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diff --git a/Applied_Physics_for_Engineers/Chapter_10.ipynb b/Applied_Physics_for_Engineers/Chapter_10.ipynb new file mode 100755 index 00000000..6c1f1d6b --- /dev/null +++ b/Applied_Physics_for_Engineers/Chapter_10.ipynb @@ -0,0 +1,264 @@ +{ + "metadata": { + "name": "" + }, + "nbformat": 3, + "nbformat_minor": 0, + "worksheets": [ + { + "cells": [ + { + "cell_type": "heading", + "level": 1, + "metadata": {}, + "source": [ + "Chapter 10: Electrostatics" + ] + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 10.1, Page 507" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "#Variable Declaration\n", + "m = 4e-013; # Mass of the particle, kg\n", + "q = 2.4e-019; # Charge on particle, C\n", + "d = 2e-002; # Distance between the two horizontally charged plates, m\n", + "g = 9.8; #`Acceleration due to gravity, m/sec-square\n", + "\n", + "#Calculations\n", + "E = (m*g)/q ; # Electric field strength, N/C\n", + "V = E*d; # Potential difference between the two charged horizontal plates, V\n", + "\n", + "#Result\n", + "print \"The potential difference between the two horizontally charged plates = %3.1e V\"%V\n", + "#Incorrect answer in textbook" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The potential difference between the two horizontally charged plates = 3.3e+05 V\n" + ] + } + ], + "prompt_number": 9 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 10.2, Page 507" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "from math import *\n", + "\n", + "#Variable Declaration\n", + "q1 = 1e-009; # Charge at first corner, C\n", + "q2 = 2e-009; # Charge at second corner, C\n", + "q3 = 3e-009; # Charge at third corner, C\n", + "d = 1.; # Side of the equilateral triangle, m\n", + "theta = 30; # Angle at which line joining the observation point to the source charge makes with the side, degrees\n", + "\n", + "#Calculations\n", + "r = (d/2)/cos(theta*pi/180); # Distance of observation point from the charges, m\n", + "#since,1/4*%pi*%eps = 9e+009;\n", + "V = (q1+q2+q3)*(9e+009)/r; # Elecric potential, V\n", + "\n", + "#Result\n", + "print \"The electric potential at the point equidistant from the three corners of the triangle = %4.1f V\"%V\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The electric potential at the point equidistant from the three corners of the triangle = 93.5 V\n" + ] + } + ], + "prompt_number": 10 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 10.3, Page 508" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "from math import *\n", + "\n", + "#Variable Declaration\n", + "q = 2e-008; \n", + "q1 = q; # Charge at first corner, C\n", + "q2 = -2*q; # Charge at second corner, C\n", + "q3 = 3*q; # Charge at third corner, C\n", + "q4 = 2*q; # Charge at fourth corner, C\n", + "d = 1; # Side of the square, m\n", + "\n", + "#Calculations\n", + "r = round(d*sin(45*pi/180),2); # Distance of centre of the square from each corner, m\n", + "V = (q1+q2+q3+q4)*(9e+009)/r; # Elecric potential at the centre of the square, V \n", + "\n", + "#Result\n", + "print \"The electric potential at the centre of the square = %4d V\"%V\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The electric potential at the centre of the square = 1014 V\n" + ] + } + ], + "prompt_number": 17 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 10.6, Page 511" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "#Variable Declaration\n", + "V = 60; # Electric potential of smaller drop, volt\n", + "r = 1; # For simplcity assume radius of each small drop to be unity, unit\n", + "q = 1; # For simplicity assume charge on smaller drop to be unity, C\n", + "k = 1; # For simplicity assume Coulomb's constant to be unity, unit\n", + "\n", + "#Calculations\n", + "R = 2**(1./3)*r; # Radius of bigger drop, unit\n", + "Q = 2*q; # Charge on bigger drop, C\n", + "V_prime = k*Q/R*V; # Electric potential of bigger drop, volt\n", + "\n", + "#Result\n", + "print \"The electric potential of new drop = %4.1f V\"%V_prime\n", + "#Incorrect answer in the textbook" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The electric potential of new drop = 95.2 V\n" + ] + } + ], + "prompt_number": 19 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 10.7, Page 512" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "#Variable Declaration\n", + "m = 9.1e-031; # Mass of the electron, kg\n", + "e = 1.6e-019; # Charge on an electron, C\n", + "g = 9.8; # Acceleration due to gravity, m/sec-square\n", + "\n", + "#Calculations\n", + "# Electric force, F = e*E, where F = m*g or e*E = m*g\n", + "E = m*g/e; # Electric field which would balance the weight of an electron placed in it, N/C\n", + "\n", + "#Result\n", + "print \"The required electric field strength = %3.1e N/C\"%E\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The required electric field strength = 5.6e-11 N/C\n" + ] + } + ], + "prompt_number": 20 + }, + { + "cell_type": "heading", + "level": 2, + "metadata": {}, + "source": [ + "Example 10.8, Page 512" + ] + }, + { + "cell_type": "code", + "collapsed": false, + "input": [ + "#Variable Declaration\n", + "q1 = 8e-007; # First Charge, C\n", + "q2 = -8e-007; # Second Charge, C\n", + "r = 15e-002; # Distance between the two charges, m\n", + "k = 9e+009; # Coulomb's constant, N-metre-square/coulomb-square\n", + "\n", + "#Calculations&#Results\n", + "E1 = k*q1/r**2; # Electric field strength due to charge 8e-007 C\n", + "print \"The electric field strength at midpoint = %3.1e N/C\"%E1\n", + "E2 = abs(k*q2/r**2); # Electric field strength -8e-007 C \n", + "print \"The electric field strength at midpoint = %3.1e N/C\"%E2\n", + "# Total electric field strength at the mid-point is\n", + "E = E1+E2; # Net electric field at mid point, N/C\n", + "print \"The net electric field strength at midpoint = %3.1e N/C\"%E\n" + ], + "language": "python", + "metadata": {}, + "outputs": [ + { + "output_type": "stream", + "stream": "stdout", + "text": [ + "The electric field strength at midpoint = 3.2e+05 N/C\n", + "The electric field strength at midpoint = 3.2e+05 N/C\n", + "The net electric field strength at midpoint = 6.4e+05 N/C\n" + ] + } + ], + "prompt_number": 21 + } + ], + "metadata": {} + } + ] +}
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