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|
{
"cells": [
{
"cell_type": "markdown",
"metadata": {},
"source": [
"# Chapter 2 - Semiconductor Diodes"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 99 example 1"
]
},
{
"cell_type": "code",
"execution_count": 1,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"ratio of reverse saturation current = 4963.36\n"
]
}
],
"source": [
"q=0.01##centimetre\n",
"sigma1=1##ohm centimetre inverse\n",
"q1=0.01##centimetre\n",
"sigm11=0.01##ohm centimetre inverse\n",
"iratio=(0.0224**2*2.11*20)*3.6**2/((3.11*(4.3**2*10**-6)**2*2.6*20*10**3))#\n",
"for q in range(0,2):\n",
" if q==1:\n",
" un=3800#\n",
" up=1500#\n",
" q=1.6*10**-19#\n",
" ni=2.5*10#\n",
" else:\n",
" q=1.6*10**-19#\n",
" up=500\n",
" un=1300#\n",
" ni=1.5*10\n",
"\n",
" \n",
" b=un/up#\n",
" sigmai=(un+up)*q*ni#\n",
"\n",
"print \"ratio of reverse saturation current = %0.2f\"%((iratio))\n",
"##correction required in the book"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 100 example 2"
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"reverse current ratio = 7.79e-09\n"
]
}
],
"source": [
"sigma1=0.01##ohm centimetre inverse\n",
"area11=4*10**-3##metre square\n",
"q=0.01*10**-2##metre\n",
"un=1300.0#\n",
"up=500.0#\n",
"ni=1.5*10**15##per cubic centimetre\n",
"sigma1=(un+up)*1.6*10**-19*ni#\n",
"iratio=(4*10**-10*0.026*sigma1**2*2.6*2/10**-4)/3.6**2#\n",
"print \"reverse current ratio = %0.2e\"%((iratio))\n",
"##correction required in the book"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 100 example 3"
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"reverse saturation current = 3.48e-06 ampere\n"
]
}
],
"source": [
"a=4*10**-4##metre square\n",
"sigmap=1#\n",
"sigman=0.1#\n",
"de=0.15#\n",
"vtem=26*10**-3#\n",
"i=(a*vtem*((2.11)*(0.224))/((3.22)**(2)))*((1/de*sigman)+(1/de*sigmap))#\n",
"print \"reverse saturation current = %0.2e\"%(i),\"ampere\"#correction in the book"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 101 example 4"
]
},
{
"cell_type": "code",
"execution_count": 4,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"voltage at which the reverse saturation current at saturate = -0.06 volt\n",
"reverse saturation current = -6.84 ampere\n",
"reverse saturation current 0.10 = 0.000 ampere\n",
"reverse saturation current 0.20 = 0.022 ampere\n",
"reverse saturation current 0.30 = 1.026 ampere\n"
]
}
],
"source": [
"from math import log, exp\n",
"w=0.9#\n",
"voltaf=0.05##volt\n",
"revcur=10*10**-6##ampere\n",
"#(1) voltage\n",
"volrev=0.026*(log((-w+1)))##voltage at which the reverse saturation current at saturate\n",
"resacu=((exp(voltaf/0.026)-1)/((exp(-voltaf/0.026)-1)))##reverse saturation current\n",
"print \"voltage at which the reverse saturation current at saturate = %0.2f\"%((volrev)),\"volt\"\n",
"print \"reverse saturation current = %0.2f\"%((resacu)),\"ampere\"\n",
"u=0.1#\n",
"for q in range(0,3):\n",
" reverc=revcur*(exp((u/0.026))-1)\n",
" print \"reverse saturation current %0.2f\"%((u)),\" = %0.3f\"%((reverc)),\"ampere\"\n",
" u=u+0.1#\n"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 103 example 6"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"capacitance = 7.08e-11 farad\n"
]
}
],
"source": [
"a=1*10**-6##metre square\n",
"w=2*10**-6##thick centimetre\n",
"re=16#\n",
"eo=8.854*10**-12#\n",
"c=(eo*re*a)/w#\n",
"print \"capacitance = %0.2e\"%(c),\"farad\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 105 example 7"
]
},
{
"cell_type": "code",
"execution_count": 6,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"width of depletion layer at -10.00 = 7.73e-06 metre\n",
"width of depletion layer at -0.10 = 1.33e-06 metre\n",
"width of depletion layer at 0.10 = 7.65e-07 metre\n",
"capacitance at -10.00 = 1.57e-11 farad\n",
"capacitance at -0.10 = 9.13e-11 farad\n"
]
}
],
"source": [
"from math import sqrt\n",
"volbar=0.2##barrier voltage for germanium volt\n",
"na=3*10**20##atoms per metre\n",
"#(1) width of depletion layer at 10 and 0.1 volt\n",
"\n",
"for q in [-10, -0.1, 0.1]:\n",
" w=2.42*10**-6*sqrt((0.2-(q)))#\n",
" print \"width of depletion layer at %0.2f\"%((q)),\" = %0.2e\"%((w)),\"metre\"#for -0.1volt correction in the book\n",
"\n",
"#(d) capacitance\n",
"for q in [-10, -0.1]:\n",
" capaci=0.05*10**-9/sqrt(0.2-q)#\n",
" print \"capacitance at %0.2f\"%((q)),\" = %0.2e\"%((capaci)),\"farad\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 104 example 8"
]
},
{
"cell_type": "code",
"execution_count": 7,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"maximum forward current = 2.22 ampere\n",
"forward diode resistance = 0.40 ohm\n"
]
}
],
"source": [
"p=2##watts\n",
"voltaf=900*10**-3##volt\n",
"i1=p/voltaf#\n",
"r1=voltaf/i1#\n",
"print \"maximum forward current = %0.2f\"%(i1),\"ampere\"\n",
"\n",
"\n",
"print \"forward diode resistance = %0.2f\"%(r1),\"ohm\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 108 example 11"
]
},
{
"cell_type": "code",
"execution_count": 8,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"alpha = 104.86 degree\n"
]
}
],
"source": [
"from math import atan, degrees\n",
"r=250##ohm\n",
"c=40*10**-6##farad\n",
"alpha1=180-degrees(atan(377*r*c))\n",
"print \"alpha = %0.2f\"%(alpha1),\"degree\" "
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 109 example 12"
]
},
{
"cell_type": "code",
"execution_count": 9,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"inductance = 3022899.27 henry\n",
"output voltage = 31.03 volt\n"
]
}
],
"source": [
"from math import sqrt\n",
"i1=0.1##current in ampere\n",
"vms=40##rms voltage in volts\n",
"c=40*10**-6##capacitance in farad\n",
"r1=50##resistance in ohms\n",
"ripple=0.0001#\n",
"induct=((1.76/c)*sqrt(0.472/ripple))##inductance\n",
"outv=(2*sqrt(2)*vms)/3.14-i1*r1##output voltage\n",
"print \"inductance = %0.2f\"%(induct),\"henry\"#correction in the book\n",
"print \"output voltage = %0.2f\"%(outv),\"volt\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 109 example 14"
]
},
{
"cell_type": "code",
"execution_count": 10,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"ripple voltage = 0.093 volt\n",
"ripple voltage including filters = 118.49 volt\n",
"ripple voltage = 0.0040 volt\n"
]
}
],
"source": [
"from math import sqrt\n",
"voltag=40##volt\n",
"i1=0.2##ampere\n",
"c1=40*10**-6##farad\n",
"c2=c1#\n",
"induct=2##henry\n",
"#(1) ripple\n",
"vdc=2*sqrt(2)*voltag/3.14#\n",
"r1=vdc/i1#\n",
"induc1=r1/1130#\n",
"v1=voltag/(3*3.14**3*120**2*4*induct*c1)#\n",
"print \"ripple voltage = %0.3f\"%((v1)),\"volt\"\n",
"#(2) with two filter\n",
"v1=4*voltag/((3*3.14**5)*(16*120**2*induct**2*c1**2))#\n",
"print \"ripple voltage including filters = %0.2f\"%((v1)),\"volt\"#correction in the book\n",
"#(3)ripple voltage\n",
"v1=4*voltag/(5*3.14*1.414*2*3.14*240*240*3.14*induct*c1)#\n",
"v1=v1/20#\n",
"print \"ripple voltage = %0.4f\"%((v1)),\"volt\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 111 example 15"
]
},
{
"cell_type": "code",
"execution_count": 11,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"voltage and ripple with load\n",
"vdc = 250.21 volt\n",
"ripple = 3.13e-02\n",
"capacitance connected across load\n",
"vdc = 497.91 volt\n",
"ripple = 3.76e-02\n",
"filter containing two inductors and capacitors in parallel\n",
"vdc = 250.00 volt\n",
"ripple = 6.48e-04\n",
"two filter\n",
"vdc = 250.00 volt\n",
"ripple = 4.76e-06\n",
"vdc = 358.26 volt\n",
"ripple = 1.61e-04\n"
]
}
],
"source": [
"from __future__ import division\n",
"from math import sqrt\n",
"voltag=375##volt\n",
"r1=2000##ohm\n",
"induct=20##henry\n",
"c1=16*10**-6##farad\n",
"r11=100##ohm\n",
"r=200##ohm\n",
"#(1) voltage and ripple with load\n",
"print \"voltage and ripple with load\"\n",
"r=r+r11+400#\n",
"vdc=((2*sqrt(2)*voltag/3.14))/1.35#\n",
"ripple=r1/(3*sqrt(2)*(377)*induct*2)#\n",
"print \"vdc = %0.2f\"%((vdc)),\"volt\"\n",
"print \"ripple = %0.2e\"%((ripple))\n",
"#(2) capacitance connected across load\n",
"print \"capacitance connected across load\"\n",
"vdc=sqrt(2)*voltag/(1+1/(4*(60)*r1*2*c1))#\n",
"ripple=1/(4*sqrt(3)*(60)*r1*2*c1)#\n",
"print \"vdc = %0.2f\"%((vdc)),\"volt\"\n",
"print \"ripple = %0.2e\"%((ripple))\n",
"#(3) filter containing two inductors and capacitors in parallel\n",
"print \"filter containing two inductors and capacitors in parallel\"\n",
"vdc=250##volt\n",
"ripple=0.83*10**-6/(2*induct*2*c1)##correction in the book\n",
"print \"vdc = %0.2f\"%((vdc)),\"volt\"\n",
"print \"ripple = %0.2e\"%((ripple))\n",
"#(4) two filter\n",
"print \"two filter\"\n",
"vdc=250#\n",
"ripple=sqrt(2)/(3*16*3.14**2*60**2*induct*c1)**2##correction in the book\n",
"print \"vdc = %0.2f\"%((vdc)),\"volt\"\n",
"print \"ripple = %0.2e\"%((ripple))\n",
"vdc=sqrt(2)*voltag/(1+(4170/(r1*16))+(r/r1))#\n",
"ripple=3300/(16**2*2*20*r1)#\n",
"print \"vdc = %0.2f\"%((vdc)),\"volt\"\n",
"print \"ripple = %0.2e\"%((ripple))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 112 example 16"
]
},
{
"cell_type": "code",
"execution_count": 12,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"output voltage = 362.14 volt\n",
"ripple voltage = 1.46e-03\n"
]
}
],
"source": [
"from math import sqrt\n",
"capaci=4##farad\n",
"induct=20##henry\n",
"i1=50*10**-3##ampere\n",
"resist=200##ohm\n",
"maxvol=300*sqrt(2)#\n",
"vdc=maxvol-((4170/capaci)*(i1))-(i1*resist)#\n",
"ripple=(3300*i1)/((capaci**2)*(induct)*353)#\n",
"print \"output voltage = %0.2f\"%((vdc)),\"volt\"\n",
"print \"ripple voltage = %0.2e\"%((ripple))"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 113 example 17"
]
},
{
"cell_type": "code",
"execution_count": 13,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"inductance of filter = 4.98 henry\n",
"resistance of filter = 250.00 ohm\n"
]
}
],
"source": [
"from math import sqrt\n",
"voltag=25##volt\n",
"c1=10*10**-6##farad\n",
"i1=100*10**-3##ampere\n",
"ripple=0.001#\n",
"w=754##radians\n",
"#(1) inductance and resistance\n",
"\n",
"\n",
"r1=voltag/i1#\n",
"induct=40/(sqrt(2)*w**2*(c1))#\n",
"print \"inductance of filter = %0.2f\"%((induct)),\"henry\"#correction in the book\n",
"print \"resistance of filter = %0.2f\"%((r1)),\"ohm\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 113 example 18"
]
},
{
"cell_type": "code",
"execution_count": 14,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"current = 2.83e-04 ampere\n",
"current at 100celsius rise\n",
"current = 6.81e-04 ampere\n"
]
}
],
"source": [
"from math import exp\n",
"resacu=0.1*10**-12##ampere\n",
"u=20+273##kelvin\n",
"voltaf=0.55##volt\n",
"w=1.38*10**-23#\n",
"q=1.6*10**-19#\n",
"for z in range(1,3):\n",
" if z==2 :\n",
" u=100+273#\n",
" print \"current at 100celsius rise\"\n",
" \n",
" voltag=w*u/q#\n",
" i1=(10**-13)*(exp((voltaf/voltag))-1)#\n",
" if z==2:\n",
" i1=(256*10**-13)*((exp(voltaf/voltag)-1))#\n",
" \n",
" print \"current = %0.2e\"%((i1)),\"ampere\"\n"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 114 example 19"
]
},
{
"cell_type": "code",
"execution_count": 15,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"thermal voltage = 0.026 volt\n",
"barrier voltage = 0.535 volt\n"
]
}
],
"source": [
"from math import log\n",
"na=10*22##atoms per cubic metre\n",
"nd=1.2*10**21##donor per cubic metre\n",
"voltag=1.38*10**-23*(273+298)/(1.6*10**-19)##correction in the book\n",
"voltag=0.026#\n",
"ni=1.5*10**16#\n",
"ni=ni**2#\n",
"v1=voltag*log((na*nd)/(ni))#\n",
"print \"thermal voltage = %0.3f\"%((voltag)),\"volt\"\n",
"print \"barrier voltage = %0.3f\"%(abs(v1)),\"volt\"#correction in the book"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 114 example 20"
]
},
{
"cell_type": "code",
"execution_count": 16,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"current = 9.16e-06 ampere\n"
]
}
],
"source": [
"from math import exp\n",
"i1=2*10**-7##ampere\n",
"voltag=0.026##volt\n",
"i=i1*((exp(0.1/voltag)-1))#\n",
"print \"current = %0.2e\"%((i)),\"ampere\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 115 example 21"
]
},
{
"cell_type": "code",
"execution_count": 17,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"resistance at 150mvolt = 80.74 ohm\n"
]
}
],
"source": [
"from math import exp\n",
"resacu=1*10**-6##ampere\n",
"voltaf=150*10**-3##volt\n",
"w=8.62*10**-5#\n",
"voltag=0.026##volt\n",
"u=300##kelvin\n",
"uw=u*w#\n",
"resist=(uw)/((resacu)*exp(voltaf/voltag))#\n",
"print \"resistance at 150mvolt = %0.2f\"%((resist)),\"ohm\"#correction in the book"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 115 example 22"
]
},
{
"cell_type": "code",
"execution_count": 18,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"change in barrier = 0.18 volt\n"
]
}
],
"source": [
"from math import log\n",
"dopfac=1000#\n",
"w=300##kelvin\n",
"q=0.026*log(dopfac)#\n",
"print \"change in barrier = %0.2f\"%((q)),\"volt\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 116 example 23"
]
},
{
"cell_type": "code",
"execution_count": 19,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"depletion capacitance = 1.09e-11 farad\n",
"capacitance = 3.85e-07 farad\n"
]
}
],
"source": [
"from math import sqrt\n",
"area12=1*10**-8##metre square\n",
"volre1=-1##reverse voltage\n",
"capac1=5*10**-12##farad\n",
"volbu1=0.9##volt\n",
"voltag=0.5##volt\n",
"i1=10*10**-3##ampere\n",
"durmin=1*10**-6##ssecond\n",
"#(1) capacitance\n",
"capac1=capac1*sqrt((volre1-volbu1)/(voltag-volbu1))#\n",
"print \"depletion capacitance = %0.2e\"%((capac1)),\"farad\"\n",
"#(2) capacitance\n",
"capac1=i1*durmin/(0.026)#\n",
"\n",
"print \"capacitance = %0.2e\"%((capac1)),\"farad\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 116 example 24"
]
},
{
"cell_type": "code",
"execution_count": 20,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"potential germanium = 0.34 volt\n",
"potential silicon = 0.74 volt\n"
]
}
],
"source": [
"from math import log\n",
"quantg=4*10**22##atoms per cubic centimetre\n",
"quants=5*10**22##atoms per cubic centimetre\n",
"w=2.5*10**13##per cubic centimetre\n",
"w1=1.5*10**10##per cubic centimetre\n",
"for q in [quantg, quants]:\n",
" na=2*q/(10**8)\n",
" nd=500*na#\n",
" if q==quantg :\n",
" w=w#\n",
" voltag=0.026*log(na*nd/w**2)#\n",
" print \"potential germanium = %0.2f\"%((voltag)),\"volt\"\n",
" \n",
" if q==quants:\n",
" w=w1#\n",
" voltag=0.026*log(na*nd/w**2)#\n",
" print \"potential silicon = %0.2f\"%((voltag)),\"volt\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## PageNumber 117 example 25"
]
},
{
"cell_type": "code",
"execution_count": 21,
"metadata": {
"collapsed": false
},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
"electrons density = 9.62e+20 per cubic metre\n",
"holes density = 1.25e+23 per cubic metre\n"
]
}
],
"source": [
"u=0.05##metre square per velocity second correction in the book\n",
"un=0.13##metre square per velocity second\n",
"condun=20##second per metre conductivity of n region\n",
"condup=1000##second per metre conductivity of p region\n",
"p=condup/(1.6*10**-19*u)#\n",
"no=condun/(1.6*10**-19*un)#\n",
"print \"electrons density = %0.2e\"%((no)),\"per cubic metre\"\n",
"print \"holes density = %0.2e\"%((p)),\"per cubic metre\"#others to find is not in the book"
]
}
],
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"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"
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|