+"//results\n",
+"printf('Change in entropy = %.5f unit of entropy',dS)"
+ ]
+ }
+],
+"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
+}
diff --git a/Thermodynamics_for_Engineers_by_J_S_Doolittle/8-Availability_of_Energy.ipynb b/Thermodynamics_for_Engineers_by_J_S_Doolittle/8-Availability_of_Energy.ipynb
new file mode 100644
index 0000000..f41176a
--- /dev/null
+++ b/Thermodynamics_for_Engineers_by_J_S_Doolittle/8-Availability_of_Energy.ipynb
@@ -0,0 +1,108 @@
+{
+"cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter 8: Availability of Energy"
+ ]
+ },
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 8.1: Energy_loss_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"q=1000 //Btu\n",
+"th=1140 //F\n",
+"tl=40 //F\n",
+"ts=940 //F\n",
+"//calculations\n",
+"Q1=q*(th-tl)/(th+460)\n",
+"Q2=q*(ts-tl)/(ts+460)\n",
+"dif=Q1-Q2\n",
+"//results\n",
+"printf('Available energy loss = %d Btu',dif)"
+ ]
+ }
+,
+{
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 8.2: Energy_loss_calculations.sce"
+ ]
+ },
+ {
+"cell_type": "code",
+ "execution_count": null,
+ "metadata": {
+ "collapsed": true
+ },
+ "outputs": [],
+"source": [
+"clc\n",
+"clear\n",
+"//Initialization of variables\n",
+"ma=200000 //lb\n",
+"cpa=0.26\n",
+"T2g=1200 //F\n",
+"T1g=300 //F\n",
+"T1w=200 //F\n",
+"mw=250000 //lb\n",
+"cpw=1.02\n",
+"Tl=560 //R\n",
+"cx=1.01\n",
+"//calculations\n",
+"T2w=T1w+ ma*cpa*(T2g-T1g)/(mw*cpw)\n",
+"Qun=Tl*ma*cpa*log((T2g+460)/(T1g+460))\n",
+"Qtr=ma*cpa*(T2g-T1g)\n",
+"Qav=Qtr-Qun\n",
+"Qun2=Tl*mw*cx*log((T2w+460)/(T1w+460))\n",
+"Qav2=Qtr-Qun2\n",
+"ht1=Qav-Qav2\n",
+"//results\n",
+"printf('For gas, Untransferred energy = %d Btu/hr',Qun)\n",
+"printf('\n For gas, transferred energy = %d Btu/hr',Qtr)\n",
+"printf('\n For gas, available energy = %d Btu/hr',Qav)\n",
+"printf('\n For water, Untransferred energy = %d Btu/hr',Qun2)\n",
+"printf('\n For water, available energy = %d Btu/hr',Qav2)\n",
+"printf('\n Loss of available energy = %d Btu/hr',ht1)\n",
+"disp('The answers are a bit different due to rounding off error in textbook')"
+ ]
+ }
+],
+"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
+}