{ "metadata": { "name": "", "signature": "sha256:599e62479fb81312d9e71ded8b631cb3f6c046aff5ae2a1f3f8129c2f46ca250" }, "nbformat": 3, "nbformat_minor": 0, "worksheets": [ { "cells": [ { "cell_type": "heading", "level": 1, "metadata": {}, "source": [ "Chapter 13:Oscillators" ] }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Example 13.1 Page no.421" ] }, { "cell_type": "code", "collapsed": false, "input": [ "\n", "L=58.6*10**(-6) # H, inductance\n", "C=300*10**(-12) # F, capacitance\n", "\n", "#Calculation\n", "import math\n", "fo=1/(2*math.pi*math.sqrt(L*C))\n", "\n", "#Result\n", "print \" The Frequency of Oscillation of Tuned Collector Oscillator is fo = \",round(fo/10**3,2),\"KHz\"" ], "language": "python", "metadata": {}, "outputs": [] }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Example 13.2 Page no.427" ] }, { "cell_type": "code", "collapsed": false, "input": [ "\n", "R=100000.0 # Ohms, resistance\n", "C=0.01*10**(-6) #F, capacitance\n", "\n", "#Calculation\n", "import math\n", "fo=1/(2*math.pi*R*C*math.sqrt(6))\n", "#Result\n", "print \"The Frequency of Oscillation of Vacuum Tube Phase Shift Oscillator is fo = \",round(fo,2),\"Hz\"" ], "language": "python", "metadata": {}, "outputs": [] }, { "cell_type": "heading", "level": 3, "metadata": {}, "source": [ "Example 13.3 Page no.427" ] }, { "cell_type": "code", "collapsed": false, "input": [ "\n", "R1=220000.0 # Ohms, Resistance 1\n", "R2=220000.0 # Ohms Resistance 2\n", "C1=250*10**(-12) #F, capacitance 1 \n", "C2=250*10**(-12) #F, capacitance 2\n", "\n", "#Calculation\n", "import math\n", "fo=1/(2*math.pi*math.sqrt(R1*C1*R2*C2))\n", "# Result\n", "print \"The Frequency of Oscillation of Wein Bridge Oscillator is fo = \",round(fo/10**3,2),\"KHz\"" ], "language": "python", "metadata": {}, "outputs": [] } ], "metadata": {} } ] }