From 534e42c1dee8fefa92f28d4496f273f8c6e4bd94 Mon Sep 17 00:00:00 2001
From: FOSSEE SysAds
Date: Tue, 8 Dec 2015 15:04:13 +0600
Subject: Added(A)/Deleted(D) following books  A 
 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/README.txt
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/ch2_1.ipynb
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/ch3_1.ipynb
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/ch4_1.ipynb
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/ch5_1.ipynb
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/ch6_1.ipynb
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/ch7_1.ipynb
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/ch8_1.ipynb
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/ch9_1.ipynb
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/screenshots/ch2_1.png
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/screenshots/ch7_1.png
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 A_Course_In_Mechanical_Measurements_And_Instrumentation_by_A._K._Sawhney_And_P._Sawhney/screenshots/kVSv5.png
 A  A_First_Course_on_Electrical_Drives_by_S._K._Pillai/CHAPTER2_1.ipynb A 
 A_First_Course_on_Electrical_Drives_by_S._K._Pillai/CHAPTER4_2.ipynb A 
 A_First_Course_on_Electrical_Drives_by_S._K._Pillai/CHAPTER5_2.ipynb A 
 A_First_Course_on_Electrical_Drives_by_S._K._Pillai/CHAPTER6_2.ipynb A 
 A_First_Course_on_Electrical_Drives_by_S._K._Pillai/CHAPTER7_2.ipynb A 
 A_First_Course_on_Electrical_Drives_by_S._K._Pillai/README.txt A 
 A_First_Course_on_Electrical_Drives_by_S._K._Pillai/screenshots/CHAP2.png A 
 A_First_Course_on_Electrical_Drives_by_S._K._Pillai/screenshots/CHAP4.png A 
 A_First_Course_on_Electrical_Drives_by_S._K._Pillai/screenshots/CHAP5.png D 
 A_First_course_in_Programming_with_C/Chapter14.ipynb M 
 A_First_course_in_Programming_with_C_by_T_Jeyapoovan/Chapter14_2.ipynb A 
 A_First_course_in_Programming_with_C_by_T_Jeyapoovan/README.txt A 
 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT1.2.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT1.3.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT1.7.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT1_2.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT1_3.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT1_7.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.10.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.11.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.13.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.14.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.15.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.16.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.17.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.18.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.2.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.3.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.4.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.5.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.6.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.7.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.8.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2.9.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_10.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_11.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_13.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_14.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_15.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_16.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_17.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_18.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_2.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_3.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_4.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_5.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_6.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_7.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_8.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT2_9.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.1.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.10.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.2.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.3.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.4.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.6.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.7.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.8.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3.9.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_1.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_10.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_2.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_3.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_4.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_6.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_7.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_8.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT3_9.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.1.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.2.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.3.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.4.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.5.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.6.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.7.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.8.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4.9.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4_1.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4_2.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4_3.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4_5.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4_6.ipynb
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 A_Textbook_on_Power_System_Engineering_by_A_Chakrabarti,_M_L_Soni,_P_V_Gupta,_U_S_Bhatnagar/CHAPT4_7.ipynb
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+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#10: Optical Materials"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.1, Page number 10.61"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 32,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "wavelength of emission is 8628.0 angstrom\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "h=6.626*10**-34;       #plancks constant(J s)\n",
+    "c=3*10**8;     #velocity of light(m/s)\n",
+    "Eg=1.44*1.6*10**-19;    #band gap(J)\n",
+    "\n",
+    "#Calculation\n",
+    "lamda=h*c/Eg;      #wavelength of emission(m)\n",
+    "\n",
+    "#Result\n",
+    "print \"wavelength of emission is\",round(lamda*10**10),\"angstrom\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.2, Page number 10.61"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 33,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "band gap is 0.8 eV\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "lamda=1.55;     #wavelength(micro m)\n",
+    "\n",
+    "#Calculation\n",
+    "Eg=1.24/lamda;     #band gap(eV)\n",
+    "\n",
+    "#Result\n",
+    "print \"band gap is\",Eg,\"eV\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.3, Page number 10.61"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 34,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "number of electron-hole pairs is 3.25 *10**5\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "eta=0.65;     #quantum efficiency\n",
+    "n=5*10**5;    #number of photons incident\n",
+    "\n",
+    "#Calculation\n",
+    "N=eta*n;      #number of electron-hole pairs\n",
+    "\n",
+    "#Result\n",
+    "print \"number of electron-hole pairs is\",N/10**5,\"*10**5\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.4, Page number 10.61"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 35,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "responsibility is 0.628 A/W\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "eta=0.6;     #quantum efficiency\n",
+    "q=1.6*10**-19;    #charge(coulomb)\n",
+    "lamda=1.3*10**-6;    #lamda(m)\n",
+    "h=6.625*10**-34;       #plancks constant(J s)\n",
+    "c=3*10**8;     #velocity of light(m/s)\n",
+    "\n",
+    "#Calculation\n",
+    "R=eta*q*lamda/(h*c);     #responsibility(A/W)\n",
+    "\n",
+    "#Result\n",
+    "print \"responsibility is\",round(R,3),\"A/W\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.5, Page number 10.61"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 36,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "multiplication factor is 41\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "eta=0.7;     #quantum efficiency\n",
+    "q=1.6*10**-19;    #charge(coulomb)\n",
+    "lamda=863*10**-9;    #lamda(m)\n",
+    "P0=0.5*10**-6;     #optical power(W)\n",
+    "h=6.625*10**-34;       #plancks constant(J s)\n",
+    "c=3*10**8;     #velocity of light(m/s)\n",
+    "IT=10*10**-6;    #current(A)\n",
+    "\n",
+    "#Calculation\n",
+    "IP=eta*q*lamda*P0/(h*c);\n",
+    "M=IT/IP;       #multiplication factor\n",
+    "\n",
+    "#Result\n",
+    "print \"multiplication factor is\",int(M)"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.6, Page number 10.62"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 37,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "critical angle is 78.5 degrees\n",
+      "numerical aperture is 0.3\n",
+      "acceptance angle is 17.4 degrees\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "n2=1.47;              #refractive index of cladding\n",
+    "n1=1.5;    #refractive index of core\n",
+    "\n",
+    "#Calculation\n",
+    "phi_c=math.asin(n2/n1);     #critical angle(radian)\n",
+    "phi_c=phi_c*180/math.pi;    #critical angle(degrees)\n",
+    "NA=math.sqrt(n1**2-n2**2);     #numerical aperture\n",
+    "phi_max=math.asin(NA);       #acceptance angle(radian)\n",
+    "phi_max=phi_max*180/math.pi;    #acceptance angle(degrees)\n",
+    "\n",
+    "#Result\n",
+    "print \"critical angle is\",round(phi_c,1),\"degrees\"\n",
+    "print \"numerical aperture is\",round(NA,1)\n",
+    "print \"acceptance angle is\",round(phi_max,1),\"degrees\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.7, Page number 10.62"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 38,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "total number of guided modes is 490.0\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "d=50*10**-6;     #diameter(m)\n",
+    "NA=0.2;      #numerical aperture(m)\n",
+    "lamda=1*10**-6;    #wavelength(m)\n",
+    "\n",
+    "#Calculation\n",
+    "N=4.9*(d*NA/lamda)**2;     #total number of guided modes\n",
+    "\n",
+    "#Result\n",
+    "print \"total number of guided modes is\",N"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.8, Page number 10.62"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 41,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "total number of guided modes is 1\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "d=5*10**-6;     #diameter(m)\n",
+    "n2=1.447;              #refractive index of cladding\n",
+    "n1=1.45;    #refractive index of core\n",
+    "lamda=1*10**-6;    #wavelength(m)\n",
+    "\n",
+    "#Calculation\n",
+    "NA=math.sqrt(n1**2-n2**2);      #numerical aperture\n",
+    "N=4.9*(d*NA/lamda)**2;     #total number of guided modes\n",
+    "\n",
+    "#Result\n",
+    "print \"total number of guided modes is\",int(N)"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.9, Page number 10.63"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 42,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "numerical aperture is 0.46\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "n1=1.46;    #refractive index of core\n",
+    "delta=0.05;    #refractive index difference\n",
+    "\n",
+    "#Calculation\n",
+    "NA=n1*math.sqrt(2*delta);     #numerical aperture\n",
+    "\n",
+    "#Result\n",
+    "print \"numerical aperture is\",round(NA,2)"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.10, Page number 10.63"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 44,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "V number is 94.72\n",
+      "maximum number of modes is 4486.0\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "a=50;\n",
+    "n2=1.5;              #refractive index of cladding\n",
+    "n1=1.53;    #refractive index of core\n",
+    "lamda0=1;    #wavelength(micro m)\n",
+    "\n",
+    "#Calculation\n",
+    "V_number=round(2*math.pi*a*math.sqrt(n1**2-n2**2)/lamda0,2);     #V number\n",
+    "n=V_number**2/2;     #maximum number of modes\n",
+    "\n",
+    "#Result\n",
+    "print \"V number is\",V_number\n",
+    "print \"maximum number of modes is\",round(n)"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.11, Page number 10.63"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 45,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "total number of modes is 49178.0\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "a=100*10**-6;\n",
+    "NA=0.3;      #numerical aperture(m)\n",
+    "lamda=850*10**-9;    #wavelength(m)\n",
+    "\n",
+    "#Calculation\n",
+    "V_number=round(2*math.pi**2*a**2*NA**2/lamda**2);     #number of modes\n",
+    "\n",
+    "#Result\n",
+    "print \"total number of modes is\",2*V_number"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.12, Page number 10.63"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 46,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "cutoff wavelength is 1.315 micro m\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "a=25*10**-6;\n",
+    "n1=1.48;    #refractive index of core\n",
+    "delta=0.01;    #refractive index difference\n",
+    "V=25;     #Vnumber\n",
+    "\n",
+    "#Calculation\n",
+    "lamda=2*math.pi*a*n1*math.sqrt(2*delta)/V;      #cutoff wavelength(m)\n",
+    "\n",
+    "#Result\n",
+    "print \"cutoff wavelength is\",round(lamda*10**6,3),\"micro m\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 10.13, Page number 10.63"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 48,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "maximum value of core radius is 9.95 micro m\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "V=2.405;     #Vnumber\n",
+    "lamda=1.3;    #wavelength(micro m)\n",
+    "NA=0.05;      #numerical aperture(m)\n",
+    "\n",
+    "#Calculation\n",
+    "amax=V*lamda/(2*math.pi*NA);     #maximum value of core radius(micro m)\n",
+    "\n",
+    "#Result\n",
+    "print \"maximum value of core radius is\",round(amax,2),\"micro m\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter12_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter12_1.ipynb
new file mode 100755
index 00000000..c8688bf4
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter12_1.ipynb
@@ -0,0 +1,454 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#12: Mechanical Behaviour of Materials"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.1, Page number 12.115"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 40,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "yield strength is 86.026 kg/mm**2\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "sigma0=8.55;\n",
+    "K=2.45;      \n",
+    "sigma=10**-3;      #steel size(mm)\n",
+    "\n",
+    "#Calculation\n",
+    "sigma=sigma0+(K/math.sqrt(sigma));      #yield strength\n",
+    "\n",
+    "#Result\n",
+    "print \"yield strength is\",round(sigma,3),\"kg/mm**2\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.2, Page number 12.115"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 41,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "fracture strength is 0.211 GPa\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "E=70*10**9;     #young's modulus(Pa)\n",
+    "gama=1;     #surface energy(joule/m**2)\n",
+    "C=1*10**-6;    #depth(m)\n",
+    "\n",
+    "#Calculation\n",
+    "sigma_f=math.sqrt(2*E*gama/(math.pi*C));      #fracture strength(GPa)\n",
+    "\n",
+    "#Result\n",
+    "print \"fracture strength is\",round(sigma_f/10**9,3),\"GPa\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.3, Page number 12.116"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 42,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "ultimate tensile strength is 736.0 MPa\n",
+      "ductility % of elongation is 10.0 %\n",
+      "ductility % of reduction is 75.0 %\n",
+      "modulus of toughness is 49 *10**6 Pa\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "ml=57800;     #load(N)\n",
+    "d=10*10**-3;    #diameter(m)\n",
+    "D=5;      #diameter after fracture(mm)\n",
+    "l=50;    #guage length(mm)\n",
+    "L=55;    #length after fracture(mm)\n",
+    "\n",
+    "#Calculation\n",
+    "ts=ml/(math.pi*(d/2)**2);    #ultimate tensile strength(MPa)\n",
+    "de=(L-l)*100/l;          #ductility % of elongation(%)\n",
+    "dr=((2*D)**2-D**2)*100/(2*D)**2;      #ductility % of reduction(%)\n",
+    "t=(2/3)*ts*de/100;        #modulus of toughness(Pa)\n",
+    "\n",
+    "#Result\n",
+    "print \"ultimate tensile strength is\",round(ts/10**6),\"MPa\"\n",
+    "print \"ductility % of elongation is\",de,\"%\"\n",
+    "print \"ductility % of reduction is\",dr,\"%\"\n",
+    "print \"modulus of toughness is\",int(t/10**6),\"*10**6 Pa\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.4, Page number 12.116"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 43,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "elastic strain in 1st case is 0.001\n",
+      "ratio of elastic and plastic strain in 2nd case is 2.5 %\n",
+      "ratio of elastic and plastic strain in 3rd case is 1.0 %\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "pl1=206850*10**3;     #proportional limit(Pa)\n",
+    "pl2=310275*10**3;     #proportional limit(Pa)\n",
+    "pl3=413700*10**3;     #proportional limit(Pa)\n",
+    "s2=0.0615;      #strain\n",
+    "s3=0.2020;      #strain\n",
+    "Y=2.0685*10**11;    #young's modulus(Pa)\n",
+    "\n",
+    "#Calculation\n",
+    "e1=pl1/Y;     #elastic strain in 1st case\n",
+    "e2=pl2/Y;     #elastic strain in 2nd case\n",
+    "p2=s2-e2;     #plastic strain in 2nd case\n",
+    "r2=e2*100/p2;   #ratio of elastic and plastic strain in 2nd case\n",
+    "e3=pl3/Y;     #elastic strain in 2nd case   \n",
+    "p3=s3-e3;     #plastic strain in 2nd case \n",
+    "r3=e3*100/p3;   #ratio of elastic and plastic strain in 3rd case\n",
+    "\n",
+    "#Result\n",
+    "print \"elastic strain in 1st case is\",e1\n",
+    "print \"ratio of elastic and plastic strain in 2nd case is\",r2,\"%\"\n",
+    "print \"ratio of elastic and plastic strain in 3rd case is\",r3,\"%\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.5, Page number 12.117"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 44,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "effective modulus is 738750.0 *10**3 Pa\n",
+      "cross sectional area is 1.0831 *10**-4 m**2\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "s=12411*10**3;      #stress(Pa)\n",
+    "t=0.0168;     #tension\n",
+    "e=0.127;     #elongation(cm)\n",
+    "l=15.24;     #length(cm)\n",
+    "g=9.8;\n",
+    "L=68.04;     #load(kg)\n",
+    "\n",
+    "#Calculation\n",
+    "E_eff=s/t;     #effective modulus(Pa)\n",
+    "S=e/l;      \n",
+    "W=E_eff*S;\n",
+    "A=L*g/W;       #cross sectional area(m**2)\n",
+    "\n",
+    "#Result\n",
+    "print \"effective modulus is\",E_eff/10**3,\"*10**3 Pa\"\n",
+    "print \"cross sectional area is\",round(A*10**4,4),\"*10**-4 m**2\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.6, Page number 12.117"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 45,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "transition temperature is 229.0 K\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "E=35*10**10;     #youngs modulus(Pa)\n",
+    "gama=2;     #specific surface energy(J/m**2)\n",
+    "C=2*10**-6;    #length(m)\n",
+    "x=17700;    \n",
+    "y=2.1;\n",
+    "z=31.25;\n",
+    "\n",
+    "#Calculation\n",
+    "sigma_f=math.sqrt(2*E*gama/(math.pi*C));     #fracture stress(Pa)\n",
+    "T=x/((sigma_f/(9.8*10**6))-y+z);    #transition temperature(K)\n",
+    "\n",
+    "#Result\n",
+    "print \"transition temperature is\",round(T),\"K\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.7, Page number 12.118"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 46,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "critical resolved shear stress is 0.898 MPa\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "h1=1;\n",
+    "h2=1;\n",
+    "k1=1;\n",
+    "k2=1;\n",
+    "l1=1;\n",
+    "l2=1;\n",
+    "l3=0;\n",
+    "s=3.5*10**6;      #stress(Pa)\n",
+    "\n",
+    "#Calculation\n",
+    "x=math.sqrt(h1**2+k1**2+l1**2);\n",
+    "y=math.sqrt(h2**2+k2**2+l2**2);\n",
+    "z=math.sqrt(h2**2+k2**2+l3**2);\n",
+    "cos_phi=((h1*h2)-(k1*k2)+(l1*l2))/(x*y);\n",
+    "sin_phi=math.sqrt(1-(cos_phi)**2);\n",
+    "cos_theta=((h1*h2)+(k1*k2)+(l1*l3))/(x*z);\n",
+    "ss=s*cos_theta*cos_phi*sin_phi;        #critical resolved shear stress(Pa)\n",
+    "\n",
+    "#Result\n",
+    "print \"critical resolved shear stress is\",round(ss/10**6,3),\"MPa\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.8, Page number 12.119"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 47,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "activation energy is 192.393 kJ/mol\n",
+      "answer varies due to rounding off errors\n",
+      "diffusion coefficient is 0.394 *10**-4 m**2/s\n",
+      "diffusivity at 300 C is 11.37 *10**-23 m**2/s\n",
+      "diffusivity at 700 C is 1.846 *10**-15 m**2/s\n",
+      "answer given in the book is wrong\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "dz1=4*10**-18;    #diffusivity(m**2/s)\n",
+    "dz2=5*10**-13;    #diffusivity(m**2/s)\n",
+    "T1=773;    #temperature(K)\n",
+    "T2=1273;   #temperature(K)\n",
+    "T3=573;   #temperature(K)\n",
+    "T4=973;   #temperature(K)\n",
+    "\n",
+    "#Calculation\n",
+    "x1=round(math.log(dz1),2);\n",
+    "y1=round(math.log(dz2),3);\n",
+    "x2=round(-1/(8.314*T1),7);\n",
+    "y2=round(-1/(8.314*T2),7);\n",
+    "x=round((x1-y1),3);\n",
+    "y=round((x2-y2),6);\n",
+    "Q=x/y;      #activation energy(J/mol)\n",
+    "z=round(y1-(y2*Q),4);\n",
+    "D0=math.exp(z);          #diffusion coefficient(m**2/Vs)\n",
+    "D1=D0*math.exp(-Q/(8.314*T3));    #diffusivity at 300 C(m**2/s)\n",
+    "D2=D0*math.exp(-Q/(8.314*T4));    #diffusivity at 700 C(m**2/s)\n",
+    "\n",
+    "#Result\n",
+    "print \"activation energy is\",round(Q/10**3,3),\"kJ/mol\"\n",
+    "print \"answer varies due to rounding off errors\"\n",
+    "print \"diffusion coefficient is\",round(D0*10**4,3),\"*10**-4 m**2/s\"\n",
+    "print \"diffusivity at 300 C is\",round(D1*10**23,2),\"*10**-23 m**2/s\"\n",
+    "print \"diffusivity at 700 C is\",round(D2*10**15,3),\"*10**-15 m**2/s\"\n",
+    "print \"answer given in the book is wrong\"\n"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 12.9, Page number 12.119"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 49,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "diffusion is 4.9 *10**-15 m**2/s\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "D0=0.73*10**-4;     #diffusion coefficient(m**2/s)\n",
+    "Q=170*10**3;     #activation energy(J/mol)\n",
+    "R=8.314; \n",
+    "T=873;    #temperature(K)\n",
+    "\n",
+    "#Calculation\n",
+    "D=D0*math.exp(-Q/(R*T));     #diffusion(m**2/s)\n",
+    "\n",
+    "#Result\n",
+    "print \"diffusion is\",round(D*10**15,1),\"*10**-15 m**2/s\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter1_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter1_1.ipynb
new file mode 100755
index 00000000..223b1028
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter1_1.ipynb
@@ -0,0 +1,97 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#1: Introduction"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 1.1, Page number 1.4"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 9,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "ratio of Al is 37.18 *10**3\n",
+      "ratio of Mg is 30.9 *10**3\n",
+      "ratio of steel is 17.69 *10**3\n",
+      "ratio of glass is 25.55 *10**3\n",
+      "Aluminium alloy is the best material\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "ws_al=103;     #working stress of Al\n",
+    "ws_mg=55;     #working stress of Mg\n",
+    "ws_st=138;     #working stress of steel\n",
+    "ws_g=35;     #working stress of glass\n",
+    "d_al=2770;   #density of Al\n",
+    "d_mg=1780;   #density of Mg\n",
+    "d_st=7800;   #density of steel\n",
+    "d_g=1370;   #density of glass\n",
+    "A=10**6;   #area\n",
+    "l=1;      #length\n",
+    "\n",
+    "#Calculation\n",
+    "L_al=ws_al*A;    #load of Al\n",
+    "L_mg=ws_mg*A;    #load of Mg\n",
+    "L_st=ws_st*A;    #load of steel\n",
+    "L_g=ws_g*A;    #load of glass\n",
+    "W_al=d_al*l;    #weight of Al\n",
+    "W_mg=d_mg*l;    #weight of Mg\n",
+    "W_st=d_st*l;    #weight of steel\n",
+    "W_g=d_g*l;    #weight of glass\n",
+    "r_al=L_al/W_al;     #ratio of Al\n",
+    "r_mg=L_mg/W_mg;     #ratio of Mg\n",
+    "r_st=L_st/W_st;     #ratio of steel\n",
+    "r_g=L_g/W_g;     #ratio of glass\n",
+    "\n",
+    "#Result\n",
+    "print \"ratio of Al is\",round(r_al/10**3,2),\"*10**3\"\n",
+    "print \"ratio of Mg is\",round(r_mg/10**3,2),\"*10**3\"\n",
+    "print \"ratio of steel is\",round(r_st/10**3,2),\"*10**3\"\n",
+    "print \"ratio of glass is\",round(r_g/10**3,2),\"*10**3\"\n",
+    "print \"Aluminium alloy is the best material\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter2_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter2_1.ipynb
new file mode 100755
index 00000000..b52f9be5
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter2_1.ipynb
@@ -0,0 +1,151 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#2: Chemical Bonds"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 2.1, Page number 2.21"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 5,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "-2*a/r**3 + 90*b/r**11\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "from sympy import Symbol\n",
+    "import numpy as np\n",
+    "\n",
+    "#Variable declaration\n",
+    "n=1;\n",
+    "m=9;\n",
+    "a=Symbol('a')\n",
+    "b=Symbol('b')\n",
+    "r=Symbol('r')\n",
+    "\n",
+    "#Calculation\n",
+    "y=(-a/(r**n))+(b/(r**m));\n",
+    "y=diff(y,r);\n",
+    "y=diff(y,r);\n",
+    "\n",
+    "#Result\n",
+    "print y"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 28,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "young's modulus is 157 GPa\n"
+     ]
+    }
+   ],
+   "source": [
+    "#since the values of a,b,r are declared as symbols in the above cell, it cannot be solved there. hence it is being solved here with the given variable declaration\n",
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "a=7.68*10**-29;     \n",
+    "r0=2.5*10**-10;    #radius(m)\n",
+    "\n",
+    "#Calculation\n",
+    "b=a*(r0**8)/9;\n",
+    "y=((-2*a*r0**8)+(90*b))/r0**11;    \n",
+    "E=y/r0;           #young's modulus(Pa)\n",
+    "\n",
+    "#Result\n",
+    "print \"young's modulus is\",int(E/10**9),\"GPa\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 2.2, Page number 2.22"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 31,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "effective charge is 0.72 *10**-19 coulomb\n",
+      "answer given in the book is wrong\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "dm=1.98*(10**-29)*(1/3);      #dipole moment\n",
+    "l=0.92*10**-10;        #bond length(m)\n",
+    "\n",
+    "#Calculation\n",
+    "ec=dm/l;        #effective charge(coulomb)\n",
+    "\n",
+    "#Result\n",
+    "print \"effective charge is\",round(ec*10**19,2),\"*10**-19 coulomb\"\n",
+    "print \"answer given in the book is wrong\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter3_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter3_1.ipynb
new file mode 100755
index 00000000..f6d276be
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter3_1.ipynb
@@ -0,0 +1,503 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#3: Elementary Crystallography"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 3.2, Page number 3.50"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 23,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "spacing between (100) plane is 5.64 angstrom\n",
+      "spacing between (110) plane is 3.99 angstrom\n",
+      "spacing between (111) plane is 3.26 angstrom\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "a=5.64;      #lattice constant(angstrom)\n",
+    "h1=1;\n",
+    "k1=0;\n",
+    "l1=0;\n",
+    "h2=1;\n",
+    "k2=1;\n",
+    "l2=0;\n",
+    "h3=1;\n",
+    "k3=1;\n",
+    "l3=1;\n",
+    "\n",
+    "#Calculation\n",
+    "d100=a/math.sqrt(h1**2+k1**2+l1**2);     #spacing between (100) plane\n",
+    "d110=a/math.sqrt(h2**2+k2**2+l2**2);     #spacing between (110) plane\n",
+    "d111=a/math.sqrt(h3**2+k3**2+l3**2);     #spacing between (111) plane\n",
+    "\n",
+    "#Result\n",
+    "print \"spacing between (100) plane is\",d100,\"angstrom\"\n",
+    "print \"spacing between (110) plane is\",round(d110,2),\"angstrom\"\n",
+    "print \"spacing between (111) plane is\",round(d111,2),\"angstrom\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 3.3, Page number 3.51"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 25,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "number of atoms in (100) is 1.535 *10**13 atoms/mm**2\n",
+      "number of atoms in (110) is 1.085 *10**13 atoms/mm**2\n",
+      "number of atoms in (111) is 1.772 *10**13 atoms/mm**2\n",
+      "answer varies due to rounding off errors\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "a=3.61*10**-7;        #lattice constant(mm)\n",
+    "\n",
+    "#Calculation\n",
+    "A100=a**2;     #surface area(mm**2)\n",
+    "n=1+(4*(1/4));\n",
+    "N1=n/A100;      #number of atoms in (100)(per mm**2)\n",
+    "A110=math.sqrt(2)*a**2;      #surface area(mm**2)\n",
+    "N2=n/A110;      #number of atoms in (110)(per mm**2)\n",
+    "A111=math.sqrt(3)*a**2/2;    #surface area(mm**2)\n",
+    "N3=n/A111;     #number of atoms in (110)(per mm**2)\n",
+    "\n",
+    "#Result\n",
+    "print \"number of atoms in (100) is\",round(N1/10**13,3),\"*10**13 atoms/mm**2\"\n",
+    "print \"number of atoms in (110) is\",round(N2/10**13,3),\"*10**13 atoms/mm**2\"\n",
+    "print \"number of atoms in (111) is\",round(N3/10**13,3),\"*10**13 atoms/mm**2\"\n",
+    "print \"answer varies due to rounding off errors\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {
+    "collapsed": true
+   },
+   "source": [
+    "##Example number 3.4, Page number 3.52"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 27,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "wavelength of x rays is 1.552 angstrom\n",
+      "answer varies due to rounding off errors\n",
+      "energy of x rays is 8 *10**3 eV\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "n=4;      \n",
+    "A=107.87;    #atomic weight\n",
+    "rho=10500;     #density(kg/m**3)\n",
+    "N=6.02*10**26;    #number of molecules\n",
+    "theta=19+(12/60);   #angle(degrees)\n",
+    "h=1;\n",
+    "k=1;\n",
+    "l=1;\n",
+    "h0=6.625*10**-34;     #planck constant\n",
+    "c=3*10**8;     #velocity of light(m/s)\n",
+    "e=1.6*10**-19;   #charge(coulomb)\n",
+    "\n",
+    "#Calculation\n",
+    "theta=theta*math.pi/180;     #angle(radian)\n",
+    "a=(n*A/(N*rho))**(1/3);\n",
+    "d=a*10**10/math.sqrt(h**2+k**2+l**2);      \n",
+    "lamda=2*d*math.sin(theta);     #wavelength of x rays(angstrom)\n",
+    "E=h0*c/(lamda*10**-10*e);      #energy of x rays(eV)\n",
+    "\n",
+    "#Result\n",
+    "print \"wavelength of x rays is\",round(lamda,3),\"angstrom\"\n",
+    "print \"answer varies due to rounding off errors\"\n",
+    "print \"energy of x rays is\",int(E/10**3),\"*10**3 eV\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 3.5, Page number 3.52"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 28,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "density is 2332 kg/m**3\n",
+      "answer varies due to rounding off errors\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "n=8;    #number of atoms\n",
+    "r=2.351*10**-10;     #bond length(angstrom)\n",
+    "A=28.09;                #Atomic wt. of NaCl\n",
+    "N=6.02*10**26           #Avagadro number\n",
+    "\n",
+    "#Calculation\n",
+    "a=4*r/math.sqrt(3);     \n",
+    "rho=n*A/(N*a**3);     #density(kg/m**3)\n",
+    "\n",
+    "#Result\n",
+    "print \"density is\",int(rho),\"kg/m**3\"\n",
+    "print \"answer varies due to rounding off errors\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {
+    "collapsed": true
+   },
+   "source": [
+    "##Example number 3.6, Page number 3.53"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 29,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "radius of largest sphere is 0.1547 r\n",
+      "maximum radius of sphere is 0.414 r\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "from sympy import Symbol\n",
+    "\n",
+    "#Variable declaration\n",
+    "r=Symbol('r')\n",
+    "\n",
+    "#Calculation\n",
+    "a1=4*r/math.sqrt(3);\n",
+    "R1=(a1/2)-r;           #radius of largest sphere\n",
+    "a2=4*r/math.sqrt(2);\n",
+    "R2=(a2/2)-r;       #maximum radius of sphere\n",
+    "\n",
+    "#Result\n",
+    "print \"radius of largest sphere is\",round(R1/r,4),\"r\"\n",
+    "print \"maximum radius of sphere is\",round(R2/r,3),\"r\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 3.7, Page number 3.54"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 30,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "percent volume change is 0.5 %\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "r1=1.258*10**-10;     #radius(m)\n",
+    "r2=1.292*10**-10;     #radius(m)\n",
+    "\n",
+    "#Calculation\n",
+    "a_bcc=4*r1/math.sqrt(3);\n",
+    "v=a_bcc**3;\n",
+    "V1=v/2;\n",
+    "a_fcc=2*math.sqrt(2)*r2;\n",
+    "V2=a_fcc**3/4;\n",
+    "V=(V1-V2)*100/V1;           #percent volume change is\",V,\"%\"\n",
+    "\n",
+    "#Result\n",
+    "print \"percent volume change is\",round(V,1),\"%\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 3.8, Page number 3.55"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 31,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "number of vacancies at 0K is 0 per mol\n",
+      "number of vacancies at 300K is 768.0 per mol\n",
+      "number of vacancies at 900K is 6.53 *10**16 per mol\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "delta_Hf=120*10**3;      \n",
+    "T1=0;    #temperature(K)\n",
+    "T2=300;    #temperature(K)\n",
+    "n1=0;\n",
+    "N=6.022*10**23;\n",
+    "R=8.314;\n",
+    "T3=900;    #temperature(K)\n",
+    "\n",
+    "#Calculation\n",
+    "n2=N*math.exp(-delta_Hf/(R*T2));     #number of vacancies at 300K(per mol)\n",
+    "n3=N*math.exp(-delta_Hf/(R*T3));     #number of vacancies at 900K(per mol)\n",
+    "\n",
+    "#Result\n",
+    "print \"number of vacancies at 0K is\",n1,\"per mol\"\n",
+    "print \"number of vacancies at 300K is\",round(n2),\"per mol\"\n",
+    "print \"number of vacancies at 900K is\",round(n3/10**16,2),\"*10**16 per mol\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 3.9, Page number 3.56"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 34,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "interplanar spacing of crystal is  1.824 angstrom\n",
+      "answer varies due to rounding off errors\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "theta1=6.45;      #angle(degrees)\n",
+    "theta2=9.15;      #angle(degrees)\n",
+    "theta3=13;      #angle(degrees)\n",
+    "lamda=0.58;     #wavelength(angstrom)\n",
+    "\n",
+    "#Calculation\n",
+    "theta1=theta1*math.pi/180;     #angle(radian)\n",
+    "theta2=theta2*math.pi/180;     #angle(radian)\n",
+    "theta3=theta3*math.pi/180;     #angle(radian)\n",
+    "d=lamda/(2*math.sin(theta2));    #interplanar spacing of crystal(angstrom)\n",
+    "\n",
+    "#Result\n",
+    "print \"interplanar spacing of crystal is \",round(d,3),\"angstrom\"\n",
+    "print \"answer varies due to rounding off errors\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 3.10, Page number 3.56"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 35,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "lattice parameter of lead is 4.1 *10**-10 m\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "n=1;     #order of diffraction\n",
+    "lamda=1.54*10**-10;     #wavelength(m)\n",
+    "theta=32;      #angle(degrees)\n",
+    "h=2;\n",
+    "k=2;\n",
+    "l=0;\n",
+    "\n",
+    "#Calculation\n",
+    "theta=theta*math.pi/180;     #angle(radian)\n",
+    "d=n*lamda/(2*math.sin(theta));\n",
+    "a=d*math.sqrt(h**2+k**2+l**2);    #lattice parameter of lead(m)\n",
+    "\n",
+    "#Result\n",
+    "print \"lattice parameter of lead is\",round(a*10**10,1),\"*10**-10 m\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 3.11, Page number 3.57"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 37,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "amount of climb down is 0.36915 *10**-8 cm\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "delta_Hf=1.6*10**-19;      \n",
+    "T=500;    #temperature(K)\n",
+    "N=6.026*10**23;\n",
+    "k=1.38*10**-23;    #boltzmann constant\n",
+    "mv=5.55;    #molar volume(cm**3)\n",
+    "ne=10**6;    #number of edge dislocations(per cm**3)\n",
+    "v=5*10**7;    #number of vacancies\n",
+    "a=2*10**-8;   #lattice parameter(cm)\n",
+    "\n",
+    "#Calculation\n",
+    "n=(N/mv)*math.exp(-delta_Hf/(k*T));     #number of vacancies at 300K(per mol)\n",
+    "ac=n*a/(v*ne);      #amount of climb down(cm)\n",
+    "\n",
+    "#Result\n",
+    "print \"amount of climb down is\",round(ac*10**8,5),\"*10**-8 cm\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter4_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter4_1.ipynb
new file mode 100755
index 00000000..8da77cca
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter4_1.ipynb
@@ -0,0 +1,370 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#4: Electron Theory of Solids"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 4.1, Page number 4.57"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 10,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "de broglie wavelength is 0.00286 angstrom\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "E=10**4*1.6*10**-19;      #kinetic energy(J)\n",
+    "m=1.675*10**-27;     #mass(kg)\n",
+    "h=6.625*10**-34;     #planck's constant\n",
+    "\n",
+    "#Calculation\n",
+    "v=math.sqrt(2*E/m);     #velocity(m/s)\n",
+    "lamda=h/(m*v);          #de broglie wavelength(m)\n",
+    "\n",
+    "#Result\n",
+    "print \"de broglie wavelength is\",round(lamda*10**10,5),\"angstrom\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 4.2, Page number 4.58"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 11,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "energy difference is 1.81 *10**-37 J\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "m=9.1*10**-31;     #mass(kg)\n",
+    "nx=ny=nz=1;\n",
+    "n=6;\n",
+    "a=1;     #edge(m)\n",
+    "h=6.63*10**-34;     #planck's constant\n",
+    "\n",
+    "#Calculation\n",
+    "E1=h**2*(nx**2+ny**2+nz**2)/(8*m*a**2);\n",
+    "E2=h**2*n/(8*m*a**2);\n",
+    "E=E2-E1;               #energy difference(J)\n",
+    "\n",
+    "#Result\n",
+    "print \"energy difference is\",round(E*10**37,2),\"*10**-37 J\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 4.3, Page number 4.58"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 15,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "temperature is 1261 K\n",
+      "answer varies due to rounding off errors\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "y=1/100;    #percentage of probability\n",
+    "x=0.5*1.6*10**-19;     #energy(J)\n",
+    "k=1.38*10**-23;       #boltzmann constant\n",
+    "\n",
+    "#Calculation\n",
+    "xbykT=math.log((1/y)-1);\n",
+    "T=x/(k*xbykT);       #temperature(K)\n",
+    "\n",
+    "#Result\n",
+    "print \"temperature is\",int(T),\"K\"\n",
+    "print \"answer varies due to rounding off errors\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 4.4, Page number 4.58"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 16,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "fermi energy is 3.15 eV\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "d=970;    #density(kg/m**3)\n",
+    "Na=6.02*10**26;    #avagadro number\n",
+    "w=23;    #atomic weight\n",
+    "m=9.1*10**-31;     #mass(kg)\n",
+    "h=6.62*10**-34;     #planck's constant\n",
+    "\n",
+    "#Calculation\n",
+    "N=d*Na/w;    #number of atoms/m**3\n",
+    "x=h**2/(8*m);\n",
+    "y=(3*N/math.pi)**(2/3);\n",
+    "EF=x*y;     #fermi energy(J)\n",
+    "\n",
+    "#Result\n",
+    "print \"fermi energy is\",round(EF/(1.6*10**-19),2),\"eV\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 4.5, Page number 4.59"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 18,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "work function is 4.14 eV\n",
+      "maximum kinetic energy is 0.758 eV\n",
+      "answer varies due to rounding off errors\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "h=6.625*10**-34;     #planck's constant\n",
+    "c=3*10**8;     #velocity of light(m/s)\n",
+    "lamda0=3000*10**-10;   #wavelength(m)\n",
+    "e=1.6*10**-19;    #charge(coulomb)\n",
+    "lamda=2536*10**-10;      #wavelength(m)\n",
+    "\n",
+    "#Calculation\n",
+    "hf0=c*h/(lamda0*e);    #work function(eV)\n",
+    "E=c*h*((1/lamda)-(1/lamda0))/e;            #maximum kinetic energy(eV)\n",
+    "\n",
+    "#Result\n",
+    "print \"work function is\",round(hf0,2),\"eV\"\n",
+    "print \"maximum kinetic energy is\",round(E,3),\"eV\"\n",
+    "print \"answer varies due to rounding off errors\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 4.6, Page number 4.59"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 19,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "lowest energy of neutron is 2.05 MeV\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "n=1;\n",
+    "hbar=1.054*10**-34;    \n",
+    "m=1.67*10**-27;    #mass of neutron(kg)\n",
+    "a=10**-14;      #size(m)\n",
+    "\n",
+    "#Calculation\n",
+    "E=n**2*math.pi**2*hbar**2/(2*m*a**2);     #lowest energy of neutron(J)\n",
+    "\n",
+    "#Result\n",
+    "print \"lowest energy of neutron is\",round(E/(1.6*10**-13),2),\"MeV\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 4.7, Page number 4.59"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 20,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "probability of particle is 0.0158\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "from scipy.integrate import quad\n",
+    "\n",
+    "#Variable declaration\n",
+    "k=1;\n",
+    "\n",
+    "#Calculation\n",
+    "def zintg(x):\n",
+    "\treturn math.exp(-2*k*x)\n",
+    "\n",
+    "a=quad(zintg,2/k,3/k)[0];        #probability of particle\n",
+    "\n",
+    "#Result\n",
+    "print \"probability of particle is\",round(2*a,4)"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 4.8, Page number 4.60"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 22,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "voltage appeared is 1.83 mV\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "i=10**-2;    #current(ampere)\n",
+    "A=0.01*0.001;     #area(m**2)\n",
+    "RH=3.66*10**-4;   #hall coefficient(m**3/coulomb)\n",
+    "Bz=0.5;     #magnetic induction(weber/m**2)\n",
+    "\n",
+    "#Calculation\n",
+    "Jx=i/A;     \n",
+    "Ey=RH*Bz*Jx;    \n",
+    "Vy=Ey*i;      #voltage appeared(V)\n",
+    "\n",
+    "#Result\n",
+    "print \"voltage appeared is\",Vy*10**3,\"mV\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter5_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter5_1.ipynb
new file mode 100755
index 00000000..2e530c83
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter5_1.ipynb
@@ -0,0 +1,303 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#5: Conducting Materials"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 5.1, Page number 5.34"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 1,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "drift speed is 36.6 *10**-5 m/s\n",
+      "mean free path is 3.34 *10**-8 m\n",
+      "answer given in the book is wrong\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "Na=6.023*10**26;    #avagadro number\n",
+    "e=1.602*10**-19;\n",
+    "d=8960;     #density\n",
+    "N=1;       #number of free electrons\n",
+    "w=63.54;    #atomic weight\n",
+    "i=10;      #current(ampere)\n",
+    "m=9.1*10**-31;    \n",
+    "rho=2*10**-8;   #resistivity(ohm m)\n",
+    "r=0.08*10**-2;    #radius(m)\n",
+    "c=1.6*10**6;   #mean thermal velocity(m/s)\n",
+    "\n",
+    "#Calculation\n",
+    "A=math.pi*r**2;    #area(m**2)\n",
+    "n=Na*d*N/w;\n",
+    "vd=i/(A*n*e);     #drift speed(m/s)\n",
+    "tow_c=m/(n*e**2*rho);\n",
+    "lamda=tow_c*c;      #mean free path(m)\n",
+    "\n",
+    "#Result\n",
+    "print \"drift speed is\",round(vd*10**5,1),\"*10**-5 m/s\"\n",
+    "print \"mean free path is\",round(lamda*10**8,2),\"*10**-8 m\"\n",
+    "print \"answer given in the book is wrong\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 5.2, Page number 5.35"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 3,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "electrical conductivity is 4.8 *10**7 ohm-1 m-1\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "e=1.602*10**-19;\n",
+    "m=9.1*10**-31;  #mass(kg)\n",
+    "tow=2*10**-14;    #time(s)\n",
+    "n=8.5*10**28;    \n",
+    "\n",
+    "#Calculation\n",
+    "sigma=n*e**2*tow/m;    #electrical conductivity(ohm-1 m-1)\n",
+    "\n",
+    "#Result\n",
+    "print \"electrical conductivity is\",round(sigma/10**7,1),\"*10**7 ohm-1 m-1\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 5.3, Page number 5.35"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 4,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "relaxation time is 4.0 *10**-14 s\n",
+      "mobility of electrons is 7.0 *10**-3 m**2/Vs\n",
+      "drift velocity is 0.7 m/s\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "e=1.6*10**-19;\n",
+    "m=9.1*10**-31;  #mass(kg)\n",
+    "n=5.8*10**28;  \n",
+    "rho=1.54*10**-8;    #resistivity(ohm m)\n",
+    "E=1*10**2;\n",
+    "\n",
+    "#Calculation\n",
+    "tow=m/(rho*n*e**2);      #relaxation time(s)\n",
+    "mew_e=1/(rho*e*n);       #mobility of electrons(m**2/Vs)\n",
+    "vd=mew_e*E;       #drift velocity(m/s)\n",
+    "\n",
+    "#Result\n",
+    "print \"relaxation time is\",round(tow*10**14),\"*10**-14 s\"\n",
+    "print \"mobility of electrons is\",round(mew_e*10**3),\"*10**-3 m**2/Vs\"\n",
+    "print \"drift velocity is\",round(vd,1),\"m/s\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 5.4, Page number 5.35"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 5,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "resistivity is 5.51 *10**-8 ohm m\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "rho=1.7*10**-8;    #resistivity(ohm m)\n",
+    "T=300;     #temperature(K)\n",
+    "T1=973;    #temperature(K)\n",
+    "\n",
+    "#Calculation\n",
+    "a=rho/T;    \n",
+    "rho_973=a*T1;    #resistivity(ohm m)\n",
+    "\n",
+    "#Result\n",
+    "print \"resistivity is\",round(rho_973*10**8,2),\"*10**-8 ohm m\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 5.5, Page number 5.36"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 8,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "increase of resistivity is 0.54 *10**-8 ohm m\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "rho1=1.2*10**-8;    #resistivity(ohm m)\n",
+    "rho2=0.12*10**-8;    #resistivity(ohm m)\n",
+    "p1=0.4;    #atomic percent\n",
+    "p2=0.5;    #atomic percent\n",
+    "rho=1.5*10**-8;    #resistivity(ohm m)\n",
+    "\n",
+    "#Calculation\n",
+    "rho_i=(rho1*p1)+(rho2*p2);     #increase of resistivity(ohm m)\n",
+    "Tr=rho+rho_i;       #total resistivity of copper alloy(ohm m)\n",
+    "\n",
+    "#Result\n",
+    "print \"increase of resistivity is\",round(rho_i*10**8,2),\"*10**-8 ohm m\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 5.6, Page number 5.36"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 16,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "electrical conductivity is 1.688 *10**7 ohm-1 m-1\n",
+      "thermal conductivity is 123.93 W/m/K\n",
+      "lorentz number is 2.447 *10**-8 watt ohm K-2\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "e=1.6*10**-19;\n",
+    "m=9.1*10**-31;  #mass(kg)\n",
+    "n=6*10**28;     #density(per m**3)\n",
+    "tow=10**-14;    #relaxation time(s)\n",
+    "T=300;    #temperature(K)\n",
+    "k=1.38*10**-23;   #boltzmann constant\n",
+    "\n",
+    "#Calculation\n",
+    "sigma=n*e**2*tow/m;    #electrical conductivity(ohm-1 m-1)\n",
+    "K=n*math.pi**2*k**2*T*tow/(3*m);    #thermal conductivity(W/m/K)\n",
+    "L=K/(sigma*T);    #lorentz number(watt ohm K-2)\n",
+    "\n",
+    "#Result\n",
+    "print \"electrical conductivity is\",round(sigma/10**7,3),\"*10**7 ohm-1 m-1\"\n",
+    "print \"thermal conductivity is\",round(K,2),\"W/m/K\"\n",
+    "print \"lorentz number is\",round(L*10**8,3),\"*10**-8 watt ohm K-2\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter6_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter6_1.ipynb
new file mode 100755
index 00000000..8da69c01
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter6_1.ipynb
@@ -0,0 +1,308 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#6: Dielectric Materials"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 6.1, Page number 6.34"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 40,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "insulation resistance is 0.85 *10**18 ohm\n",
+      "answer varies due to rounding off errors\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "rho=5*10**16;   #resistivity(ohm m)\n",
+    "l=5*10**-2;    #thickness(m)\n",
+    "b=8*10**-2;    #length(m)\n",
+    "w=3*10**-2;    #width(m)\n",
+    "\n",
+    "#Calculation\n",
+    "A=b*w;    #area(m**2)\n",
+    "Rv=rho*l/A;    \n",
+    "X=l+b;      #length(m)\n",
+    "Y=w;      #perpendicular(m)\n",
+    "Rs=Rv*X/Y;    \n",
+    "Ri=Rs*Rv/(Rs+Rv);       #insulation resistance(ohm)\n",
+    "\n",
+    "#Result\n",
+    "print \"insulation resistance is\",round(Ri/10**18,2),\"*10**18 ohm\"\n",
+    "print \"answer varies due to rounding off errors\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 6.2, Page number 6.34"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 41,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "DC dielectric loss is 1 *10**-3 watt\n",
+      "AC dielectric loss is 22.22 *10**-3 watt\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "rho=10**10;   #resistivity(ohm m)\n",
+    "d=10**-3;    #thickness(m)\n",
+    "A=10**4*10**-6;    #area(m**2)\n",
+    "V=10**3;    #voltage(V)\n",
+    "f=50;     #power frequency(Hz)\n",
+    "epsilonr=8;\n",
+    "epsilon0=8.84*10**-12;\n",
+    "tan_delta=0.1;\n",
+    "\n",
+    "#Calculation\n",
+    "Rv=rho*d/A; \n",
+    "dl_DC=V**2/Rv;      #DC dielectric loss(watt)\n",
+    "C=A*epsilon0*epsilonr/d;\n",
+    "dl_AC=V**2*2*math.pi*f*C*tan_delta;     #AC dielectric loss(watt)\n",
+    "\n",
+    "#Result\n",
+    "print \"DC dielectric loss is\",int(dl_DC*10**3),\"*10**-3 watt\"\n",
+    "print \"AC dielectric loss is\",round(dl_AC*10**3,2),\"*10**-3 watt\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 6.3, Page number 6.35"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 42,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "polarisability of He is 0.185 *10**-40 farad m**2\n",
+      "relative permittivity is 1.000056\n",
+      "answer varies due to rounding off errors\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "epsilon0=8.84*10**-12;\n",
+    "R=0.55*10**-10;    #radius(m)\n",
+    "N=2.7*10**25;      #number of atoms\n",
+    "\n",
+    "#Calculation\n",
+    "alpha_e=4*math.pi*epsilon0*R**3;    #polarisability of He(farad m**2)\n",
+    "epsilonr=1+(N*alpha_e/epsilon0);      #relative permittivity\n",
+    "\n",
+    "#Result\n",
+    "print \"polarisability of He is\",round(alpha_e*10**40,3),\"*10**-40 farad m**2\"\n",
+    "print \"relative permittivity is\",round(epsilonr,6)\n",
+    "print \"answer varies due to rounding off errors\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 6.4, Page number 6.35"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 43,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "field strength is 3.535 *10**7 V/m\n",
+      "total dipole moment is 33.4 *10**-12 Cm\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "A=360*10**-4;    #area(m**2)\n",
+    "V=15;    #voltage(V)\n",
+    "C=6*10**-6;     #capacitance(farad)\n",
+    "epsilonr=8;\n",
+    "epsilon0=8.84*10**-12;\n",
+    "\n",
+    "#Calculation\n",
+    "E=V*C/(epsilon0*epsilonr*A);     #field strength(V/m)\n",
+    "dm=epsilon0*(epsilonr-1)*V*A;    #total dipole moment(Cm)\n",
+    "\n",
+    "#Result\n",
+    "print \"field strength is\",round(E/10**7,3),\"*10**7 V/m\"\n",
+    "print \"total dipole moment is\",round(dm*10**12,1),\"*10**-12 Cm\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 6.5, Page number 6.36"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 44,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "capacitance is 226.3 *10**-12 farad\n",
+      "parallel loss resistance is 10 mega ohm\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "d=0.08*10**-3;    #thickness(m)\n",
+    "A=8*10**-4;    #area(m**2)\n",
+    "epsilonr=2.56;\n",
+    "epsilon0=8.84*10**-12;\n",
+    "tan_delta=0.7*10**-4;\n",
+    "new=10**6;    #frequency(Hz)\n",
+    "\n",
+    "#Calculation\n",
+    "C=A*epsilon0*epsilonr/d;     #capacitance(farad)\n",
+    "epsilonrdash=tan_delta*epsilonr;\n",
+    "omega=2*math.pi*new;\n",
+    "R=d/(epsilon0*epsilonrdash*omega*A);     #parallel loss resistance(ohm)\n",
+    "\n",
+    "#Result\n",
+    "print \"capacitance is\",round(C*10**12,1),\"*10**-12 farad\"\n",
+    "print \"parallel loss resistance is\",int(R/10**6),\"mega ohm\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 6.6, Page number 6.36"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 45,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "the complex polarizability is (3.50379335033-0.0600074383321j) *10**-40 F-m**2\n",
+      "answer cant be rouned off to 2 decimals as given in the textbook. Since it is a complex number and complex cant be converted to float\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "epsilonr=4.36;      #dielectric constant\n",
+    "t=2.8*10**-2;       #loss tangent(t)\n",
+    "N=4*10**28;         #number of electrons\n",
+    "epsilon0=8.84*10**-12;      \n",
+    "\n",
+    "#Calculation\n",
+    "epsilon_r = epsilonr*t;\n",
+    "epsilonstar = (complex(epsilonr,-epsilon_r));\n",
+    "alphastar = (epsilonstar-1)/(epsilonstar+2);\n",
+    "alpha_star = 3*epsilon0*alphastar/N;             #complex polarizability(Fm**2)\n",
+    "\n",
+    "#Result\n",
+    "print \"the complex polarizability is\",alpha_star*10**40,\"*10**-40 F-m**2\"\n",
+    "print \"answer cant be rouned off to 2 decimals as given in the textbook. Since it is a complex number and complex cant be converted to float\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter7_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter7_1.ipynb
new file mode 100755
index 00000000..df8d9205
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter7_1.ipynb
@@ -0,0 +1,288 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#7: Magnetic Materials"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 7.1, Page number 7.36"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 7,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "temperature rise is 8.43 K\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "El=10**-2*50;       #energy loss(J)\n",
+    "H=El*60;      #heat produced(J)\n",
+    "d=7.7*10**3;    #iron rod(kg/m**3)\n",
+    "s=0.462*10**-3;    #specific heat(J/kg K)\n",
+    "\n",
+    "#Calculation\n",
+    "theta=H/(d*s);     #temperature rise(K)\n",
+    "\n",
+    "#Result\n",
+    "print \"temperature rise is\",round(theta,2),\"K\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 7.2, Page number 7.36"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 8,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "magnetic field at the centre is 14.0 weber/m**2\n",
+      "dipole moment is 9.0 *10**-24 ampere/m**2\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "e=1.6*10**-19;    #charge(coulomb)\n",
+    "new=6.8*10**15;   #frequency(revolutions per second)\n",
+    "mew0=4*math.pi*10**-7;\n",
+    "R=5.1*10**-11;     #radius(m)\n",
+    "\n",
+    "#Calculation\n",
+    "i=round(e*new,4);          #current(ampere)\n",
+    "B=mew0*i/(2*R);    #magnetic field at the centre(weber/m**2)\n",
+    "A=math.pi*R**2;\n",
+    "d=i*A;       #dipole moment(ampere/m**2)\n",
+    "\n",
+    "#Result\n",
+    "print \"magnetic field at the centre is\",round(B),\"weber/m**2\"\n",
+    "print \"dipole moment is\",round(d*10**24),\"*10**-24 ampere/m**2\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 7.3, Page number 7.36"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 9,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "intensity of magnetisation is 5.0 ampere/m\n",
+      "flux density in material is 1.257 weber/m**2\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "chi=0.5*10**-5;    #magnetic susceptibility\n",
+    "H=10**6;     #field strength(ampere/m)\n",
+    "mew0=4*math.pi*10**-7;\n",
+    "\n",
+    "#Calculation\n",
+    "I=chi*H;     #intensity of magnetisation(ampere/m)\n",
+    "B=mew0*(I+H);    #flux density in material(weber/m**2)\n",
+    "\n",
+    "#Result\n",
+    "print \"intensity of magnetisation is\",I,\"ampere/m\"\n",
+    "print \"flux density in material is\",round(B,3),\"weber/m**2\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 7.4, Page number 7.36"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 10,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "number of Bohr magnetons is 2.22 bohr magneon/atom\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "B=9.27*10**-24;      #bohr magneton(ampere m**2)\n",
+    "a=2.86*10**-10;      #edge(m)\n",
+    "Is=1.76*10**6;       #saturation value of magnetisation(ampere/m)\n",
+    "\n",
+    "#Calculation\n",
+    "N=2/a**3;\n",
+    "mew_bar=Is/N;      #number of Bohr magnetons(ampere m**2)\n",
+    "mew_bar=mew_bar/B;      #number of Bohr magnetons(bohr magneon/atom)\n",
+    "\n",
+    "#Result\n",
+    "print \"number of Bohr magnetons is\",round(mew_bar,2),\"bohr magneon/atom\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 7.5, Page number 7.37"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 11,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "average magnetic moment is 2.79 *10**-3 bohr magneton/spin\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "mew0=4*math.pi*10**-7;\n",
+    "H=9.27*10**-24;      #bohr magneton(ampere m**2)\n",
+    "beta=10**6;      #field(ampere/m)\n",
+    "k=1.38*10**-23;    #boltzmann constant\n",
+    "T=303;    #temperature(K)\n",
+    "\n",
+    "#Calculation\n",
+    "mm=mew0*H*beta/(k*T);    #average magnetic moment(bohr magneton/spin)\n",
+    "\n",
+    "#Result\n",
+    "print \"average magnetic moment is\",round(mm*10**3,2),\"*10**-3 bohr magneton/spin\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 7.6, Page number 7.37"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 13,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "hysteresis loss per cycle is 188.0 J/m**3\n",
+      "hysteresis loss per second is 9400.0 watt/m**3\n",
+      "power loss is 1.23 watt/kg\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "A=94;      #area(m**2)\n",
+    "vy=0.1;    #value of length(weber/m**2)\n",
+    "vx=20;     #value of unit length\n",
+    "n=50;      #number of magnetization cycles\n",
+    "d=7650;    #density(kg/m**3)\n",
+    "\n",
+    "#Calculation\n",
+    "h=A*vy*vx;     #hysteresis loss per cycle(J/m**3)\n",
+    "hs=h*n;       #hysteresis loss per second(watt/m**3)\n",
+    "pl=hs/d;      #power loss(watt/kg)\n",
+    "\n",
+    "#Result\n",
+    "print \"hysteresis loss per cycle is\",h,\"J/m**3\"\n",
+    "print \"hysteresis loss per second is\",hs,\"watt/m**3\"\n",
+    "print \"power loss is\",round(pl,2),\"watt/kg\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter8_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter8_1.ipynb
new file mode 100755
index 00000000..5b490a55
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter8_1.ipynb
@@ -0,0 +1,71 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#8: Superconducting Materials"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 8.2, Page number 8.16"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 3,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "critical field is 33.64 *10**3 ampere/m\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "H0=64*10**3;    #initial field(ampere/m)\n",
+    "T=5;    #temperature(K)\n",
+    "Tc=7.26;   #transition temperature(K)\n",
+    "\n",
+    "#Calculation\n",
+    "H=H0*(1-(T/Tc)**2);     #critical field(ampere/m)\n",
+    "\n",
+    "#Result\n",
+    "print \"critical field is\",round(H/10**3,2),\"*10**3 ampere/m\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/Chapter9_1.ipynb b/Materials_Science_by_Dr._M._Arumugam/Chapter9_1.ipynb
new file mode 100755
index 00000000..2a72be5d
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/Chapter9_1.ipynb
@@ -0,0 +1,276 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "#9: Semiconducting Materials"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 9.1, Page number 9.23"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 39,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "number of electron hole pairs is 2.32 *10**16 per cubic metre\n",
+      "answer varies due to rounding off errors\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "ni1=2.5*10**19;    #number of electron hole pairs\n",
+    "T1=300;     #temperature(K)\n",
+    "Eg1=0.72*1.6*10**-19;    #energy gap(J)\n",
+    "k=1.38*10**-23;     #boltzmann constant\n",
+    "T2=310;    #temperature(K)\n",
+    "Eg2=1.12*1.6*10**-19;    #energy gap(J)\n",
+    "\n",
+    "#Calculation\n",
+    "x1=-Eg1/(2*k*T1);\n",
+    "y1=(T1**(3/2))*math.exp(x1);\n",
+    "x2=-Eg2/(2*k*T2);\n",
+    "y2=(T2**(3/2))*math.exp(x2);\n",
+    "ni=ni1*(y2/y1);          #number of electron hole pairs\n",
+    "\n",
+    "#Result\n",
+    "print \"number of electron hole pairs is\",round(ni/10**16,2),\"*10**16 per cubic metre\"\n",
+    "print \"answer varies due to rounding off errors\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 9.2, Page number 9.24"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 41,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "intrinsic conductivity is 1.434 *10**4 ohm-1 m-1\n",
+      "intrinsic resistivity is 0.697 *10**-4 ohm m\n",
+      "answer varies due to rounding off errors\n",
+      "number of germanium atoms per m**3 is 4.5 *10**28\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "w=72.6;    #atomic weight\n",
+    "d=5400;    #density(kg/m**3)\n",
+    "Na=6.025*10**26;    #avagadro number\n",
+    "mew_e=0.4;    #mobility of electron(m**2/Vs)\n",
+    "mew_h=0.2;    #mobility of holes(m**2/Vs)\n",
+    "e=1.6*10**-19;\n",
+    "m=9.108*10**-31;    #mass(kg)\n",
+    "ni=2.1*10**19;      #number of electron hole pairs\n",
+    "Eg=0.7;    #band gap(eV)\n",
+    "k=1.38*10**-23;    #boltzmann constant\n",
+    "h=6.625*10**-34;    #plancks constant\n",
+    "T=300;     #temperature(K)\n",
+    "\n",
+    "#Calculation\n",
+    "sigmab=ni*e*(mew_e+mew_h);    #intrinsic conductivity(ohm-1 m-1)\n",
+    "rhob=1/sigmab;     #resistivity(ohm m)\n",
+    "n=Na*d/w;     #number of germanium atoms per m**3\n",
+    "p=n/10**5;   #boron density\n",
+    "sigma=p*e*mew_h;\n",
+    "rho=1/sigma;\n",
+    "\n",
+    "#Result\n",
+    "print \"intrinsic conductivity is\",round(sigma/10**4,3),\"*10**4 ohm-1 m-1\"\n",
+    "print \"intrinsic resistivity is\",round(rho*10**4,3),\"*10**-4 ohm m\"\n",
+    "print \"answer varies due to rounding off errors\"\n",
+    "print \"number of germanium atoms per m**3 is\",round(n/10**28,1),\"*10**28\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 9.3, Page number 9.25"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 44,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "charge carrier density is 2 *10**22 per m**3\n",
+      "electron mobility is 0.035 m**2/Vs\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "e=1.6*10**-19;\n",
+    "RH=3.66*10**-4;    #hall coefficient(m**3/coulomb)\n",
+    "sigma=112;      #conductivity(ohm-1 m-1)\n",
+    "\n",
+    "#Calculation\n",
+    "ne=3*math.pi/(8*RH*e);    #charge carrier density(per m**3)\n",
+    "mew_e=sigma/(e*ne);      #electron mobility(m**2/Vs)\n",
+    "\n",
+    "#Result\n",
+    "print \"charge carrier density is\",int(ne/10**22),\"*10**22 per m**3\"\n",
+    "print \"electron mobility is\",round(mew_e,3),\"m**2/Vs\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 9.4, Page number 9.25"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 45,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "intrinsic conductivity is 0.432 *10**-3 ohm-1 m-1 10.4\n",
+      "conductivity during donor impurity is 10.4 ohm-1 m-1\n",
+      "conductivity during acceptor impurity is 4 ohm-1 m-1\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "mew_e=0.13;    #mobility of electron(m**2/Vs)\n",
+    "mew_h=0.05;    #mobility of holes(m**2/Vs)\n",
+    "e=1.6*10**-19;\n",
+    "ni=1.5*10**16;      #number of electron hole pairs\n",
+    "N=5*10**28;\n",
+    "\n",
+    "#Calculation\n",
+    "sigma1=ni*e*(mew_e+mew_h);    #intrinsic conductivity(ohm-1 m-1)\n",
+    "ND=N/10**8;\n",
+    "n=ni**2/ND;\n",
+    "sigma2=ND*e*mew_e;     #conductivity(ohm-1 m-1)\n",
+    "sigma3=ND*e*mew_h;     #conductivity(ohm-1 m-1)\n",
+    "\n",
+    "#Result\n",
+    "print \"intrinsic conductivity is\",round(sigma1*10**3,3),\"*10**-3 ohm-1 m-1\",sigma2\n",
+    "print \"conductivity during donor impurity is\",sigma2,\"ohm-1 m-1\"\n",
+    "print \"conductivity during acceptor impurity is\",int(sigma3),\"ohm-1 m-1\""
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "metadata": {},
+   "source": [
+    "##Example number 9.5, Page number 9.26"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 50,
+   "metadata": {
+    "collapsed": false
+   },
+   "outputs": [
+    {
+     "name": "stdout",
+     "output_type": "stream",
+     "text": [
+      "conductivity is 4.97 mho m-1\n"
+     ]
+    }
+   ],
+   "source": [
+    "#importing modules\n",
+    "import math\n",
+    "from __future__ import division\n",
+    "\n",
+    "#Variable declaration\n",
+    "e=1.6*10**-19;\n",
+    "Eg=0.72;    #band gap(eV)\n",
+    "k=1.38*10**-23;    #boltzmann constant\n",
+    "T1=293;     #temperature(K)\n",
+    "T2=313;     #temperature(K)\n",
+    "sigma1=2;    #conductivity(mho m-1)\n",
+    "\n",
+    "#Calculation\n",
+    "x=(Eg*e/(2*k))*((1/T1)-(1/T2));\n",
+    "y=round(x/2.303,3);\n",
+    "z=round(math.log10(sigma1),3);\n",
+    "log_sigma2=y+z;\n",
+    "sigma2=10**log_sigma2;     #conductivity(mho m-1)\n",
+    "\n",
+    "#Result\n",
+    "print \"conductivity is\",round(sigma2,2),\"mho m-1\""
+   ]
+  }
+ ],
+ "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
+}
diff --git a/Materials_Science_by_Dr._M._Arumugam/README.txt b/Materials_Science_by_Dr._M._Arumugam/README.txt
new file mode 100755
index 00000000..786b790c
--- /dev/null
+++ b/Materials_Science_by_Dr._M._Arumugam/README.txt
@@ -0,0 +1,10 @@
+Contributed By: Sandhya Arroju
+Course: others
+College/Institute/Organization: Kakatiya University
+Department/Designation: BA
+Book Title: Materials Science
+Author: Dr. M. Arumugam
+Publisher: Anuradha Publications, Chennai
+Year of publication: 2002
+Isbn: 8187721057
+Edition: 3
\ No newline at end of file
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