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+{
+ "metadata": {
+ "name": ""
+ },
+ "nbformat": 3,
+ "nbformat_minor": 0,
+ "worksheets": [
+ {
+ "cells": [
+ {
+ "cell_type": "heading",
+ "level": 1,
+ "metadata": {},
+ "source": [
+ "Chapter 01 : Energy Band in Solid"
+ ]
+ },
+ {
+ "cell_type": "heading",
+ "level": 2,
+ "metadata": {},
+ "source": [
+ "Example 1.2, Page No 55"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "collapsed": false,
+ "input": [
+ "import math\n",
+ "#initialisation of variables\n",
+ "\n",
+ "d=0.001 #distance between parallel plate in m\n",
+ "V=1000.0 #applied voltage\n",
+ "q=1.6*(10**-19) #charge on an electron\n",
+ "m = 9.1*(10**-31) #mass of electron in kg\n",
+ "#Time taken by electron to reach other side of parallel plate capacitor\n",
+ "E=V/d #Electric Field in V/m\n",
+ "#Formulae : s = u*t + (a*t^2)/2\n",
+ "\n",
+ "#Calculations\n",
+ "a = (q*E)/m #acceleration on electron in m/s^2\n",
+ "t = (2*d/a)**0.5 #time taken to reach the other side of plate\n",
+ "print(\"Time taken to reach other side = %.2f sec \" %t)\n",
+ "\n",
+ "#Magnitude of force exerted on electron\n",
+ "print('Since the potential is constant the force will be constant between the paltes of capacitor')\n",
+ "F=q*E #force\n",
+ "print(\"Force on electron = %.2f N \" %F)\n",
+ "#Velocity of electron at the other plate\n",
+ "#Formulae: v = u + a*t\n",
+ "v = a*t #velocity at the end of other plate\n",
+ "\n",
+ "#Results\n",
+ "print(\"V = %.2f m/sec \" %V)\n"
+ ],
+ "language": "python",
+ "metadata": {},
+ "outputs": [
+ {
+ "output_type": "stream",
+ "stream": "stdout",
+ "text": [
+ "Time taken to reach other side = 0.00 sec \n",
+ "Since the potential is constant the force will be constant between the paltes of capacitor\n",
+ "Force on electron = 0.00 N \n",
+ "V = 1000.00 m/sec \n"
+ ]
+ }
+ ],
+ "prompt_number": 1
+ }
+ ],
+ "metadata": {}
+ }
+ ]
+} \ No newline at end of file