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author | hardythe1 | 2015-06-11 17:31:11 +0530 |
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committer | hardythe1 | 2015-06-11 17:31:11 +0530 |
commit | 79c59acc7af08ede23167b8455de4b716f77601f (patch) | |
tree | 2d6ff34b6f131d2671e4c6b798f210b3cb1d4ac7 /Electronic_Devices_and_Circuits/Chapter16_1.ipynb | |
parent | df60071cf1d1c18822d34f943ab8f412a8946b69 (diff) | |
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diff --git a/Electronic_Devices_and_Circuits/Chapter16_1.ipynb b/Electronic_Devices_and_Circuits/Chapter16_1.ipynb deleted file mode 100755 index 9d8b3b5f..00000000 --- a/Electronic_Devices_and_Circuits/Chapter16_1.ipynb +++ /dev/null @@ -1,581 +0,0 @@ -{
- "metadata": {
- "name": ""
- },
- "nbformat": 3,
- "nbformat_minor": 0,
- "worksheets": [
- {
- "cells": [
- {
- "cell_type": "heading",
- "level": 1,
- "metadata": {},
- "source": [
- "Chapter 16 : Signal generators"
- ]
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.1, Page No 668"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "\n",
- "Vcc=10.0\n",
- "Ib=500.0*10**-9\n",
- "Acl=29.0\n",
- "f=1.0*10**3\n",
- "\n",
- "#Calculations\n",
- "print(\" phase shift oscillator\")\n",
- "I1=100*Ib\n",
- "vo=Vcc-1\n",
- "vi=vo/Acl\n",
- "R1=vi/I1\n",
- "R1=5.6*10**3#use standard value 5.6Kohm\n",
- "R2=Acl*R1\n",
- "R2=180*10**3#use satndard value 180Kohm to give Acl>180\n",
- "R3=R2R=R1\n",
- "C=1.0/(2*3.14*R3*f*math.sqrt(6))\n",
- "\n",
- "#Results\n",
- "print(\"The value of C = %.2f \" %(C*10**9))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- " phase shift oscillator\n",
- "The value of C = 11.61 \n"
- ]
- }
- ],
- "prompt_number": 28
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.2, Page No 672"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "#initialisation of variables\n",
- "\n",
- "f=40.0*10**3\n",
- "L=100.0*10**-3\n",
- "vp=8.0\n",
- "\n",
- "#Calculations\n",
- "print(\"colpitts oscillator\")\n",
- "Ct=1/(4*3.14*3.14*(f**2)*L)\n",
- "C1=10*Ct\n",
- "C2=1/((1/Ct)-(1/C1))\n",
- "C2=180*10**-12#use standard value\n",
- "Xc2=1/(2*3.14*f*C2)\n",
- "Xc1=1/(2*3.14*f*C1)\n",
- "R1=10*Xc1\n",
- "R1=27*10**3#use standard value\n",
- "Acl=C1/C2\n",
- "R2=Acl*R1\n",
- "R2=270*10**3#use stabdard value\n",
- "R3=(R1*R2)/(R1+R2)\n",
- "f2=Acl*f\n",
- "SR=2*3.14*f*vp\n",
- "\n",
- "#Results\n",
- "print(\"The value of SR is %.2f \" %(SR/1000))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "colpitts oscillator\n",
- "The value of SR is 2009.60 \n"
- ]
- }
- ],
- "prompt_number": 29
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.3 Page No 678"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "#initialisation of variables\n",
- "\n",
- "vo=8.0\n",
- "f=100.0*10**3\n",
- "print(\" hartley oscillator\")\n",
- "Vcc=vo+1\n",
- "Xl2=1.0*10**3\n",
- "\n",
- "#Calculations\n",
- "L2=Xl2/(2*3.14*f)\n",
- "L2=1.5*10**-3#use standard value\n",
- "L1=L2/10.0\n",
- "Lt=L1+L2#(assuming M=0)\n",
- "C1=1/(4*(3.14**2)*(f**2)*Lt)\n",
- "C1=1500*10**-12#use 1500pF with aadditional parallel capacitance if necessary\n",
- "#C1>>stray capacitance\n",
- "Xl1=2*3.14*f*L1#R1>>Xl1\n",
- "R1=1*10**3\n",
- "Acl=L2/L1\n",
- "R2=Acl*R1\n",
- "R3=(R1*R2)/(R1+R2)\n",
- "print(\"full power bandwidth \")\n",
- "f2=Acl*f\n",
- "SR=2*3.14*f*vo\n",
- "\n",
- "#Results\n",
- "print(\"The value of SR is %.2f \" %(SR/1000))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- " hartley oscillator\n",
- "full power bandwidth \n",
- "The value of SR is 5024.00 \n"
- ]
- }
- ],
- "prompt_number": 30
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.4, Page No 680"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "\n",
- "f=100.0*10**3\n",
- "Vo=9.0\n",
- "Acl=3.0\n",
- "\n",
- "#Calculations\n",
- "print(\" design of wein bridge oscillator\")\n",
- "Vcc=Vo+1\n",
- "C1=1000.0*10**-12#standard value\n",
- "C2=C1\n",
- "R1=1.0/(2*3.14*f*C1)\n",
- "R2=R1\n",
- "R4=R2\n",
- "R3=2*R4\n",
- "R3=3.3*10**3#use standard value\n",
- "print(\" minimum full power bandwidth\")\n",
- "f2=Acl*f\n",
- "SR=2*3.14*f*Vo\n",
- "\n",
- "#Results\n",
- "print(\"The value of SR is %.2f \" %(SR/1000))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- " design of wein bridge oscillator\n",
- " minimum full power bandwidth\n",
- "The value of SR is 5652.00 \n"
- ]
- }
- ],
- "prompt_number": 31
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.5 Page No 683"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "\n",
- "f=5.0*10**3\n",
- "vo=5.0\n",
- "I1=1.0*10**-3\n",
- "Vf=0.7\n",
- "\n",
- "#Calculations\n",
- "print(\"phase shift oscillator\")\n",
- "R1=(vo/29.0)/I1\n",
- "R1=150#use standard value\n",
- "R2=29*R1\n",
- "R4=(2*Vf)/I1\n",
- "R4=1.5*10**3#use 1.5kohm standard value\n",
- "R5=R2-R4\n",
- "R6=.4*R5\n",
- "R7=.8*R5\n",
- "R=R1\n",
- "C=1.0/(2*3.14*R*f*math.sqrt(6))\n",
- "\n",
- "#Results\n",
- "print(\"The value of C is %.2f mF\" %(C*10**9))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "phase shift oscillator\n",
- "The value of C is 86.68 mF\n"
- ]
- }
- ],
- "prompt_number": 32
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.6 Page No 686"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "#initialisation of variables\n",
- "\n",
- "rds=600.0\n",
- "Vgs=1.0\n",
- "Vd1=0.7\n",
- "f=100.0*10**3\n",
- "\n",
- "#Calculations\n",
- "print(\"wien bridge ocillator\")\n",
- "R4=560.0\n",
- "R3=2*((R4*rds)/(R4+rds))\n",
- "I5=200.0*10**-6\n",
- "Vo=6\n",
- "R6=Vgs/I5\n",
- "R5=(Vo-(Vgs+Vd1))/I5\n",
- "print(\" C4 discharge voltage \")\n",
- "Vc=.1*Vgs\n",
- "print(\"C4 discharge time\")\n",
- "T=1/f\n",
- "Ic=I5\n",
- "C4=(Ic*T)/Vc\n",
- "Xc3=rds/10#at oscillating frequency\n",
- "C3=1/(2*3.14*f*Xc3)\n",
- "\n",
- "#Results\n",
- "print(\"The value of C3 is %.2f mF\" %(C3*10**9))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "wien bridge ocillator\n",
- " C4 discharge voltage \n",
- "C4 discharge time\n",
- "The value of C3 is 26.54 mF\n"
- ]
- }
- ],
- "prompt_number": 33
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.7, Page No 689"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "\n",
- "Vo=14.0\n",
- "Vr3=.5\n",
- "Ib=500.0*10**-9\n",
- "f=1.0*10**3\n",
- "\n",
- "#Calculations\n",
- "print(\"square wave generator\")\n",
- "Vcc=Vo+1\n",
- "UTP=Vr3\n",
- "LTP=UTP\n",
- "I2=100*Ib\n",
- "R3=Vr3/I2\n",
- "R2=(Vo-Vr3)/I2\n",
- "t=1/(2*f)\n",
- "V=UTP-(-LTP)\n",
- "C1=.1*10**-6\n",
- "I1=(C1*V)/t\n",
- "R1=Vo/I1\n",
- "\n",
- "#Results\n",
- "print(\"The value of R1 is %.2f kohm\" %(R1/1000))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "square wave generator\n",
- "The value of R1 is 70.00 kohm\n"
- ]
- }
- ],
- "prompt_number": 34
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.8 Page No 694"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math \n",
- "\n",
- "#initialisation of variables\n",
- "\n",
- "R1=2.2*10**3\n",
- "R2=2.7*10**3\n",
- "C2=.5*10**-6\n",
- "Vcc=15.0\n",
- "\n",
- "#Calculations\n",
- "t1=.693*C2*(R1+R2)\n",
- "t2=.693*C2*R2\n",
- "T=t1+t2\n",
- "f=1/T\n",
- "Ic1=(Vcc/3)/(R1+R2)\n",
- "\n",
- "#Results\n",
- "print(\"The value of Ic1 is %.2f mA\" %(Ic1*10**3))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "The value of Ic1 is 1.02 mA\n"
- ]
- }
- ],
- "prompt_number": 35
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.10 Page No 699"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "#initialisation of variables\n",
- "\n",
- "Vcc=9.0\n",
- "Vo=3\n",
- "I1=1.0*10**-3\n",
- "f=500.0\n",
- "UTP=3.0\n",
- "\n",
- "#Calculations\n",
- "print(\"design the triangular wave\")\n",
- "Vi=Vcc-1\n",
- "V=Vo-(-Vo)\n",
- "print(\" I1>>Ibmax for op-amp\")\n",
- "R1=Vi/I1\n",
- "t=1.0/(2*f)\n",
- "C1=(I1*t)/V\n",
- "print(\"schmitt design\")\n",
- "I2=1.0*10**-3\n",
- "R2=UTP/I2\n",
- "R3=(Vcc-1)/I2\n",
- "\n",
- "#Results\n",
- "print(\"The value of R3 is %.2f kohm\" %(R3/1000))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "design the triangular wave\n",
- " I1>>Ibmax for op-amp\n",
- "schmitt design\n",
- "The value of R3 is 8.00 kohm\n"
- ]
- }
- ],
- "prompt_number": 36
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.11 Page No 705"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "#initialisation of variables\n",
- "\n",
- "f=100.0*10**3\n",
- "Rs=1.5*10**3\n",
- "R1=2.0*Rs\n",
- "\n",
- "\n",
- "#Calculations\n",
- "R1=2.7*10**3#use standard value\n",
- "R2=R1+Rs\n",
- "C1=1/(2*3.14*f*R2)\n",
- "R4=R2\n",
- "R3=2*R4\n",
- "\n",
- "#Results\n",
- "print(\"The value of R3 is %.2f kohm\" %(R3/1000))"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- "The value of R3 is 8.40 kohm\n"
- ]
- }
- ],
- "prompt_number": 37
- },
- {
- "cell_type": "heading",
- "level": 2,
- "metadata": {},
- "source": [
- "Example 16.12, Page No 705"
- ]
- },
- {
- "cell_type": "code",
- "collapsed": false,
- "input": [
- "import math\n",
- "\n",
- "#initialisation of variables\n",
- "\n",
- "fs=1.0*10**6\n",
- "Rs=700.0\n",
- "C1=1000.0*10**-12\n",
- "C2=100.0*10**-12\n",
- "R1=1.0*10**6\n",
- "R2=10.0*10**3\n",
- "Rs=700.0\n",
- "Vdd=5\n",
- "\n",
- "#Calculations\n",
- "Ct=(C1*C2)/(C1+C2)\n",
- "print(\" at resonance Xl=Xct 2*pi*f*L=1/2*pi*f*Ct\")\n",
- "L=1/(((2*3.14*f)**2)*Ct)\n",
- "ip=Vdd/(R1+R2+Rs)\n",
- "Pd=(((.707*ip)**2)*Rs)*10**9\n",
- "\n",
- "#Results\n",
- "print(\" peak power dissipated is %.3fnW \" %Pd)"
- ],
- "language": "python",
- "metadata": {},
- "outputs": [
- {
- "output_type": "stream",
- "stream": "stdout",
- "text": [
- " at resonance Xl=Xct 2*pi*f*L=1/2*pi*f*Ct\n",
- " peak power dissipated is 8.563nW \n"
- ]
- }
- ],
- "prompt_number": 38
- }
- ],
- "metadata": {}
- }
- ]
-}
\ No newline at end of file |