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Fifth Edition, last update November 06, 2021

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Lessons In Electric Circuits, Volume III –SemiconductorsBy Tony R. KuphaldtFifth Edition, last update November 06, 2021

ic 2000-2021, Tony R. KuphaldtThis book is published under the terms and conditions of the Design Science License. Theseterms and conditions allow for free copying, distribution, and/or modification of this documentby the general public. The full Design Science License text is included in the last chapter.As an open and collaboratively developed text, this book is distributed in the hope thatit will be useful, but WITHOUT ANY WARRANTY; without even the implied warranty ofMERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the Design ScienceLicense for more details.Available in its entirety as part of the Open Book Project collection tsPRINTING HISTORY First Edition: Printed in June of 2000. Plain-ASCII illustrations for universal computerreadability. Second Edition: Printed in September of 2000. Illustrations reworked in standard graphic(eps and jpeg) format. Source files translated to Texinfo format for easy online and printedpublication. Third Edition: Printed in January 2002. Source files translated to SubML format. SubMLis a simple markup language designed to easily convert to other markups like LATEX,HTML, or DocBook using nothing but search-and-replace substitutions. Fourth Edition: Printed in December 2002. New sections added, and error correctionsmade, since third edition. Fith Edition: Printed in July 2007. New sections added, and error corrections made,format change.

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Contents1 AMPLIFIERS AND ACTIVE DEVICES1.1 From electric to electronic . . . . . . .1.2 Active versus passive devices . . . . .1.3 Amplifiers . . . . . . . . . . . . . . . .1.4 Amplifier gain . . . . . . . . . . . . . .1.5 Decibels . . . . . . . . . . . . . . . . .1.6 Absolute dB scales . . . . . . . . . . .1.7 Attenuators . . . . . . . . . . . . . . .11336814162 SOLID-STATE DEVICE THEORY2.1 Introduction . . . . . . . . . . . . . . . . . . . . . .2.2 Quantum physics . . . . . . . . . . . . . . . . . . .2.3 Valence and Crystal structure . . . . . . . . . . .2.4 Band theory of solids . . . . . . . . . . . . . . . . .2.5 Electrons and “holes” . . . . . . . . . . . . . . . . .2.6 The P-N junction . . . . . . . . . . . . . . . . . . .2.7 Junction diodes . . . . . . . . . . . . . . . . . . . .2.8 Bipolar junction transistors . . . . . . . . . . . . .2.9 Junction field-effect transistors . . . . . . . . . . .2.10 Insulated-gate field-effect transistors (MOSFET)2.11 Thyristors . . . . . . . . . . . . . . . . . . . . . . .2.12 Semiconductor manufacturing techniques . . . .2.13 Superconducting devices . . . . . . . . . . . . . . .2.14 Quantum devices . . . . . . . . . . . . . . . . . . .2.15 Semiconductor devices in SPICE . . . . . . . . . .Bibliography . . . . . . . . . . . . . . . . . . . . . . . . .27272841475055586065707375808391933 DIODES AND RECTIFIERS3.1 Introduction . . . . . . . .3.2 Meter check of a diode . .3.3 Diode ratings . . . . . . .3.4 Rectifier circuits . . . . .3.5 Peak detector . . . . . . .3.6 Clipper circuits . . . . . .9798103107108115117.iii.

CONTENTSiv3.7 Clamper circuits . . . . . . . .3.8 Voltage multipliers . . . . . . .3.9 Inductor commutating circuits3.10 Diode switching circuits . . . .3.11 Zener diodes . . . . . . . . . . .3.12 Special-purpose diodes . . . . .3.13 Other diode technologies . . . .3.14 SPICE models . . . . . . . . . .Bibliography . . . . . . . . . . . . . .1211231301321351431631631724 BIPOLAR JUNCTION TRANSISTORS4.1 Introduction . . . . . . . . . . . . . . .4.2 The transistor as a switch . . . . . . .4.3 Meter check of a transistor . . . . . .4.4 Active mode operation . . . . . . . . .4.5 The common-emitter amplifier . . . .4.6 The common-collector amplifier . . . .4.7 The common-base amplifier . . . . . .4.8 The cascode amplifier . . . . . . . . .4.9 Biasing techniques . . . . . . . . . . .4.10 Biasing calculations . . . . . . . . . .4.11 Input and output coupling . . . . . . .4.12 Feedback . . . . . . . . . . . . . . . . .4.13 Amplifier impedances . . . . . . . . .4.14 Current mirrors . . . . . . . . . . . . .4.15 Transistor ratings and packages . . .4.16 BJT quirks . . . . . . . . . . . . . . . .Bibliography . . . . . . . . . . . . . . . . . 732805 JUNCTION FIELD-EFFECT TRANSISTORS5.1 Introduction . . . . . . . . . . . . . . . . . . . .5.2 The transistor as a switch . . . . . . . . . . . .5.3 Meter check of a transistor . . . . . . . . . . .5.4 Active-mode operation . . . . . . . . . . . . . .5.5 The common-source amplifier – PENDING . .5.6 The common-drain amplifier – PENDING . .5.7 The common-gate amplifier – PENDING . . .5.8 Biasing techniques – PENDING . . . . . . . .5.9 Transistor ratings and packages – PENDING5.10 JFET quirks – PENDING . . . . . . . . . . . .2832832852882902993003003003013016 INSULATED-GATE FIELD-EFFECT TRANSISTORS6.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . .6.2 Depletion-type IGFETs . . . . . . . . . . . . . . . . .6.3 Enhancement-type IGFETs – PENDING . . . . . . .6.4 Active-mode operation – PENDING . . . . . . . . . .303303304313313

CONTENTS6.56.66.76.86.96.106.116.12vThe common-source amplifier – PENDING . .The common-drain amplifier – PENDING . .The common-gate amplifier – PENDING . . .Biasing techniques – PENDING . . . . . . . .Transistor ratings and packages – PENDINGIGFET quirks – PENDING . . . . . . . . . . .MESFETs – PENDING . . . . . . . . . . . . .IGBTs . . . . . . . . . . . . . . . . . . . . . . .7 THYRISTORS7.1 Hysteresis . . . . . . . . . . . . . . . .7.2 Gas discharge tubes . . . . . . . . . .7.3 The Shockley Diode . . . . . . . . . . .7.4 The DIAC . . . . . . . . . . . . . . . .7.5 The Silicon-Controlled Rectifier (SCR)7.6 The TRIAC . . . . . . . . . . . . . . .7.7 Optothyristors . . . . . . . . . . . . . .7.8 The Unijunction Transistor (UJT) . .7.9 The Silicon-Controlled Switch (SCS) .7.10 Field-effect-controlled thyristors . . .Bibliography . . . . . . . . . . . . . . . . . 3463523543568 OPERATIONAL AMPLIFIERS8.1 Introduction . . . . . . . . . . . . . . . .8.2 Single-ended and differential amplifiers8.3 The ”operational” amplifier . . . . . . .8.4 Negative feedback . . . . . . . . . . . .8.5 Divided feedback . . . . . . . . . . . . .8.6 An analogy for divided feedback . . . .8.7 Voltage-to-current signal conversion . .8.8 Averager and summer circuits . . . . .8.9 Building a differential amplifier . . . .8.10 The instrumentation amplifier . . . . .8.11 Differentiator and integrator circuits .8.12 Positive feedback . . . . . . . . . . . . .8.13 Practical considerations . . . . . . . . .8.14 Operational amplifier models . . . . . .8.15 Data . . . . . . . . . . . . . . . . . . . .3573573583623683713743803823843863873903944104159 PRACTICAL ANALOG SEMICONDUCTOR CIRCUITS9.1 ElectroStatic Discharge . . . . . . . . . . . . . . . . . .9.2 Power Supply circuits . . . . . . . . . . . . . . . . . . .9.3 Amplifier circuits – PENDING . . . . . . . . . . . . . .9.4 Oscillator circuits – INCOMPLETE . . . . . . . . . . .9.5 Phase-locked loops – PENDING . . . . . . . . . . . . .9.6 Radio circuits – INCOMPLETE . . . . . . . . . . . . . .417417423435435437437

CONTENTSvi9.7 Computational circuits . . . . . . . . . .9.8 Measurement circuits – INCOMPLETE9.9 Control circuits – PENDING . . . . . .Bibliography . . . . . . . . . . . . . . . . . . .44646746846810 ACTIVE FILTERS47110.1 Two pole active filters . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 47111 DC MOTOR DRIVES47311.1 Pulse Width Modulation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 47312 INVERTERS AND AC MOTOR DRIVES13 ELECTRON TUBES13.1 Introduction . . . . . . . . . .13.2 Early tube history . . . . . .13.3 The triode . . . . . . . . . . .13.4 The tetrode . . . . . . . . . .13.5 Beam power tubes . . . . . .13.6 The pentode . . . . . . . . . .13.7 Combination tubes . . . . . .13.8 Tube parameters . . . . . . .13.9 Ionization (gas-filled) tubes .13.10Display tubes . . . . . . . . .13.11Microwave tubes . . . . . . .13.12Tubes versus 97500503A-1 ABOUT THIS BOOK507A-2 CONTRIBUTOR LIST511A-3 CC BY License519INDEX522

Chapter 1AMPLIFIERS AND ACTIVEDEVICESContents1.11.21.31.41.51.61.71.1From electric to electronic . .Active versus passive devicesAmplifiers . . . . . . . . . . . . .Amplifier gain . . . . . . . . . .Decibels . . . . . . . . . . . . . .Absolute dB scales . . . . . . .Attenuators . . . . . . . . . . .1.7.1 Decibels . . . . . . . . . .1.7.2 T-section attenuator . . . .1.7.3 PI-section attenuator . . .1.7.4 L-section attenuator . . .1.7.5 Bridged T attenuator . . .1.7.6 Cascaded sections . . . .1.7.7 RF attenuators . . . . . .13368141617192021212323From electric to electronicThis third volume of the book series Lessons In Electric Circuits makes a departure from theformer two in that the transition between electric circuits and electronic circuits is formallycrossed. Electric circuits are connections of conductive wires and other devices whereby theuniform flow of electrons occurs. Electronic circuits add a new dimension to electric circuitsin that some means of control is exerted over the flow of electrons by another electrical signal,either a voltage or a current.1

CHAPTER 1. AMPLIFIERS AND ACTIVE DEVICES2In and of itself, the control of electron flow is nothing new to the student of electric circuits. Switches control the flow of electrons, as do potentiometers, especially when connectedas variable resistors (rheostats). Neither the switch nor the potentiometer should be new toyour experience by this point in your study. The threshold marking the transition from electricto electronic, then, is defined by how the flow of electrons is controlled rather than whether ornot any form of control exists in a circuit. Switches and rheostats control the flow of electronsaccording to the positioning of a mechanical device, which is actuated by some physical forceexternal to the circuit. In electronics, however, we are dealing with special devices able to control the flow of electrons according to another flow of electrons, or by the application of a staticvoltage. In other words, in an electronic circuit, electricity is able to control electricity.The historic precursor to the modern electronics era was invented by Thomas Edison in1880 while developing the electric incandescent lamp. Edison found that a small currentpassed from the heated lamp filament to a metal plate mounted inside the vacuum envelop.(Figure 1.1 (a)) Today this is known as the “Edison effect”. Note that the battery is only necessary to heat the filament. Electrons would still flow if a non-electrical heat source was used.controle-1e-1(a)(b)e-1 - (c)Figure 1.1: (a) Edison effect, (b) Fleming valve or vacuum diode, (c) DeForest audion triodevacuum tube amplifier.By 1904 Marconi Wireless Company adviser John Flemming found that an externally applied current (plate battery) only passed in one direction from filament to plate (Figure 1.1 (b)),but not the reverse direction (not shown). This invention was the vacuum diode, used to convert alternating currents to DC. The addition of a third electrode by Lee DeForest (Figure 1.1(c)) allowed a small signal to control the larger electron flow from filament to plate.Historically, the era of electronics began with the invention of the Audion tube, a devicecontrolling the flow of an electron stream through a vacuum by the application of a smallvoltage between two metal structures within the tube. A more detailed summary of so-calledelectron tube or vacuum tube technology is available in the last chapter of this volume for thosewho are interested.Electronics technology experienced a revolution in 1948 with the invention of the transistor. This tiny device achieved approximately the same effect as the Audion tube, but ina vastly smaller amount of space and with less material. Transistors control the flow of elec-

1.2. ACTIVE VERSUS PASSIVE DEVICES3trons through solid semiconductor substances rather than through a vacuum, and so transistortechnology is often referred to as solid-state electronics.1.2Active versus passive devicesAn active device is any type of circuit component with the ability to electrically control electronflow (electricity controlling electricity). In order for a circuit to be properly called electronic,it must contain at least one active device. Components incapable of controlling current bymeans of another electrical signal are called passive devices. Resistors, capacitors, inductors,transformers, and even diodes are all considered passive devices. Active devices include, butare not limited to, vacuum tubes, transistors, silicon-controlled rectifiers (SCRs), and TRIACs.A case might be made for the saturable reactor to be defined as an active device, since it is ableto control an AC current with a DC current, but I’ve never heard it referred to as such. Theoperation of each of these active devices will be explored in later chapters of this volume.All active devices control the flow of electrons through them. Some active devices allow avoltage to control this current while other active devices allow another current to do the job.Devices utilizing a static voltage as the controlling signal are, not surprisingly, called voltagecontrolled devices. Devices working on the principle of one current controlling another currentare known as current-controlled devices. For the record, vacuum tubes are voltage-controlleddevices while transistors are made as either voltage-controlled or current controlled types. Thefirst type of transistor successfully demonstrated was a current-controlled device.1.3AmplifiersThe practical benefit of active devices is their amplifying ability. Whether the device in question be voltage-controlled or current-controlled, the amount of power required of the controlling signal is typically far less than the amount of power available in the controlled current.In other words, an active device doesn’t just allow electricity to control electricity; it allows asmall amount of electricity to control a large amount of electricity.Because of this disparity between controlling and controlled powers, active devices may beemployed to govern a large amount of power (controlled) by the application of a small amountof power (controlling). This behavior is known as amplification.It is a fundamental rule of physics that energy can neither be created nor destroyed. Statedformally, this rule is known as the Law of Conservation of Energy, and no exceptions to it havebeen discovered to date. If this Law is true – and an overwhelming mass of experimental datasuggests that it is – then it is impossible to build a device capable of taking a small amount ofenergy and magically transforming it into a large amount of energy. All machines, electric andelectronic circuits included, have an upper efficiency limit of 100 percent. At best, power outequals power in as in Figure 1.2.Usually, machines fail even to meet this limit, losing some of their input energy in the formof heat which is radiated into surrounding space and therefore not part of the output energystream. (Figure 1.3)Many people have attempted, without success, to design and build machines that outputmore power than they take in. Not only would such a perpetual motion machine prove that the

CHAPTER 1. AMPLIFIERS AND ACTIVE DEVICES4PinputPerfect machineEfficiency PoutputPinputPoutput 1 100%Figure 1.2: The power output of a machine can approach, but never exceed, the power inputfor 100% efficiency as an upper limit.PinputRealistic machinePoutputPlost (usually waste heat)Efficiency PoutputPinput 1 less than 100%Figure 1.3: A realistic machine most often loses some of its input energy as heat in transforming it into the output energy stream.

1.3. AMPLIFIERS5Law of Conservation of Energy was not a Law after all, but it would usher in a technologicalrevolution such as the world has never seen, for it could power itself in a circular loop andgenerate excess power for “free”. (Figure 1.4)PinputPerpetual-motionmachineEfficiency PinputPoutputPinputPoutput 1 more than 100%Perpetual-motionmachineP"free"PoutputFigure 1.4: Hypothetical “perpetual motion machine” powers itself?Despite much effort and many unscrupulous claims of “free energy” or over-unity machines,not one has ever passed the simple test of powering itself with its own energy output andgenerating energy to spare.There does exist, however, a class of machines known as amplifiers, which are able to take insmall-power signals and output signals of much greater power. The key to understanding howamplifiers can exist without violating the Law of Conservation of Energy lies in the behaviorof active devices.Because active devices have the ability to control a large amount of electrical power with asmall amount of electrical power, they may be arranged in circuit so as to duplicate the formof the input signal power from a larger amount of power supplied by an external power source.The result is a device that appears to magically magnify the power of a small electrical signal(usually an AC voltage waveform) into an identically-shaped waveform of larger magnitude.The Law of Conservation of Energy is not violated because the additional power is suppliedby an external source, usually a DC battery or equivalent. The amplifier neither creates nordestroys energy, but merely reshapes it into the waveform desired as shown in Figure 1.5.In other words, the current-controlling behavior of active devices is employed to shape DCpower from the external power source into the same waveform as the input signal, producingan output signal of like shape but different (greater) power magnitude. The transistor or otheractive device within an amplifier merely forms a larger copy of the input signal waveform outof the “raw” DC power provided by a battery or other power source.Amplifiers, like all machines, are limited in efficiency to a maximum of 100 percent. Usually, electronic amplifiers are far less efficient than that, dissipating considerable amounts ofenergy in the form of waste heat. Because the efficiency of an amplifier is always 100 percent

CHAPTER 1. AMPLIFIERS AND ACTIVE DEVICES6Externalpower sourcePinputAmplifierPoutputFigure 1.5: While an amplifier can scale a small input signal to large output, its energy sourceis an external power supply.or less, one can never be made to function as a “perpetual motion” device.The requirement of an external source of power is common to all types of amplifiers, electrical and non-electrical. A common example of a non-electrical amplification system wouldbe power steering in an automobile, amplifying the power of the driver’s arms in turning thesteering wheel to move the front wheels of the car. The source of power necessary for the amplification comes from the engine. The active device controlling the driver’s “input signal” is ahydraulic valve shuttling fluid power from a pump attached to the engine to a hydraulic pistonassisting wheel motion. If the engine stops running, the amplification system fails to amplifythe driver’s arm power and the car becomes very difficult to turn.1.4Amplifier gainBecause amplifiers have the ability to increase the magnitude of an input signal, it is useful tobe able to rate an amplifier’s amplifying ability in terms of an output/input ratio. The technicalterm for an amplifier’s output/input magnitude ratio is gain. As a ratio of equal units (powerout / power in, voltage out / voltage in, or current out / current in), gain is naturally a unitlessmeasurement. Mathematically, gain is symbolized by the capital letter “A”.For example, if an amplifier takes in an AC voltage signal measuring 2 volts RMS andoutputs an AC voltage of 30 volts RMS, it has an AC voltage gain of 30 divided by 2, or 15:AV AV VoutputVinput30 V2VAV 15Correspondingly, if we know the gain of an amplifier and the magnitude of the input signal,we can calculate the magnitude of the output. For example, if an amplifier with an AC current

1.4. AMPLIFIER GAIN7gain of 3.5 is given an AC input signal of 28 mA RMS, the output will be 3.5 times 28 mA, or98 mA:Ioutput (AI)(Iinput)Ioutput (3.5)(28 mA)Ioutput 98 mAIn the last two examples I specifically identified the gains and signal magnitudes in termsof “AC.” This was intentional, and illustrates an important concept: electronic amplifiers oftenrespond differently to AC and DC input signals, and may amplify them to different extents.Another way of saying this is that amplifiers often amplify changes or variations in inputsignal magnitude (AC) at a different ratio than steady input signal magnitudes (DC). Thespecific reasons for this are too complex to explain at this time, but the fact of the matter isworth mentioning. If gain calculations are to be carried out, it must first be understood whattype of signals and gains are being dealt with, AC or DC.Electrical amplifier gains may be expressed in terms of voltage, current, and/or power, inboth AC and DC. A summary of gain definitions is as follows. The triangle-shaped “delta”symbol ( ) represents change in mathematics, so “ Voutput / Vinput ” means “change in outputvoltage divided by change in input voltage,” or more simply, “AC output voltage divided by ACinput voltage”:DC gainsVoltageAV CurrentAI AC gainsVoutputAV VinputIoutputAI IinputPoutputPowerAP PinputAP Voutput Vinput Ioutput Iinput( Voutput)( Ioutput)( Vinput)( Iinput)AP (AV)(AI) "change in . . ."If multiple amplifiers are staged, their respective gains form an overall gain equal to theproduct (multiplication) of the individual gains. (Figure 1.6) If a 1 V signal were applied to theinput of the gain of 3 amplifier in Figure 1.6 a 3 V signal out of the first amplifier would befurther amplified by a gain of 5 at the second stage yielding 15 V at the final output.

CHAPTER 1. AMPLIFIERS AND ACTIVE DEVICES8Input signalAmplifiergain 3Amplifiergain 5Output signalOverall gain (3)(5) 15Figure 1.6: The gain of a chain of cascaded amplifiers is the product of the individual gains.1.5DecibelsIn its simplest form, an amplifier’s gain is a ratio of output over input. Like all ratios, thisform of gain is unitless. However, there is an actual unit intended to represent gain, and it iscalled the bel.As a unit, the bel was actually devised as a convenient way to represent power loss in telephone system wiring rather than gain in amplifiers. The unit’s name is derived from Alexander Graham Bell, the famous Scottish inventor whose work was instrumental in developingtelephone systems. Originally, the bel represented the amount of signal power loss due to resistance over a standard length of electrical cable. Now, it is defined in terms of the common(base 10) logarithm of a power ratio (output power divided by input power):AP(ratio) PoutputPinputAP(Bel) logPoutputPinputBecause the bel is a logarithmic unit, it is nonlinear. To give you an idea of how this works,consider the following table of figures, comparing power losses and gains in bels versus simpleratios:Table: Gain / loss in belsLoss/gain asa ratioPoutputPinputLoss/gainin belsPoutputlogPinputLoss/gain asa ratioPoutputPinputLoss/gainin belsPoutputlogPinput10003B0.1-1 B1002B0.01-2 B101B0.001-3 B0B0.0001-4 B1(no loss or gain)It was later decided that the bel was too large of a unit to be used directly, and so it became

1.5. DECIBELS9customary to apply the metric prefix deci (meaning 1/10) to it, making it decibels, or dB. Now,the expression “dB” is so common that many people do not realize it is a combination of “deci-”and “-bel,” or that there even is such a unit as the “bel.” To put this into perspective, here isanother table contrasting power gain/loss ratios against decibels:Table: Gain / loss in decibelsLoss/gain asa ratioPoutputPinputLoss/gainin decibelsPoutput10 logPinputLoss/gain asa ratioPoutputPinputLoss/gainin decibelsPoutput10 logPinput100030 dB0.1-10 dB10020 dB0.01-20 dB1010 dB0.001-30 dB0 dB0.0001-40 dB1(no loss or gain)As a logarithmic unit, this mode of power gain expression covers a wide range of ratios witha minimal span in figures. It is reasonable to ask, “why did anyone feel the need to invent alogarithmic unit for electrical signal power loss in a telephone system?” The answer is relatedto the dynamics of human hearing, the perceptive intensity of which is logarithmic in nature.Human hearing is highly nonlinear: in order to double the perceived intensity of a sound,the actual sound power must be multiplied by a factor of ten. Relating telephone signal powerloss in terms of the logarithmic “bel” scale makes perfect sense in this context: a power loss of1 bel translates to a perceived sound loss of 50 percent, or 1/2. A power gain of 1 bel translatesto a doubling in the perceived intensity of the sound.An almost perfect analogy to the bel scale is the Richter scale used to describe earthquakeintensity: a 6.0 Richter earthquake is 10 times more powerful than a 5.0 Richter earthquake; a7.0 Richter earthquake 100 times more powerful than a 5.0 Richter earthquake; a 4.0 Richterearthquake is 1/10 as powerful as a 5.0 Richter earthquake, and so on. The measurementscale for chemical pH is likewise logarithmic, a difference of 1 on the scale is equivalent toa tenfold difference in hydrogen ion concentration of a chemical solution. An advantage ofusing a logarithmic measurement scale is the tremendous range of expression afforded by arelatively small span of numerical values, and it is this advantage which secures the use ofRichter numbers for earthquakes and pH for hydrogen ion activity.Another reason for the adoption of the bel as a unit for gain is for simple expression of system gains and losses. Consider the last system example (Figure 1.6) where two amplifiers wereconnected tandem to amplify a signal. The respective gain for each amplifier was expressed asa ratio, and the overall gain for the system was the product (multiplication) of those two ratios:Overall gain (3)(5) 15If these figures represented power gains, we could directly apply the unit of bels to the task

CHAPTER 1. AMPLIFIERS AND ACTIVE DEVICES10of representing the gain of each amplifier, and of the system altogether. (Figure 1.7)AP(Bel) log AP(ratio)Input signalAP(Bel) log 3AP(Bel) log 5Amplifiergain

1.1 From electric to electronic This third volume of the book series Lessons In Electric Circuits makes a departure from the former two in that the transition between electric circuits and electronic circuits is formally crossed. Electric circuits are connections of conductive wires and other devices whereby the uniform flow of electrons occurs.

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