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diff --git a/Linear_Integrated_Circuit_by_M._S._Sivakumar/Ch13.ipynb b/Linear_Integrated_Circuit_by_M._S._Sivakumar/Ch13.ipynb deleted file mode 100755 index bf527bf0..00000000 --- a/Linear_Integrated_Circuit_by_M._S._Sivakumar/Ch13.ipynb +++ /dev/null @@ -1,438 +0,0 @@ -{ - "cells": [ - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "# Chapter 13 Waveform Generators" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.1 Pg 378" - ] - }, - { - "cell_type": "code", - "execution_count": 1, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "the frequency selective element resistor is = 6.50 K ohm \n", - "The feedback resistance is = 188.4 K ohm\n" - ] - } - ], - "source": [ - "from math import sqrt, pi\n", - "from __future__ import division\n", - "# to design RC phase shift oscillator for the oscillation frequency f = 1 KHz\n", - "f =1 # # KHz\n", - "C = 0.01 # # uF\n", - "\n", - "# The oscillation frequency of practical RC phase shift oscillator is defined as\n", - "#w = 1/(sqrt(6)*R*C)#\n", - "\n", - "# gain of practical RC phase shift oscillator is\n", - "#A = R1/R = 29 equation 1\n", - "# the frequency selective element resistor\n", - "#R = 1/(sqrt(6)*w*C)#\n", - "R = 1/(sqrt(6)*2*pi*f*C)#\n", - "print 'the frequency selective element resistor is = %0.2f'%R,' K ohm '\n", - "\n", - "# The feedback resistance\n", - "R1 = 29*R # # from equation 1\n", - "print 'The feedback resistance is = %0.1f'%R1,' K ohm'" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.2 Pg 379" - ] - }, - { - "cell_type": "code", - "execution_count": 2, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "the oscillator frequency of practical RC phase shift oscillator f is = 0.52 KHz \n" - ] - } - ], - "source": [ - "# to determine the oscillaton frequency of the phase shift oscillator\n", - "C = 0.05 # # uF\n", - "R = 2.5 # # K ohm\n", - "\n", - "# the oscillator frequency of practical RC phase shift oscillator f\n", - "f = 1/(2*pi*(sqrt(6)*(R*C)))#\n", - "print 'the oscillator frequency of practical RC phase shift oscillator f is = %0.2f'%f,' KHz '" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.3 Pg 380" - ] - }, - { - "cell_type": "code", - "execution_count": 3, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "the oscillator frequency of practical RC phase shift oscillator f is = 6.63 kHz \n" - ] - } - ], - "source": [ - "# to calculate the frequency of a wein bridge oscillator\n", - "C = 2400*10**-12 # # F\n", - "R = 10*10**3 # # ohm\n", - "\n", - "# the oscillator frequency of practical RC phase shift oscillator f\n", - "f = 1/(2*pi*R*C)/1e3#\n", - "print 'the oscillator frequency of practical RC phase shift oscillator f is = %0.2f'%f,' kHz '" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.4 Pg 380" - ] - }, - { - "cell_type": "code", - "execution_count": 4, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "the resistor R is = 15.9 K ohm \n", - "The resistor R2 value is = 20.00 K ohm \n" - ] - } - ], - "source": [ - "# to design the wien bridge oscillator for the oscillation frequency f = 1 KHz\n", - "f = 1 # # K ohm\n", - "C = 0.01 # # uF\n", - "\n", - "\n", - "# the frequency f is define as\n", - "# f = 1/(2*pi*R*C)#\n", - "\n", - "# the resistor R is\n", - "R = 1/(2*pi*f*C)#\n", - "print 'the resistor R is = %0.1f'%R,' K ohm '\n", - "\n", - "# the loop gain of the wien bridge oscillator is unity which is defined as\n", - "# A = (1+(R2/R1))*(1/3) = 1 #\n", - "# R2/R1 = 2 #\n", - "R1 = 10 # # K ohm we assume\n", - "R2 = 2*R1 #\n", - "print 'The resistor R2 value is = %0.2f'%R2,' K ohm '" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.5 Pg 382" - ] - }, - { - "cell_type": "code", - "execution_count": 5, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "the frequency of wien bridge oscillator f is = 159.155 Hz \n" - ] - } - ], - "source": [ - "# to calculate the frequency of a wein bridge oscillator\n", - "C = 0.05*10**-6 # # F\n", - "R = 20*10**3 # # ohm\n", - "R1 = 10*10**3 # # ohm\n", - "R2 = 20*10**3 # #ohm\n", - "\n", - "# the frequency of wien bridge oscillator f\n", - "f = 1/(2*pi*R*C)#\n", - "print 'the frequency of wien bridge oscillator f is = %0.3f'%f,' Hz '" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.6 Pg 382" - ] - }, - { - "cell_type": "code", - "execution_count": 10, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "The frequency of the astable multivibrator is = 0.87/(C*R)\n" - ] - } - ], - "source": [ - "from sympy import symbols, log, N\n", - "R, C = symbols('R C')\n", - "# Determine the frequency response of the astable multivibrator circuit\n", - "Vsat = 2.5 #\n", - "VT = 0.7 #\n", - "\n", - "# The frequency of the astable multivibrator is\n", - "f = (1/(2*R*C*log((Vsat+VT)/(Vsat-VT))))#\n", - "print 'The frequency of the astable multivibrator is =',N(f,2)" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.7 Pg 383" - ] - }, - { - "cell_type": "code", - "execution_count": 11, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "The value of resistance R2 is = 32.86 K ohm \n", - "The value of resistor R is = 10.52 K ohm\n" - ] - } - ], - "source": [ - "from math import log\n", - "# Design astable multivibrator for the frequency f = 10 KHz\n", - "f = 10 # # K ohm\n", - "Vsat = 3 #\n", - "VT = 0.7 #\n", - "\n", - "# The saturation voltage of an astable multivibrator is defined as\n", - "# Vsat = (R1+R2/R1)+VT #\n", - "R1 = 10 # # K ohm we choose\n", - "R2 = ((Vsat/VT)-1)*R1 #\n", - "print 'The value of resistance R2 is = %0.2f'%R2,' K ohm '\n", - "\n", - "# The frequency of an astable multivibrator is defined as\n", - "C = 0.01 # # uF\n", - "# f = (1/(2*R*C*log(1+(2*R1/R2))))#\n", - "\n", - "R = 1/(2*f*C*log(1+2*R1/R2))#\n", - "print 'The value of resistor R is = %0.2f'%R,' K ohm'" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.8 Pg 384" - ] - }, - { - "cell_type": "code", - "execution_count": 12, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "The value of resistor R is = 200.00 ohm \n" - ] - } - ], - "source": [ - "# to design astable multivibrator \n", - "f = 25*10**3 #\n", - "\n", - "# The output frequency of practical astable multivibrator is defined as\n", - "# f = 1/(2*R*C)#\n", - "C = 0.1*10**-6 # # uF we choose\n", - "R = 1/(2*f*C)#\n", - "print 'The value of resistor R is = %0.2f'%R,'ohm '" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.9 Pg 385" - ] - }, - { - "cell_type": "code", - "execution_count": 14, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "The value of resistance R is = 579.7 ohm \n", - "The value of resistance R2 is = 9.94 K ohm \n" - ] - } - ], - "source": [ - "# Design a monostable circuit with frequency f = 25 KHz\n", - "f =25*10**3 # # Hz\n", - "\n", - "# The output frequency of monostable multivibrator is defined as \n", - "# f = 1/(0.69*R*C)#\n", - "C = 0.1*10**-6 #\n", - "R = 1/(0.69*f*C)#\n", - "print 'The value of resistance R is = %0.1f'%R,' ohm '\n", - "\n", - "# In the practical monostable multivibrator\n", - "# ln(1+(R2/R1))= 0.69 #\n", - "R1 = 10*10**3 # # we choose\n", - "R2 = R1*(1.99372-1)#\n", - "print 'The value of resistance R2 is = %0.2f'%(R2/1000),' K ohm ' # Round Off Error " - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.10 Pg 386" - ] - }, - { - "cell_type": "code", - "execution_count": 16, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "the output of monostable multivibrator is = 6.01 kHz\n" - ] - } - ], - "source": [ - "# Determine the frequency of the monostable multivibrator\n", - "R1 = 5*10**3 #\n", - "R2 =15*10**3 #\n", - "C = 0.01*10**-6 #\n", - "R = 12*10**3 #\n", - "\n", - "# the output of monostable multivibrator is defined as\n", - "f = 1/(R*C*(log(1+(R2/R1))))/1e3 # kHz\n", - "print 'the output of monostable multivibrator is = %0.2f'%f,' kHz'" - ] - }, - { - "cell_type": "markdown", - "metadata": {}, - "source": [ - "## Example 13.11 Pg 386" - ] - }, - { - "cell_type": "code", - "execution_count": 17, - "metadata": { - "collapsed": false - }, - "outputs": [ - { - "name": "stdout", - "output_type": "stream", - "text": [ - "the output of monostable multivibrator is = 4.00 KHz\n" - ] - } - ], - "source": [ - " # Determine the frequency of the monostable multivibrator\n", - "R1 = 5*10**3 #\n", - "R2 =15*10**3 #\n", - "C = 0.01 #\n", - "R = 25 #\n", - "\n", - "# the output of monostable multivibrator is defined as\n", - "f = 1/(R*C)#\n", - "print 'the output of monostable multivibrator is = %0.2f'%f,' KHz'" - ] - } - ], - "metadata": { - "kernelspec": { - "display_name": "Python 2", - "language": "python", - "name": "python2" - }, - "language_info": { - "codemirror_mode": { - "name": "ipython", - "version": 2 - }, - "file_extension": ".py", - "mimetype": "text/x-python", - "name": "python", - "nbconvert_exporter": "python", - "pygments_lexer": "ipython2", - "version": "2.7.9" - } - }, - "nbformat": 4, - "nbformat_minor": 0 -} |