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authorkinitrupti2017-05-12 18:40:35 +0530
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-{
- "metadata": {
- "name": "chapter22.ipynb"
- },
- "nbformat": 3,
- "nbformat_minor": 0,
- "worksheets": [
- {
- "cells": [
- {
- "cell_type": "heading",
- "level": 1,
- "metadata": {},
- "source": [
- "Chapter 22: Kinetics Of Rigid Body:Force And Acceleration"
- ]
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 22.22-1,Page No:562"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "# Initilization of variables\n",
- "\n",
- "N=1500 # r.p.m\n",
- "r=0.5 # m # radius of the disc\n",
- "m=300 # N # weight of the disc\n",
- "t=120 # seconds # time in which the disc comes to rest\n",
- "omega=0 \n",
- "pi=3.14 \n",
- "g=9.81 # m/s^2\n",
- "\n",
- "# Calculations\n",
- "\n",
- "omega_0=(2*pi*N)*0.01666 # rad/s #1/60=0.01666\n",
- "\n",
- "# angular deceleration is given as,\n",
- "alpha=-(omega_0/t) # radian/second^2\n",
- "theta=(omega_0**2)/(2*(-alpha)) # radian\n",
- "\n",
- "# Let n be the no of revolutions taken by the disc before it comes to rest, then\n",
- "n=theta/(2*pi)\n",
- "\n",
- "# Now,\n",
- "I_G=((0.5)*m*r**2)/g\n",
- "\n",
- "# The frictional torque is given as,\n",
- "M=I_G*alpha # N-m\n",
- "\n",
- "# Results\n",
- "\n",
- "print\"(a) The no of revolutions executed by the disc before coming to rest is \",round(n,2)\n",
- "print\"(b) The frictional torque is \",round(M),\"N-m\"\n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(a) The no of revolutions executed by the disc before coming to rest is 1499.4\n",
- "(b) The frictional torque is -5.0 N-m\n"
- ]
- }
- ],
- "prompt_number": 9
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 22.22-2,Page No:563"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "# Initilization of variables\n",
- "\n",
- "s=1 # m\n",
- "mu=0.192 # coefficient of static friction\n",
- "g=9.81 # m/s^2\n",
- "\n",
- "# Calculations\n",
- "\n",
- "# The maximum angle of the inclined plane is given as,\n",
- "theta=arctan(3*mu)*(180/pi) # degree\n",
- "a=(2/3)*g*sin(theta*(pi/180)) # m/s^2 # by solving eq'n 4\n",
- "v=(2*a*s)**0.5 # m/s\n",
- "\n",
- "# Let the acceleration at the centre be A which is given as,\n",
- "A=g*sin(theta*(pi/180)) # m/s^2 # from eq'n 1\n",
- "\n",
- "# Results\n",
- "\n",
- "print\"(a) The acceleration at the centre is \",round(A,3),\"m/s^2\"\n",
- "print\"(b) The maximum angle of the inclined plane is \",round(theta),\"degree\"\n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(a) The acceleration at the centre is 4.896 m/s^2\n",
- "(b) The maximum angle of the inclined plane is 30.0 degree\n"
- ]
- }
- ],
- "prompt_number": 11
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 22.22-5,Page No:568"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "# Initilization of variables\n",
- "\n",
- "W_a=25 # N \n",
- "W_b=25 # N \n",
- "W=200 # N # weight of the pulley\n",
- "i_g=0.2 # m # radius of gyration\n",
- "g=9.81 # m/s^2\n",
- "\n",
- "# Calculations\n",
- "\n",
- "# Solving eqn's 1 & 2 for acceleration of weight A (assume a)\n",
- "a=(0.15*W_a*g)/(((W*i_g**2)/(0.45))+(0.45*W_a)+((0.6*W_b)/(3))) # m/s^2\n",
- "\n",
- "# Results\n",
- "\n",
- "print\"The acceleration of weight A is \",round(a,2),\"m/s^2\"\n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "The acceleration of weight A is 1.08 m/s^2\n"
- ]
- }
- ],
- "prompt_number": 13
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 22.22-8,Page No:571"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "# Initilization of variables\n",
- "\n",
- "r_1=0.075 # m\n",
- "r_2=0.15 # m\n",
- "P=50 # N\n",
- "W=100 # N\n",
- "i_g=0.05 # m\n",
- "theta=30 # degree\n",
- "g=9.81 # m/s^2\n",
- "\n",
- "# Calculations\n",
- "\n",
- "# The eq'n for acceleration of the pool is given by solving eqn's 1,2 &3 as,\n",
- "a=(50*g*(r_2*cos(theta*(pi/180))-r_1))/(100*((i_g**2/r_2)+r_2)) # m/s^2\n",
- "\n",
- "# Results\n",
- "\n",
- "print\"The acceleration of the pool is \",round(a,2),\"m/s^2\"\n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "The acceleration of the pool is 1.62 m/s^2\n"
- ]
- }
- ],
- "prompt_number": 15
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 22.22-10,Page No:574"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "# Initilization of variables\n",
- "\n",
- "L=1 # m # length of rod AB\n",
- "m=10 # kg # mass of the rod\n",
- "g=9.81 \n",
- "theta=30 # degree\n",
- "\n",
- "# Calculations\n",
- "\n",
- "# solving eq'n 4 for omega we get,\n",
- "omega=(2*16.82*sin(theta*(pi/180)))**0.5 # rad/s\n",
- "\n",
- "# Now solving eq'ns 1 &3 for alpha we get,\n",
- "alpha=(1.714)*g*cos(theta*(pi/180)) # rad/s\n",
- "\n",
- "# Components of reaction are given as,\n",
- "R_t=((m*g*cos(theta*(pi/180)))-((m*alpha*L)/4)) # N\n",
- "R_n=((m*omega**2*L)/4)+(m*g*sin(theta*(pi/180))) # N\n",
- "R=(R_t**2+R_n**2)**0.5 # N \n",
- "\n",
- "# Results\n",
- "\n",
- "print\"(a) The angular velocity of the rod is \",round(omega,2),\"rad/sec\"\n",
- "print\"(b) The reaction at the hinge is \",round(R,1),\"N\"\n"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "(a) The angular velocity of the rod is 4.1 rad/sec\n",
- "(b) The reaction at the hinge is 103.2 N\n"
- ]
- }
- ],
- "prompt_number": 31
- }
- ],
- "metadata": {}
- }
- ]
-} \ No newline at end of file