{ "metadata": { "name": "", "signature": "sha256:1e2ea72063f4480e1666d90f5821f69263d6f609957c096a14e46eb50fe68a8d" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Chapter 21:Motion of Rotation" ] }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 21.1, Page no.447" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#variable declaration\n", "omega_0=0 #initial angular velocity\n", "alpha=0.5 #angular acceleration in rad/sec**2\n", "t=10 #time in sec\n", "\n", "#calculation\n", "omega=omega_0+alpha*t\n", "theta=omega_0*t+(alpha*t**2/2)\n", "\n", "#Result\n", "print\"Angular velocity of the flywheel, omega=\",int(omega),\"rad/sec\"\n", "print\"Angular displacement of the flywheel, theta=\",int(theta),\"rad\"" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Angular velocity of the flywheel, omega= 5 rad/sec\n", "Angular displacement of the flywheel, theta= 25 rad\n" ] } ], "prompt_number": 1 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 21.4, Page no.448" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "#variable declaration\n", "omega_0=0 #initial angular velocity\n", "alpha=0.5 #acceleration in rad/sec**2\n", "t_1=120 #timetaken in sec\n", "omega1_0=60 #initial angular velocity when pulley is coming to rest in rad/sec\n", "alpha_2=-0.3 #Retardation in rad/sec**2\n", "\n", "\n", "#calculation\n", "#To calculate angular speed of pully in r.p.m. at the end of 2 min.\n", "omega=round((omega_0+alpha*t_1)/(2*math.pi),2)\n", "#To calculate time in which the pulley will come to rest\n", "t_2=-omega1_0/alpha_2\n", "\n", "#Result\n", "print\"Angular speed of pully in r.p.m. at the end of 2 min., omega=\",int(omega*60),\"r.p.m.\"\n", "print\"Time in which the pulley will come to rest, t_2=\",int(t_2),\"sec\"\n", "\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Angular speed of pully in r.p.m. at the end of 2 min., omega= 573 r.p.m.\n", "Time in which the pulley will come to rest, t_2= 200 sec\n" ] } ], "prompt_number": 2 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 21.9, Page no.453" ] }, { "cell_type": "code", "collapsed": false, "input": [ "#variable declaration\n", "r=0.6 #radius of wheel in m\n", "omega_0=0 #initial angular velocity\n", "alpha=0.8 #angular acceleration in rad/s**2\n", "t=5 #time in s\n", "\n", "#calculation\n", "omega=omega_0+alpha*t\n", "v=r*omega\n", "\n", "#result\n", "print\"Linear velocity of the point on the periphery of the wheel, v=\",round(v,1),\"m/s\"\n", "\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Linear velocity of the point on the periphery of the wheel, v= 2.4 m/s\n" ] } ], "prompt_number": 3 }, { "cell_type": "heading", "level": 2, "metadata": {}, "source": [ "Example 21.10, Page no.453" ] }, { "cell_type": "code", "collapsed": false, "input": [ "import math\n", "#variable declaration\n", "r=1 #Radius if pulley in m\n", "N=240 #angular frequency in r.p.m\n", "\n", "#calculation\n", "omega=2*math.pi*N/60\n", "v=r*omega\n", "\n", "#Result\n", "print\"Linear velocity of the particle on the periphery of the wheel, v=\",round(v,1),\"m/s\"\n" ], "language": "python", "metadata": {}, "outputs": [ { "output_type": "stream", "stream": "stdout", "text": [ "Linear velocity of the particle on the periphery of the wheel, v= 25.1 m/s\n" ] } ], "prompt_number": 4 }, { "cell_type": "code", "collapsed": false, "input": [], "language": "python", "metadata": {}, "outputs": [] } ], "metadata": {} } ] }