summaryrefslogtreecommitdiff
path: root/sample_notebooks/VineshSaini/ch10.ipynb
diff options
context:
space:
mode:
authorTrupti Kini2016-08-30 23:30:24 +0600
committerTrupti Kini2016-08-30 23:30:24 +0600
commit4d212577396e7d6a0c810f0ce0ec4cb863cad3bc (patch)
tree7a4152fafdd5fb45468a3d5c0be29ac56ec3f1c9 /sample_notebooks/VineshSaini/ch10.ipynb
parente05977ece06f8cd61b53adcff9febb2e443de861 (diff)
downloadPython-Textbook-Companions-4d212577396e7d6a0c810f0ce0ec4cb863cad3bc.tar.gz
Python-Textbook-Companions-4d212577396e7d6a0c810f0ce0ec4cb863cad3bc.tar.bz2
Python-Textbook-Companions-4d212577396e7d6a0c810f0ce0ec4cb863cad3bc.zip
Added(A)/Deleted(D) following books
A Digital_Communications_by_S._Haykin/Chapter1.ipynb A Digital_Communications_by_S._Haykin/Chapter2.ipynb A Digital_Communications_by_S._Haykin/Chapter3.ipynb A Digital_Communications_by_S._Haykin/Chapter4.ipynb A Digital_Communications_by_S._Haykin/Chapter5.ipynb A Digital_Communications_by_S._Haykin/Chapter6.ipynb A Digital_Communications_by_S._Haykin/Chapter7.ipynb A Digital_Communications_by_S._Haykin/Chapter8.ipynb A Digital_Communications_by_S._Haykin/Chapter9.ipynb A Digital_Communications_by_S._Haykin/screenshots/Ch-6_RaisedCosineSpectrum.png A Digital_Communications_by_S._Haykin/screenshots/Ch6_powerSpectralDensities.png A Digital_Communications_by_S._Haykin/screenshots/ch6_sinc_pilse.png A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/README.txt A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch1.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch10.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch11.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch12.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch13.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch14.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch2.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch3.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch4.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch5.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch6.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch7.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch8.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/ch9.ipynb A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/screenshots/14.png A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/screenshots/2.png A Heat_And_Mass_Transfer_-_A_Practical_Approach_by_Y._A._Cengel/screenshots/5.png A sample_notebooks/VineshSaini/ch10.ipynb
Diffstat (limited to 'sample_notebooks/VineshSaini/ch10.ipynb')
-rw-r--r--sample_notebooks/VineshSaini/ch10.ipynb351
1 files changed, 351 insertions, 0 deletions
diff --git a/sample_notebooks/VineshSaini/ch10.ipynb b/sample_notebooks/VineshSaini/ch10.ipynb
new file mode 100644
index 00000000..07f94034
--- /dev/null
+++ b/sample_notebooks/VineshSaini/ch10.ipynb
@@ -0,0 +1,351 @@
+{
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "# Chapter10 Elliptical Partial Differential Equations"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.1 page 441"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 1,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "u:\n",
+ "[[ 0. 0. 0. 0. 0. ]\n",
+ " [ 0. 6.25 12.5 18.75 25. ]\n",
+ " [ 0. 12.5 25. 37.5 50. ]\n",
+ " [ 0. 18.75 37.5 56.25 75. ]\n",
+ " [ 0. 25. 50. 75. 100. ]]\n"
+ ]
+ }
+ ],
+ "source": [
+ "from __future__ import division\n",
+ "from numpy import arange,zeros\n",
+ "from math import ceil\n",
+ "\n",
+ "h = 1/4\n",
+ "xf = 1\n",
+ "yf = 1\n",
+ "x = arange(0,h+xf,h)\n",
+ "y = arange(0,h+yf,h)\n",
+ "m = len(y)-1\n",
+ "n = len(x)-1\n",
+ "\n",
+ "u = zeros([m+1,n+1])\n",
+ "u[m,:] = [100*xx for xx in x]\n",
+ "u[:,n] = [100*yy for yy in y] # dash transpose\n",
+ "u0 = u\n",
+ "\n",
+ "I = int(ceil(m/2)) #\n",
+ "J = int(ceil(n/2)) #\n",
+ "\n",
+ "u[J,I] = (u0[J-2,I-2] + u0[J-2,I+2] + u0[J+2,I-2] + u0[J+2,I+2]) / 4\n",
+ "\n",
+ "for j in [J-1,J+1]:\n",
+ " for i in [I-1,I+1]:\n",
+ " u[j,i] = (u[j-1,i-1] + u[j-1,i+1] + u[j+1,i-1] + u[j+1,i+1]) / 4\n",
+ " \n",
+ "\n",
+ "# j and i may have loose 1\n",
+ "j1 = [J-1,J,J,J+1]\n",
+ "i1 = [I,I-1,I+1,I]\n",
+ "for k in range(0,4):\n",
+ " i = i1[(k)]\n",
+ " j = j1[(k)]\n",
+ " u[j,i] = (u[j,i-1] + u[j,i+1] + u[j-1,i] + u[j+1,i]) / 4\n",
+ "\n",
+ "\n",
+ "print \"u:\\n\",u"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.3 page 442"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 2,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ " r u11 u21 u31 u12 u22 u32 u13 u23 u33\n",
+ " ------------------------------------------------------------------------------------------------\n",
+ " 1 6.2500 9.3750 6.2500 18.7500 25.0000 18.7500 43.7500 53.1250 43.7500 \n",
+ " 1 7.0312 9.5703 7.0801 18.9453 25.0977 18.9819 43.0176 52.9663 42.9871 \n",
+ " 1 7.1289 9.8267 7.2021 18.8110 25.1465 18.8339 42.9443 52.7695 42.9008 \n"
+ ]
+ }
+ ],
+ "source": [
+ "from numpy import zeros\n",
+ "m = 5\n",
+ "n = 5\n",
+ "u = zeros([m,n])\n",
+ "u[m-1,:] = [50,100, 100, 100, 50]\n",
+ "u0 = u\n",
+ "I = int(ceil(m/2))-1\n",
+ "J = int(ceil(n/2))-1\n",
+ "\n",
+ "u[J,I] = (u0[J-2,I-2] + u0[J-2,I+2] + u0[J+2,I-2] + u0[J+2,I+2]) / 4\n",
+ "\n",
+ "for j in [J-1,J+1]:\n",
+ " for i in [I-1,I+1]:\n",
+ " u[j,i] = (u[j-1,i-1] + u[j-1,i+1] + u[j+1,i-1] + u[j+1,i+1]) / 4\n",
+ " \n",
+ "\n",
+ "j1 = [J-1, J ,J ,J+1]\n",
+ "i1 = [I ,I-1, I+1, I]\n",
+ "for k in range(0,4):\n",
+ " i = i1[(k)]\n",
+ " j = j1[(k)]\n",
+ " u[j,i] = (u[j,i-1] + u[j,i+1] + u[j-1,i] + u[j+1,i]) / 4\n",
+ "\n",
+ "\n",
+ "kf = 2\n",
+ "tab = zeros([kf+1,(m-2)*(n-2)])\n",
+ "row = []\n",
+ "for j in range(1,n-1):\n",
+ " for xx in u[j,range(1,m-1)]:\n",
+ " row.append(xx)\n",
+ "\n",
+ "tab[0,:] = row;\n",
+ "for k in range(0,kf):\n",
+ " row = [];\n",
+ " for j in range(1,n-1):\n",
+ " for i in range(1,m-1):\n",
+ " u[j,i] = (u[j,i-1] + u[j,i+1] + u[j-1,i] + u[j+1,i]) / 4;\n",
+ " for xx in u[j,range(1,m-1)]: \n",
+ " row.append(xx)\n",
+ " \n",
+ " row = [round(roww*10**4,4)/10**4 for roww in row]\n",
+ " tab[k+1,:] = row\n",
+ "\n",
+ "print \"%4s %9s %9s %9s %9s %10s %10s %10s %10s %10s\"%('r','u11','u21','u31','u12','u22','u32','u13','u23','u33')\n",
+ "print ' ','-'*96\n",
+ "for tabb in tab:\n",
+ " i=1;\n",
+ " print ' ',i,' ',\n",
+ " for tt in tabb:\n",
+ " print ' %0.4f'%(tt),' ',\n",
+ " i+=1;\n",
+ " print"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.4 page 444"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 3,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ " r u11 u21 u12 u22\n",
+ " 1 1.3889 1.7670 2.0170 2.6466 \n",
+ " 2 2.3349 2.6651 2.9151 3.0957 \n",
+ " 3 2.7840 2.8897 3.1397 3.2079 \n",
+ " 4 2.8962 2.9458 3.1958 3.2360 \n",
+ " 5 2.9243 2.9598 3.2098 3.2430 \n"
+ ]
+ }
+ ],
+ "source": [
+ "from numpy import arange\n",
+ "h = 1/3\n",
+ "x = arange(0,h+1,h)\n",
+ "y = arange(0,h+1,h)\n",
+ "m = len(y)\n",
+ "n = len(x)\n",
+ "u = zeros([m,n])\n",
+ "u[m-1,range(1,n-1)] = 1\n",
+ "\n",
+ "kf = 5\n",
+ "tab = zeros([kf,(m-2)*(n-2)])\n",
+ "for k in range(0,kf):\n",
+ " row = []\n",
+ " for j in range(1,n-1):\n",
+ " for i in range(1,m-1):\n",
+ " constant = 10/9* (5 + 1/9*(i-1)**2 + 1/9*(j-1)**2)\n",
+ " u[j,i] = (u[j,i-1] + u[j,i+1] + u[j-1,i] + u[j+1,i] + constant) / 4\n",
+ " for xx in u[j,range(1,m-1)]:\n",
+ " row.append(xx)\n",
+ " \n",
+ " row = [round(roww*10**4)/10**4 for roww in row]\n",
+ " tab[k,:] = row\n",
+ "\n",
+ "print \"%4s %9s %9s %9s %9s\"%('r','u11','u21','u12','u22')\n",
+ "i=1;\n",
+ "for tabb in tab:\n",
+ " \n",
+ " print ' ',i,' ',\n",
+ " for tt in tabb:\n",
+ " print ' %0.4f'%(tt),' ',\n",
+ " i+=1;\n",
+ " print"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "metadata": {},
+ "source": [
+ "## Example 10.5 page 446"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 4,
+ "metadata": {
+ "collapsed": false
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "u:\n",
+ "[[ 0. 0. 0. 0. 0. ]\n",
+ " [ 0. 4. 8. 12. 16. ]\n",
+ " [ 0. 6.5 16. 22.5 32. ]\n",
+ " [ 0. 6. 15. 30. 48. ]\n",
+ " [ 0. 1. 8. 27. 64. ]]\n",
+ "\n",
+ "\n",
+ "\t u11 u21 u31 u12 u22 u32 u13 u23 u33\n",
+ " 1 4.0000 8.0000 12.0000 6.5000 16.0000 22.5000 6.0000 15.0000 30.0000 \n",
+ " 2 3.5605 7.8712 11.5228 6.3712 12.4085 21.3079 5.5228 13.8079 27.1039 \n",
+ " 3 3.5606 6.7013 10.9128 5.2013 11.6421 20.2611 4.9128 12.7611 26.9886 \n",
+ " 4 2.8750 6.2983 10.5929 4.7983 10.9244 20.1033 4.5929 12.6033 26.9160 \n",
+ " 5 2.7568 6.0290 10.5228 4.5290 10.7975 20.0515 4.5228 12.5515 26.8981 \n",
+ " 6 2.6193 5.9773 10.5045 4.4773 10.7587 20.0384 4.5045 12.5384 26.8935 \n",
+ " 7 2.6127 5.9675 10.5010 4.4675 10.7520 20.0363 4.5010 12.5363 26.8931 \n",
+ " 8 2.6081 5.9649 10.5002 4.4649 10.7504 20.0358 4.5002 12.5358 26.8929 \n",
+ " 9 2.6073 5.9644 10.5000 4.4644 10.7501 20.0357 4.5000 12.5357 26.8929 \n",
+ " 10 2.6072 5.9643 10.5000 4.4643 10.7500 20.0357 4.5000 12.5357 26.8929 \n",
+ " 11 2.6072 5.9643 10.5000 4.4643 10.7500 20.0357 4.5000 12.5357 26.8929 \n"
+ ]
+ }
+ ],
+ "source": [
+ "from math import ceil\n",
+ "from numpy import cos,pi,sqrt,zeros\n",
+ "x = range(0,5)\n",
+ "y = range(0,5)\n",
+ "m = len(y)\n",
+ "n = len(x)\n",
+ "u = zeros([m,n])\n",
+ "u[m-1,:] = [xx**3 for xx in x]\n",
+ "u[:,n-1] = [16*yy for yy in y]\n",
+ "u0 = u\n",
+ "\n",
+ "I = int(ceil(m/2))-1\n",
+ "J = int(ceil(n/2))-1\n",
+ "\n",
+ "u[J,I] = (u0[J-2,I-2] + u0[J-2,I+2] + u0[J+2,I-2] + u0[J+2,I+2]) / 4\n",
+ "\n",
+ "for j in [J-1,J+1]:\n",
+ " for i in [I-1,I+1]:\n",
+ " u[j,i] = (u[j-1,i-1] + u[j-1,i+1] + u[j+1,i-1] + u[j+1,i+1]) / 4\n",
+ " \n",
+ "\n",
+ "\n",
+ "j1 = [J-1,J ,J ,J+1]\n",
+ "i1 = [I, I-1, I+1, I]\n",
+ "for k in range(0,4):\n",
+ " i = i1[(k)]\n",
+ " j = j1[(k)]\n",
+ " u[j,i] = (u[j,i-1] + u[j,i+1] + u[j-1,i] + u[j+1,i]) / 4\n",
+ "\n",
+ "print \"u:\\n\",u\n",
+ "\n",
+ "p = m-1\n",
+ "q = n-1\n",
+ "c = cos(pi/p) + cos(pi/q)\n",
+ "w = 4/(2+sqrt(4-c**2))\n",
+ "w = round(w*10**3)/10**3\n",
+ "\n",
+ "kf = 10\n",
+ "tab = zeros([kf+1,(m-2)*(n-2)])\n",
+ "row = []\n",
+ "for j in range(1,n-1):\n",
+ " for xx in u[j,range(1,m-1)]:\n",
+ " row.append(xx)\n",
+ "\n",
+ "tab[0,:] = row\n",
+ "for k in range(0,kf):\n",
+ " row = []\n",
+ " for j in range(1,n-1):\n",
+ " for i in range(1,m-1):\n",
+ " u[j,i] = (u[j,i-1] + u[j,i+1] + u[j-1,i] + u[j+1,i]) *w/4 + (1-w)*u[j,i]\n",
+ " for xx in u[j,range(1,m-1)]:\n",
+ " row.append(xx)\n",
+ " \n",
+ " row = [round(roww*10**4)/10**4 for roww in row]\n",
+ " tab[k+1,:] = row\n",
+ "\n",
+ "print \"\\n\\n\\t%8s %9s %10s %10s %9s %10s %10s %9s %9s\"%('u11','u21','u31','u12','u22','u32','u13','u23','u33')\n",
+ "i=1;\n",
+ "for tabb in tab:\n",
+ " \n",
+ " print ' ',i,' ',\n",
+ " for tt in tabb:\n",
+ " print ' %0.4f'%(tt),' ',\n",
+ " i+=1;\n",
+ " print\n"
+ ]
+ }
+ ],
+ "metadata": {
+ "kernelspec": {
+ "display_name": "Python 2",
+ "language": "python",
+ "name": "python2"
+ },
+ "language_info": {
+ "codemirror_mode": {
+ "name": "ipython",
+ "version": 2
+ },
+ "file_extension": ".py",
+ "mimetype": "text/x-python",
+ "name": "python",
+ "nbconvert_exporter": "python",
+ "pygments_lexer": "ipython2",
+ "version": "2.7.9"
+ }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 0
+}