The document provides solutions to various problems involving the analysis and design of transistor amplifiers and power supplies. It examines concepts such as maximum power transfer, voltage gain, efficiency, heat dissipation, and voltage/current characteristics. Diagrams and calculations are presented to determine operating voltages and currents, power outputs, temperature rises, and efficiency for different circuit configurations under varying conditions.
This document contains solutions to exercises from Chapter 8. The summaries are:
1) The first exercise calculates the maximum power transfer for a common emitter amplifier circuit under different voltage supply conditions.
2) The second exercise calculates temperature increases for different components in a circuit based on power dissipation.
3) The third exercise similarly calculates temperature rises for different components based on known power and thermal resistances.
This document contains solutions to problems from Chapter 11. Problem 11.1 solves for resistances in a common emitter amplifier circuit. Part c) finds the maximum and minimum voltages. Problem 11.2 calculates the common-mode gain of a differential amplifier as -0.01012. Problem 11.3a) solves for currents and voltages in a multi-emitter transistor. Part b) solves for currents when the collector voltage is changed.
This document provides solutions to example problems from Chapter 11 of an electronics textbook.
The problems cover topics such as: transistor biasing circuits, common emitter amplifier configurations, determining voltage and current values, and calculating resistor values needed for specific circuit behaviors. Detailed calculations are shown for each example problem to derive the requested values.
The document is from a solutions manual for a power electronics textbook. It provides step-by-step solutions to example problems from Chapter 2 on power semiconductor diodes and circuits and Chapter 3 on diode rectifiers. The problems cover topics like calculating diode voltage and current characteristics, analyzing diode circuits, designing rectifier circuits, and calculating output voltages and currents for various rectifier configurations.
This document contains solutions to problems involving BJT amplifier circuit analysis. Problem 6.1 calculates key transistor parameters like transconductance (gm) and output resistance (ro) for two common-emitter amplifiers. Problem 6.2 repeats this calculation for different bias currents. Subsequent problems analyze additional amplifier circuits, determining voltage gains and component values needed to meet specified conditions. Calculations involve setting up and solving equations relating bias currents, voltages, transistor parameters and circuit resistances.
This document contains the solutions to various exercises related to circuit analysis and electronics. Exercise problems cover topics such as diode circuits, rectifiers, filters, and transistor circuits. The solutions involve calculating voltages, currents, power, capacitance values, and other circuit parameters through applying circuit laws and relationships. PSpice simulations are also used to verify some of the circuit responses.
This document contains solutions to 15 exercises related to circuit analysis. The exercises calculate values like capacitance, resistance, cutoff frequency, and gain based on given circuit diagrams and specifications. Equations are set up and solved to find the desired values. For example, exercise 1 calculates the capacitance needed for a given RC circuit to have a cutoff frequency of 40 kHz. The solutions proceed methodically through each problem, showing the work to arrive at the final answers.
1) The document provides solved problems related to power electronics circuits involving thyristors, inverters, and commutation circuits.
2) Problem 9.1 calculates the capacitance needed for a series RLC load to achieve zero current switching for SCRs in a single-phase bridge inverter.
3) Problem 9.2 checks if a self-commutated SCR circuit will reliably commutate when triggered from zero voltage, and calculates voltages and current derivative at the time of commutation.
This document contains solutions to exercises from Chapter 8. The summaries are:
1) The first exercise calculates the maximum power transfer for a common emitter amplifier circuit under different voltage supply conditions.
2) The second exercise calculates temperature increases for different components in a circuit based on power dissipation.
3) The third exercise similarly calculates temperature rises for different components based on known power and thermal resistances.
This document contains solutions to problems from Chapter 11. Problem 11.1 solves for resistances in a common emitter amplifier circuit. Part c) finds the maximum and minimum voltages. Problem 11.2 calculates the common-mode gain of a differential amplifier as -0.01012. Problem 11.3a) solves for currents and voltages in a multi-emitter transistor. Part b) solves for currents when the collector voltage is changed.
This document provides solutions to example problems from Chapter 11 of an electronics textbook.
The problems cover topics such as: transistor biasing circuits, common emitter amplifier configurations, determining voltage and current values, and calculating resistor values needed for specific circuit behaviors. Detailed calculations are shown for each example problem to derive the requested values.
The document is from a solutions manual for a power electronics textbook. It provides step-by-step solutions to example problems from Chapter 2 on power semiconductor diodes and circuits and Chapter 3 on diode rectifiers. The problems cover topics like calculating diode voltage and current characteristics, analyzing diode circuits, designing rectifier circuits, and calculating output voltages and currents for various rectifier configurations.
This document contains solutions to problems involving BJT amplifier circuit analysis. Problem 6.1 calculates key transistor parameters like transconductance (gm) and output resistance (ro) for two common-emitter amplifiers. Problem 6.2 repeats this calculation for different bias currents. Subsequent problems analyze additional amplifier circuits, determining voltage gains and component values needed to meet specified conditions. Calculations involve setting up and solving equations relating bias currents, voltages, transistor parameters and circuit resistances.
This document contains the solutions to various exercises related to circuit analysis and electronics. Exercise problems cover topics such as diode circuits, rectifiers, filters, and transistor circuits. The solutions involve calculating voltages, currents, power, capacitance values, and other circuit parameters through applying circuit laws and relationships. PSpice simulations are also used to verify some of the circuit responses.
This document contains solutions to 15 exercises related to circuit analysis. The exercises calculate values like capacitance, resistance, cutoff frequency, and gain based on given circuit diagrams and specifications. Equations are set up and solved to find the desired values. For example, exercise 1 calculates the capacitance needed for a given RC circuit to have a cutoff frequency of 40 kHz. The solutions proceed methodically through each problem, showing the work to arrive at the final answers.
1) The document provides solved problems related to power electronics circuits involving thyristors, inverters, and commutation circuits.
2) Problem 9.1 calculates the capacitance needed for a series RLC load to achieve zero current switching for SCRs in a single-phase bridge inverter.
3) Problem 9.2 checks if a self-commutated SCR circuit will reliably commutate when triggered from zero voltage, and calculates voltages and current derivative at the time of commutation.
1) The document contains solved examples related to diode circuits and characteristics. It examines diode behavior in rectifier circuits, transfer characteristics, and modeling.
2) Key concepts covered include the voltage and current relationships of ideal and exponential diode models, as well as the small-signal resistance parameter rd.
3) Methods like iteration and exponential equations are used to solve for voltage and current in circuits containing single or multiple diodes.
This document contains a sample multiple choice question (MCQ) exam for electronics and communication engineering. It includes 15 sample questions related to basic electrical concepts such as current, voltage, resistance, capacitance and circuits. It also provides the solutions and explanations for each question. The document is from a book titled "GATE EC by RK Kanodia" which is intended to help students prepare for the graduate aptitude test in engineering exam for electronics and communication.
Here are the steps to verify this circuit:
1) Identify branches that do not adhere to the passive sign convention: branches with voltages and currents of the same sign. These are the 3 V, 3 A branch and the -2 V, -4 A branch.
2) For branches that adhere to the passive sign convention, calculate power as voltage × current. For non-passive branches, calculate power as -voltage × current.
3) Sum the powers for each branch:
- (3 V)(3 A) = -9 W (non-passive)
- (-2 V)(-4 A) = 8 W (non-passive)
- (5 V)(2 A) = 10 W
1) This document discusses alternating current (AC) circuits and includes problems involving capacitors and inductors in AC circuits.
2) It covers key concepts like reactance, time constants, and calculating current, voltage, charge and inductance in circuits containing resistors, capacitors, inductors and AC sources.
3) Many problems involve calculating values after a certain time or frequency using the equations for RC circuits, RL circuits and reactance of capacitors and inductors.
This document provides solved problems from GATE (Graduate Aptitude Test in Engineering) exams from 1996-2013 in the subject of Engineering Mathematics. It contains one-mark and two-mark questions related to topics like differential equations, matrices, probability, complex analysis etc. along with their solutions. The document is available for purchase in digital format at www.nodia.co.in in separate sections or 'units'.
This document provides an errata listing corrections to errors found in the 6th edition of the textbook "Introduction to Electric Circuits" by R.C. Dorf and J.A. Svoboda. The errata is organized by chapter and page number and provides corrections to issues such as incorrect equations, figures, answers to problems, and typos or grammatical errors in the text. A link is also provided to access the errata online which contains additional corrections not listed in the printed document.
[E book] introduction to electric circuits 6th ed [r. c. dorf and j. a. svoboda]tensasparda
This document provides an errata listing corrections to errors found in the 6th edition of the textbook "Introduction to Electric Circuits" by R.C. Dorf and J.A. Svoboda. The errata is organized by chapter and page number and provides corrections to issues such as incorrect equations, figures, answers to problems, and textual errors. A link is also provided to access the errata online which contains additional corrections not listed in the printed document.
The document contains solutions to example problems from Chapter 17 of an exercise book. Problem EX17.1 involves calculating currents in a circuit with a voltage source and two resistors. Part a calculates the currents with different input voltages. Part b calculates the node voltages. EX17.2 calculates power dissipation for a logic gate circuit with different input voltages.
This document contains the answers to a 30 question multiple choice network theory test taken on June 10, 2017. The answers are provided in a numbered list from 1 to 30 without the corresponding questions. An answer key for the test is also included which provides the answers. The document aims to provide the answers to a network theory test for a student.
This document contains sample problems and solutions related to semiconductor physics. Problem EX1.1 calculates intrinsic carrier concentrations ni for GaAs, Ge, and Si at 300K using the intrinsic carrier concentration equation. Problem EX1.2 calculates minority and majority carrier concentrations. Problem EX1.3 calculates drift current density in n-type material.
This document summarizes Chapter 1 from the textbook "Electrical Engineering: Principles and Applications" by Allan R. Hambley. It includes sample exercises and problems from Chapter 1 on topics like charge, current, voltage, power, energy, circuits, and circuit analysis techniques. The chapter introduces fundamental concepts of electrical engineering.
Problemas del Laboratorio N°1 de Física IIguestf39ed9c1
This chapter discusses electric current, Ohm's law, power and heat loss, resistivity, and the temperature coefficient of resistance. Key points include:
- Ohm's law relates current, voltage, and resistance. It is used to calculate current, charge, time, voltage, power, and resistance in various circuits.
- Power is the rate at which electrical energy is transferred by a current. It is calculated using Power = Current x Voltage.
- Resistivity is a material's inherent resistance to conducting an electric current. It is used along with length and cross-sectional area to calculate resistance of wires.
- Resistance of conductors increases with temperature based on their temperature coefficient of resist
This document contains solutions to 10 exercises involving bipolar junction transistors and MOSFET circuits. The key points summarized are:
1) Exercise 10.1 calculates the reference and base currents in a BJT circuit. Exercise 10.2 calculates the reference current, zero bias current, and small signal output resistance.
2) Exercise 10.3 calculates the various currents in a multi-emitter BJT. Exercise 10.4 calculates the early effect resistance and voltage difference between two BJTs.
3) Exercise 10.5 again calculates reference current and zero bias current. Exercises 10.6 through 10.11 involve various MOSFET and BJT circuit calculations.
This document summarizes key concepts about capacitance from a physics textbook chapter:
1) It defines capacitance and provides examples of calculating the charge stored on metal spheres and capacitors of various geometries using the capacitance formula.
2) It explains how to calculate the capacitance of parallel plate capacitors using the capacitance equation and defines key terms like dielectric strength.
3) It demonstrates how to analyze circuits involving capacitors connected in series and parallel, including calculating equivalent capacitance and charge/voltage across individual capacitors.
This document summarizes key concepts from Chapter 24 of a physics textbook on electric fields.
1) It provides examples of calculating electric field intensity (E) given force (F) on a charge (q) or vice versa.
2) It explains how to find the resultant electric field (ER) between two or more charges using vector addition.
3) It introduces Gauss's law and shows how it can be used to calculate E outside a charged sphere or hollow sphere.
PROBLEMAS RESUELTOS (42) DE LABORATORIO N° 1 DE FÍSICA II - TIPPENSLUIS POWELL
This document summarizes key concepts and formulas related to electric current, resistance, and Ohm's law from a physics textbook chapter. It includes:
- Formulas for calculating current, charge, resistance, voltage, power, and energy from given values.
- Examples of applying the formulas to calculate values in electric circuits.
- Concepts of resistivity and how resistance changes with temperature based on the material's temperature coefficient of resistance.
Gate 2013 complete solutions of ec electronics and communication engineeringmanish katara
The document is a sample paper for GATE 2013 that contains 25 multiple choice questions related to engineering topics like logic gates, vector fields, impulse response of systems, diodes, IC technology, and more. Each question is followed by a brief explanation of the answer. The questions cover a range of fundamental concepts in areas like signals and systems, electronics, semiconductor devices, and mathematics.
This document provides 30 problems related to calculating forces and torques in magnetic fields. It covers topics like calculating torque on loops and coils using the torque formula, determining required currents and magnetic field strengths, and converting galvanometers into voltmeters and ammeters by adding resistances. The problems involve setting up and solving equations for torque, current, resistance, and magnetic field based on given parameters like loop/coil area, number of turns, angle with the magnetic field, and desired deflection or measurement values.
1) The document contains examples of calculations for MOSFET circuit analysis, including determining operating point values like I_D, V_GS, and g_m.
2) Equations are provided and used to solve for transistor parameters like threshold voltage, transconductance, and output resistance.
3) Circuit examples include common source, common gate, and common drain configurations to determine voltage gain and output resistance.
This document contains solutions to exercises from Chapter 4. The summaries are:
1) Exercise 4.1 calculates the transconductance (gm) and output resistance (ro) for a MOSFET with given parameters.
2) Exercise 4.2 calculates the voltage gain (Av) of a common-source amplifier using the gm from Exercise 4.1.
3) Exercise 4.3 calculates various voltage and current values for a common-source amplifier using given resistor values. It also calculates the voltage gain (Av) of the amplifier.
This document contains solutions to various circuit analysis problems. Problem 2.1 solves for the output voltage of a voltage divider circuit given input and resistor values. Problem 2.2 analyzes a circuit with a diode and calculates the output voltage as a function of the input voltage and diode characteristics. The remaining problems continue analyzing circuits involving resistors, diodes, capacitors and calculating values such as output voltage, current, power dissipation and more. Equations are provided and used to solve for unknown variables in each circuit.
1) The document contains solved examples related to diode circuits and characteristics. It examines diode behavior in rectifier circuits, transfer characteristics, and modeling.
2) Key concepts covered include the voltage and current relationships of ideal and exponential diode models, as well as the small-signal resistance parameter rd.
3) Methods like iteration and exponential equations are used to solve for voltage and current in circuits containing single or multiple diodes.
This document contains a sample multiple choice question (MCQ) exam for electronics and communication engineering. It includes 15 sample questions related to basic electrical concepts such as current, voltage, resistance, capacitance and circuits. It also provides the solutions and explanations for each question. The document is from a book titled "GATE EC by RK Kanodia" which is intended to help students prepare for the graduate aptitude test in engineering exam for electronics and communication.
Here are the steps to verify this circuit:
1) Identify branches that do not adhere to the passive sign convention: branches with voltages and currents of the same sign. These are the 3 V, 3 A branch and the -2 V, -4 A branch.
2) For branches that adhere to the passive sign convention, calculate power as voltage × current. For non-passive branches, calculate power as -voltage × current.
3) Sum the powers for each branch:
- (3 V)(3 A) = -9 W (non-passive)
- (-2 V)(-4 A) = 8 W (non-passive)
- (5 V)(2 A) = 10 W
1) This document discusses alternating current (AC) circuits and includes problems involving capacitors and inductors in AC circuits.
2) It covers key concepts like reactance, time constants, and calculating current, voltage, charge and inductance in circuits containing resistors, capacitors, inductors and AC sources.
3) Many problems involve calculating values after a certain time or frequency using the equations for RC circuits, RL circuits and reactance of capacitors and inductors.
This document provides solved problems from GATE (Graduate Aptitude Test in Engineering) exams from 1996-2013 in the subject of Engineering Mathematics. It contains one-mark and two-mark questions related to topics like differential equations, matrices, probability, complex analysis etc. along with their solutions. The document is available for purchase in digital format at www.nodia.co.in in separate sections or 'units'.
This document provides an errata listing corrections to errors found in the 6th edition of the textbook "Introduction to Electric Circuits" by R.C. Dorf and J.A. Svoboda. The errata is organized by chapter and page number and provides corrections to issues such as incorrect equations, figures, answers to problems, and typos or grammatical errors in the text. A link is also provided to access the errata online which contains additional corrections not listed in the printed document.
[E book] introduction to electric circuits 6th ed [r. c. dorf and j. a. svoboda]tensasparda
This document provides an errata listing corrections to errors found in the 6th edition of the textbook "Introduction to Electric Circuits" by R.C. Dorf and J.A. Svoboda. The errata is organized by chapter and page number and provides corrections to issues such as incorrect equations, figures, answers to problems, and textual errors. A link is also provided to access the errata online which contains additional corrections not listed in the printed document.
The document contains solutions to example problems from Chapter 17 of an exercise book. Problem EX17.1 involves calculating currents in a circuit with a voltage source and two resistors. Part a calculates the currents with different input voltages. Part b calculates the node voltages. EX17.2 calculates power dissipation for a logic gate circuit with different input voltages.
This document contains the answers to a 30 question multiple choice network theory test taken on June 10, 2017. The answers are provided in a numbered list from 1 to 30 without the corresponding questions. An answer key for the test is also included which provides the answers. The document aims to provide the answers to a network theory test for a student.
This document contains sample problems and solutions related to semiconductor physics. Problem EX1.1 calculates intrinsic carrier concentrations ni for GaAs, Ge, and Si at 300K using the intrinsic carrier concentration equation. Problem EX1.2 calculates minority and majority carrier concentrations. Problem EX1.3 calculates drift current density in n-type material.
This document summarizes Chapter 1 from the textbook "Electrical Engineering: Principles and Applications" by Allan R. Hambley. It includes sample exercises and problems from Chapter 1 on topics like charge, current, voltage, power, energy, circuits, and circuit analysis techniques. The chapter introduces fundamental concepts of electrical engineering.
Problemas del Laboratorio N°1 de Física IIguestf39ed9c1
This chapter discusses electric current, Ohm's law, power and heat loss, resistivity, and the temperature coefficient of resistance. Key points include:
- Ohm's law relates current, voltage, and resistance. It is used to calculate current, charge, time, voltage, power, and resistance in various circuits.
- Power is the rate at which electrical energy is transferred by a current. It is calculated using Power = Current x Voltage.
- Resistivity is a material's inherent resistance to conducting an electric current. It is used along with length and cross-sectional area to calculate resistance of wires.
- Resistance of conductors increases with temperature based on their temperature coefficient of resist
This document contains solutions to 10 exercises involving bipolar junction transistors and MOSFET circuits. The key points summarized are:
1) Exercise 10.1 calculates the reference and base currents in a BJT circuit. Exercise 10.2 calculates the reference current, zero bias current, and small signal output resistance.
2) Exercise 10.3 calculates the various currents in a multi-emitter BJT. Exercise 10.4 calculates the early effect resistance and voltage difference between two BJTs.
3) Exercise 10.5 again calculates reference current and zero bias current. Exercises 10.6 through 10.11 involve various MOSFET and BJT circuit calculations.
This document summarizes key concepts about capacitance from a physics textbook chapter:
1) It defines capacitance and provides examples of calculating the charge stored on metal spheres and capacitors of various geometries using the capacitance formula.
2) It explains how to calculate the capacitance of parallel plate capacitors using the capacitance equation and defines key terms like dielectric strength.
3) It demonstrates how to analyze circuits involving capacitors connected in series and parallel, including calculating equivalent capacitance and charge/voltage across individual capacitors.
This document summarizes key concepts from Chapter 24 of a physics textbook on electric fields.
1) It provides examples of calculating electric field intensity (E) given force (F) on a charge (q) or vice versa.
2) It explains how to find the resultant electric field (ER) between two or more charges using vector addition.
3) It introduces Gauss's law and shows how it can be used to calculate E outside a charged sphere or hollow sphere.
PROBLEMAS RESUELTOS (42) DE LABORATORIO N° 1 DE FÍSICA II - TIPPENSLUIS POWELL
This document summarizes key concepts and formulas related to electric current, resistance, and Ohm's law from a physics textbook chapter. It includes:
- Formulas for calculating current, charge, resistance, voltage, power, and energy from given values.
- Examples of applying the formulas to calculate values in electric circuits.
- Concepts of resistivity and how resistance changes with temperature based on the material's temperature coefficient of resistance.
Gate 2013 complete solutions of ec electronics and communication engineeringmanish katara
The document is a sample paper for GATE 2013 that contains 25 multiple choice questions related to engineering topics like logic gates, vector fields, impulse response of systems, diodes, IC technology, and more. Each question is followed by a brief explanation of the answer. The questions cover a range of fundamental concepts in areas like signals and systems, electronics, semiconductor devices, and mathematics.
This document provides 30 problems related to calculating forces and torques in magnetic fields. It covers topics like calculating torque on loops and coils using the torque formula, determining required currents and magnetic field strengths, and converting galvanometers into voltmeters and ammeters by adding resistances. The problems involve setting up and solving equations for torque, current, resistance, and magnetic field based on given parameters like loop/coil area, number of turns, angle with the magnetic field, and desired deflection or measurement values.
1) The document contains examples of calculations for MOSFET circuit analysis, including determining operating point values like I_D, V_GS, and g_m.
2) Equations are provided and used to solve for transistor parameters like threshold voltage, transconductance, and output resistance.
3) Circuit examples include common source, common gate, and common drain configurations to determine voltage gain and output resistance.
This document contains solutions to exercises from Chapter 4. The summaries are:
1) Exercise 4.1 calculates the transconductance (gm) and output resistance (ro) for a MOSFET with given parameters.
2) Exercise 4.2 calculates the voltage gain (Av) of a common-source amplifier using the gm from Exercise 4.1.
3) Exercise 4.3 calculates various voltage and current values for a common-source amplifier using given resistor values. It also calculates the voltage gain (Av) of the amplifier.
This document contains solutions to various circuit analysis problems. Problem 2.1 solves for the output voltage of a voltage divider circuit given input and resistor values. Problem 2.2 analyzes a circuit with a diode and calculates the output voltage as a function of the input voltage and diode characteristics. The remaining problems continue analyzing circuits involving resistors, diodes, capacitors and calculating values such as output voltage, current, power dissipation and more. Equations are provided and used to solve for unknown variables in each circuit.
This document provides specifications for an N-channel MOSFET transistor.
The transistor has a drain-source voltage rating of 650V, can handle up to 7A of continuous drain current, and has low on-resistance and fast switching times.
Tables provide information on maximum ratings, electrical characteristics, and dimensions for the TO-220 package variants. Graphs illustrate characteristics like safe operating area, thermal resistance over time, and diode recovery behavior.
1) The document contains example problems from Chapter 6 of a textbook on exercise problems involving BJT circuit analysis.
2) Problem EX6.1 involves calculating currents, voltages, and gain for a common-emitter amplifier.
3) Problem EX6.12 involves calculating the bias resistor values needed to produce a specified quiescent current and voltage for a common-emitter amplifier.
The document contains solutions to 20 example problems (labeled EX5.1 through EX5.20) relating to bipolar junction transistors. Each problem involves calculating various transistor parameters such as bias currents, voltages, and resistor values given information such as supply voltages, transistor betas, and resistor/collector resistor values. The problems cover topics such as calculating bias points, determining operating modes, and designing transistor circuits.
This document provides the electrical characteristics, maximum ratings, and package dimensions for the S TM4433A P-channel enhancement mode field effect transistor. Key specifications include:
- Drain-source voltage rating of -30V
- Continuous drain current of 2.5A and pulsed drain current of 6A
- On-resistance of 35mOhm at VGS=-10V and 55mOhm at VGS=-4.5V
- Surface mount SO-8 package with a junction-to-ambient thermal resistance of 50°C/W
This document contains solutions to problems related to MOSFET circuits. Section 16.1 calculates threshold voltage shift for an n-channel MOSFET under different gate-source voltages. Section 16.2 determines transistor parameters from output characteristics. Section 16.3 finds the transistor operating point for a different load resistance. Sections 16.4 through 16.9 solve additional problems involving MOSFET biasing, power calculations, and logic gate output voltages.
This document provides specifications for the CD4532BMS CMOS 8-Bit Priority Encoder integrated circuit, including:
- Absolute maximum ratings and operating conditions.
- Electrical performance characteristics such as supply current, input/output voltages and currents, propagation delays, and input capacitance over operating temperature and voltage ranges.
- Reliability and quality assurance information such as thermal resistance and junction temperature limits.
- Package information and a brief description of the priority encoding functionality.
Original IGBT IRG4BC20KD G4BC20KD 600V 9A TO-220 NewAUTHELECTRONIC
This document provides specifications for an insulated gate bipolar transistor (IGBT) with an integrated ultrafast soft recovery diode. It lists maximum ratings, electrical characteristics, switching characteristics, and thermal characteristics for the device. Key parameters include a collector-emitter voltage of 600V, continuous collector current ratings of 16A and 9A, and ultrafast switching times below 100ns. Graphs illustrate characteristics such as output curves, gate charge, and switching losses. The document also contains a test circuit diagram and waveform definitions for evaluating the device performance.
Original N-Channel Mosfet R6020ANX 6020 600V 20A TO-220 New ROHM SemiconductorAUTHELECTRONIC
1) This document provides specifications for the R6020ANX Nch 600V 20A Power MOSFET, including absolute maximum ratings, electrical characteristics, and typical curves.
2) The MOSFET features low on-resistance of 0.22Ω maximum, fast switching speed, simple drive circuits, and easy parallel use.
3) Key parameters include a 600V drain-source breakdown voltage, 20A continuous drain current rating, and ±30V maximum gate-source voltage range.
Original N-Channel Mosfet IRF2907ZPBF 2907 75V 170A TO-220 New IRAUTHELECTRONIC
Original N-Channel Mosfet IRF2907ZPBF 2907 75V 170A TO-220 New IR
https://authelectronic.com/original-n-channel-mosfet-irf2907zpbf-2907-75v-170a-to-220-new-ir
This document provides specifications for an Advanced Power N-CHANNEL ENHANCEMENT MODE POWER MOSFET. It has a low on-resistance of 9mΩ, simple drive requirements, and fast switching characteristics with a continuous drain current of 57A. The MOSFET is RoHS compliant, halogen-free, and has a maximum drain-source voltage of 25V. It comes in the TO-252 surface mount package.
Original P-Channel Mosfet MDD3752RH 3752 43A 40V TO-252 New MagnaChip Semicon...AUTHELECTRONIC
This document provides specifications for the MDD3752 P-channel trench MOSFET from MagnaChip Semiconductor. Some key details include:
- Absolute maximum ratings of -40V for drain-source voltage, ±20V for gate-source voltage, and continuous drain current of -43A at 25°C and -27A at 100°C.
- Electrical characteristics including a drain-source breakdown voltage of -40V, gate threshold voltage between -1V to -3V, and on-resistance below 17mΩ at -10V gate voltage.
- The device features a trench gate structure for low on-resistance and fast switching. It is packaged in a
Original IGBT IRFR4615TRLPBF IRFR4615 4615 150V 33A TO-252 New IRAUTHELECTRONIC
The document summarizes the benefits, applications, and specifications of HEXFET® Power MOSFETs. Key benefits include improved gate, avalanche and switching ruggedness as well as enhanced body diode performance. Applications include high efficiency synchronous rectification in switch-mode power supplies, uninterruptible power supplies, and high-speed power switching circuits. The document provides detailed maximum ratings, electrical characteristics, and switching performance curves over temperature for the IRFR4615PbF and IRFU4615PbF MOSFETs.
Original N-CHANNEL MOSFET SPP20N60C3 20N60C3 20N60 20A 600V TO-220 New Infine...AUTHELECTRONIC
This document provides specifications for CoolMOSTM power transistors. Key specifications include:
- An RDS(on) of 0.19 Ohms, continuous drain current of 20.7A, and 650V maximum VDS at a junction temperature of 125C.
- World's lowest RDS(on) for a TO-220 packaged transistor. Features include high voltage, current and switching speed capabilities.
- Electrical characteristics are provided such as threshold voltage, on-resistance, transconductance, capacitances and switching times. Safe operating curves, thermal performance and application information are also included.
Electronic devices and circuit theory 11th copyKitTrnTun5
This document contains significant equations and concepts related to electronic devices and circuits. Some key points include:
- Semiconductor diode equations including the relationship between voltage, current, and temperature.
- Bipolar junction transistor equations for current, voltage, power, and biasing configurations.
- Field effect transistor equations for current, voltage, power, and biasing configurations.
- Operational amplifier applications including inverting, non-inverting, summing amplifiers.
- Feedback and oscillator circuit concepts such as the Barkhausen criteria for oscillation.
Original IGBT RJH60D2DPP RJH60D2 12A 600V TO-220 New RenesasAUTHELECTRONIC
This document provides preliminary datasheet information for the RJH60D2DPP-M0 600V-12A IGBT module. Key specifications include a short circuit withstand time of 5us, low 1.7V saturation voltage, and 100ns diode reverse recovery time. The module uses trench gate and thin wafer technology for high speed switching under 80ns. It has a TO-220FL package and can withstand temperatures up to 150°C.
Original IGBT FGP20N60 20N60 FGP20N60UFD 20A 600V TO-220 NewAUTHELECTRONIC
This document provides specifications and performance characteristics for the FGP20N60UFD 600V, 20A Field Stop IGBT from Fairchild Semiconductor. The IGBT has a maximum collector-emitter voltage of 600V, continuous collector current rating of 20A, and pulsed collector current rating of 60A. Key specifications and characteristics include maximum ratings, thermal characteristics, electrical characteristics of the IGBT and diode, switching characteristics, and typical performance curves. The document also provides mechanical dimensions and packaging information for the TO-220 packaged device.
Rameysoft-ftp client server, and others+Bilal Sarwar
Ramey Soft provides software consulting services to assist clients with software design, strategy, tools, and processes in order to ensure project and product success. Their expertise includes web services, database design, web development, management systems, desktop and Android application development, and programming languages such as Java, ASP.net, C/C++, PHP, C#, SQL, and MySQL. They also provide counseling for graduate and post-graduate projects and aim to transform data into knowledge to help clients solve problems and better serve customers. Contact details are provided for Skype, email, and phone numbers.
Ramey Soft provides software consulting services to assist clients with software design, strategy, tools, and processes in order to ensure project and product success. Their services go beyond just coding to transform data into knowledge and help clients solve problems and better serve customers. They offer expertise in web services, database design, web development, management systems, desktop and Android application development, and programming languages like Java, ASP.net, C/C++, PHP, C#, SQL, and MySQL.
Ramey Soft provides software consulting services to assist clients with software design, strategy, tools, and processes in order to ensure project and product success. Their expertise includes web services, database design, web and desktop application development, and management systems for various industries. They also provide counseling for graduate and post-graduate projects, with the goal of transforming data into knowledge to help clients solve problems and better serve customers. Ramey Soft can be contacted via email, Skype, or phone for web development, database design, and application development services in languages like Java, ASP.NET, C/C++, PHP, C#, and technologies like SQL, MySQL, and graphics.
This document contains the solutions to exercises from Chapter 16. The first exercise solves for the threshold voltage (VTN) of a NMOS transistor. The second exercise calculates the output voltage and current of a common source amplifier. The third exercise analyzes the output characteristics of an inverter. The remaining exercises involve additional circuit analysis problems related to topics in Chapter 16 such as CMOS inverters, logic gates and power calculations.
This document contains solutions to problems from Chapter 15. It provides detailed calculations and examples for various circuit analysis problems involving filters. Some key points:
- It calculates transfer functions, corner frequencies, and component values for low-pass filters, high-pass filters, and bandpass filters.
- It determines the number of poles needed in a filter to achieve a given attenuation level.
- It analyzes the transfer function of a maximally flat high-pass filter and derives the relationship between component values.
- It provides an example of designing a circuit to meet given low-frequency and high-frequency gain specifications using an op-amp.
The document demonstrates analytical techniques for analyzing and designing passive filter
This document contains solutions to problems from Chapter 14. Problem 14.1 calculates the maximum and rms input voltages for a circuit. Problem 14.2 calculates output current and minimum load resistance. Problem 14.3 lists voltage values for another circuit. Problem 14.4 calculates closed-loop gain. The remaining problems involve calculating various voltage and current values, closed-loop gains, and input and feedback resistances for multiple stage amplifier circuits using provided equations. Lengthy calculations are shown for some problems.
This document contains solutions to exercises from Chapter 14. The solutions involve calculations for amplifier circuits using op amp specifications like gain bandwidth, input offset voltage, input bias current, slew rate, and more. Some key results include:
- The input offset voltage for a circuit is calculated as 1.27 mV.
- The input resistance of a voltage follower circuit with a large resistor is calculated as 5000 MΩ.
- The maximum frequency of a circuit before the gain drops by 3 dB is calculated as 20 kHz.
This document contains solutions to problems in Chapter 13 regarding computer simulations and analyses of bipolar junction transistor circuits. The key points summarized are:
1) Problem 13.1 provides a computer simulation of a circuit and calculates the overall gain as -1.59x106.
2) Problem 13.6 calculates various currents in a BJT reference circuit, including the reference current of 0.5 mA and collector current of 21.1 μA.
3) Problem 13.8 calculates currents in another BJT reference circuit, including the reference current of 0.22 mA, collector current of 14.2 μA, and other node currents.
This document contains solutions to exercises from Chapter 13. The solutions involve calculating various currents and voltages in BJT amplifier circuits. Equations are provided and values are calculated for currents, voltages, gains, and other circuit parameters. Detailed steps are shown for each calculation.
This document contains solutions to problems from Chapter 12. It provides detailed calculations and explanations for problems involving feedback amplifiers, frequency response, input and output impedances, and circuit configurations. Key points addressed include:
- Calculating voltage gain, feedback factor, and input/output impedances for various amplifier circuits.
- Deriving frequency response expressions and bandwidth calculations.
- Determining circuit types based on input/output impedance characteristics.
- Solving for voltage and current variables in feedback amplifier circuits.
This document contains solutions to examples from Chapter 12 of an exercise book. It includes 12 examples covering topics like:
1) Calculating voltage gain, input resistance, and output resistance of non-inverting op-amps.
2) Analyzing the bandwidth, voltage gain, and input/output resistances of inverting op-amps.
3) Determining the voltage transfer characteristics, transconductance, and voltage gain of BJT common emitter amplifiers.
The examples provide step-by-step workings and calculations to arrive at the key parameters and specifications for different amplifier circuit configurations.
1) This document provides solutions to problems involving bipolar junction transistors. It analyzes various circuit configurations to determine values like current, voltage, and resistance.
2) Key steps involve writing equations for the relationships between currents, applying Kirchhoff's laws, and solving the equations simultaneously to find the unknown values.
3) The analysis considers factors like the effect of beta on collector and base currents, and how resistance values must be set for desired output currents and voltages.
This document contains solutions to problems from Chapter 9. It provides worked examples of calculating voltages and currents in circuits containing operational amplifiers. Key steps and results are shown for multiple circuit configurations, including calculating voltage gains, identifying resistor values, and determining output voltages and currents given input signals. Operational amplifier circuits with one, two and multiple stages are analyzed using relevant equations.
The document contains solutions to example problems from Chapter 9 of an exercise book.
The examples calculate resistor values for circuits involving operational amplifiers to achieve specified voltage gains, current values, and time constants. Computer analysis examples also calculate output voltages and currents for various input conditions in operational amplifier circuits.
This document summarizes solutions to problems involving circuit analysis using Laplace transforms.
1) The first problem analyzes a simple RC circuit and calculates the transfer function, cutoff frequency, and output response to a step input.
2) The second problem analyzes a similar RC circuit with different component values and calculates the transfer function and cutoff frequency.
3) Additional circuit examples are provided involving resistors, capacitors, and inductors. Transfer functions are derived and cutoff frequencies are calculated.
4) A multiple time constant circuit is analyzed and its frequency response is characterized.
5) Circuits involving operational amplifiers are analyzed to derive transfer functions and calculate bandwidth parameters.
This document contains solutions to exercises from Chapter 7. The exercises involve analyzing RC circuits, operational amplifiers, and transistors. The solutions calculate values like capacitance, frequency response, gain, and bias points by setting up and solving equations that model the circuit behavior. Circuit diagrams are included with some of the solutions. The exercises cover topics like low-pass filters, amplifiers, and basic transistor circuits.
This document contains solutions to problems involving BJT circuit analysis. Key points include:
1) Problem 5.1 analyzes two common emitter amplifier circuits and calculates currents and voltages.
2) Problem 5.2 calculates alpha and collector current values for two common emitter circuits with different beta values.
3) The remaining problems involve calculating various parameter values like currents, voltages, and gains for additional common emitter, common base, and common collector BJT circuits. Circuit analysis methods like Kirchhoff's laws and transistor biasing equations are applied.
4) Graphs and calculations of operating points are presented for some circuits. Effects of component value variations are considered, such as the impact on collector
This document provides solutions to problems involving MOSFET circuit analysis, calculating current (ID) and other parameters using equations that relate gate voltage (VGS), drain voltage (VDS), threshold voltage (VT), and transconductance (Kn or Kp) for n-channel or p-channel MOSFETs. Various regions of operation are considered including saturation, cut-off, and non-saturation. Worked examples calculate ID for different bias conditions and device parameters such as width (W) and length (L).
How to Get CNIC Information System with Paksim Ga.pptxdanishmna97
Pakdata Cf is a groundbreaking system designed to streamline and facilitate access to CNIC information. This innovative platform leverages advanced technology to provide users with efficient and secure access to their CNIC details.
In the rapidly evolving landscape of technologies, XML continues to play a vital role in structuring, storing, and transporting data across diverse systems. The recent advancements in artificial intelligence (AI) present new methodologies for enhancing XML development workflows, introducing efficiency, automation, and intelligent capabilities. This presentation will outline the scope and perspective of utilizing AI in XML development. The potential benefits and the possible pitfalls will be highlighted, providing a balanced view of the subject.
We will explore the capabilities of AI in understanding XML markup languages and autonomously creating structured XML content. Additionally, we will examine the capacity of AI to enrich plain text with appropriate XML markup. Practical examples and methodological guidelines will be provided to elucidate how AI can be effectively prompted to interpret and generate accurate XML markup.
Further emphasis will be placed on the role of AI in developing XSLT, or schemas such as XSD and Schematron. We will address the techniques and strategies adopted to create prompts for generating code, explaining code, or refactoring the code, and the results achieved.
The discussion will extend to how AI can be used to transform XML content. In particular, the focus will be on the use of AI XPath extension functions in XSLT, Schematron, Schematron Quick Fixes, or for XML content refactoring.
The presentation aims to deliver a comprehensive overview of AI usage in XML development, providing attendees with the necessary knowledge to make informed decisions. Whether you’re at the early stages of adopting AI or considering integrating it in advanced XML development, this presentation will cover all levels of expertise.
By highlighting the potential advantages and challenges of integrating AI with XML development tools and languages, the presentation seeks to inspire thoughtful conversation around the future of XML development. We’ll not only delve into the technical aspects of AI-powered XML development but also discuss practical implications and possible future directions.
Cosa hanno in comune un mattoncino Lego e la backdoor XZ?Speck&Tech
ABSTRACT: A prima vista, un mattoncino Lego e la backdoor XZ potrebbero avere in comune il fatto di essere entrambi blocchi di costruzione, o dipendenze di progetti creativi e software. La realtà è che un mattoncino Lego e il caso della backdoor XZ hanno molto di più di tutto ciò in comune.
Partecipate alla presentazione per immergervi in una storia di interoperabilità, standard e formati aperti, per poi discutere del ruolo importante che i contributori hanno in una comunità open source sostenibile.
BIO: Sostenitrice del software libero e dei formati standard e aperti. È stata un membro attivo dei progetti Fedora e openSUSE e ha co-fondato l'Associazione LibreItalia dove è stata coinvolta in diversi eventi, migrazioni e formazione relativi a LibreOffice. In precedenza ha lavorato a migrazioni e corsi di formazione su LibreOffice per diverse amministrazioni pubbliche e privati. Da gennaio 2020 lavora in SUSE come Software Release Engineer per Uyuni e SUSE Manager e quando non segue la sua passione per i computer e per Geeko coltiva la sua curiosità per l'astronomia (da cui deriva il suo nickname deneb_alpha).
HCL Notes and Domino License Cost Reduction in the World of DLAUpanagenda
Webinar Recording: https://www.panagenda.com/webinars/hcl-notes-and-domino-license-cost-reduction-in-the-world-of-dlau/
The introduction of DLAU and the CCB & CCX licensing model caused quite a stir in the HCL community. As a Notes and Domino customer, you may have faced challenges with unexpected user counts and license costs. You probably have questions on how this new licensing approach works and how to benefit from it. Most importantly, you likely have budget constraints and want to save money where possible. Don’t worry, we can help with all of this!
We’ll show you how to fix common misconfigurations that cause higher-than-expected user counts, and how to identify accounts which you can deactivate to save money. There are also frequent patterns that can cause unnecessary cost, like using a person document instead of a mail-in for shared mailboxes. We’ll provide examples and solutions for those as well. And naturally we’ll explain the new licensing model.
Join HCL Ambassador Marc Thomas in this webinar with a special guest appearance from Franz Walder. It will give you the tools and know-how to stay on top of what is going on with Domino licensing. You will be able lower your cost through an optimized configuration and keep it low going forward.
These topics will be covered
- Reducing license cost by finding and fixing misconfigurations and superfluous accounts
- How do CCB and CCX licenses really work?
- Understanding the DLAU tool and how to best utilize it
- Tips for common problem areas, like team mailboxes, functional/test users, etc
- Practical examples and best practices to implement right away
Why You Should Replace Windows 11 with Nitrux Linux 3.5.0 for enhanced perfor...SOFTTECHHUB
The choice of an operating system plays a pivotal role in shaping our computing experience. For decades, Microsoft's Windows has dominated the market, offering a familiar and widely adopted platform for personal and professional use. However, as technological advancements continue to push the boundaries of innovation, alternative operating systems have emerged, challenging the status quo and offering users a fresh perspective on computing.
One such alternative that has garnered significant attention and acclaim is Nitrux Linux 3.5.0, a sleek, powerful, and user-friendly Linux distribution that promises to redefine the way we interact with our devices. With its focus on performance, security, and customization, Nitrux Linux presents a compelling case for those seeking to break free from the constraints of proprietary software and embrace the freedom and flexibility of open-source computing.
Full-RAG: A modern architecture for hyper-personalizationZilliz
Mike Del Balso, CEO & Co-Founder at Tecton, presents "Full RAG," a novel approach to AI recommendation systems, aiming to push beyond the limitations of traditional models through a deep integration of contextual insights and real-time data, leveraging the Retrieval-Augmented Generation architecture. This talk will outline Full RAG's potential to significantly enhance personalization, address engineering challenges such as data management and model training, and introduce data enrichment with reranking as a key solution. Attendees will gain crucial insights into the importance of hyperpersonalization in AI, the capabilities of Full RAG for advanced personalization, and strategies for managing complex data integrations for deploying cutting-edge AI solutions.
Removing Uninteresting Bytes in Software FuzzingAftab Hussain
Imagine a world where software fuzzing, the process of mutating bytes in test seeds to uncover hidden and erroneous program behaviors, becomes faster and more effective. A lot depends on the initial seeds, which can significantly dictate the trajectory of a fuzzing campaign, particularly in terms of how long it takes to uncover interesting behaviour in your code. We introduce DIAR, a technique designed to speedup fuzzing campaigns by pinpointing and eliminating those uninteresting bytes in the seeds. Picture this: instead of wasting valuable resources on meaningless mutations in large, bloated seeds, DIAR removes the unnecessary bytes, streamlining the entire process.
In this work, we equipped AFL, a popular fuzzer, with DIAR and examined two critical Linux libraries -- Libxml's xmllint, a tool for parsing xml documents, and Binutil's readelf, an essential debugging and security analysis command-line tool used to display detailed information about ELF (Executable and Linkable Format). Our preliminary results show that AFL+DIAR does not only discover new paths more quickly but also achieves higher coverage overall. This work thus showcases how starting with lean and optimized seeds can lead to faster, more comprehensive fuzzing campaigns -- and DIAR helps you find such seeds.
- These are slides of the talk given at IEEE International Conference on Software Testing Verification and Validation Workshop, ICSTW 2022.
Goodbye Windows 11: Make Way for Nitrux Linux 3.5.0!SOFTTECHHUB
As the digital landscape continually evolves, operating systems play a critical role in shaping user experiences and productivity. The launch of Nitrux Linux 3.5.0 marks a significant milestone, offering a robust alternative to traditional systems such as Windows 11. This article delves into the essence of Nitrux Linux 3.5.0, exploring its unique features, advantages, and how it stands as a compelling choice for both casual users and tech enthusiasts.
Programming Foundation Models with DSPy - Meetup SlidesZilliz
Prompting language models is hard, while programming language models is easy. In this talk, I will discuss the state-of-the-art framework DSPy for programming foundation models with its powerful optimizers and runtime constraint system.
GraphSummit Singapore | The Art of the Possible with Graph - Q2 2024Neo4j
Neha Bajwa, Vice President of Product Marketing, Neo4j
Join us as we explore breakthrough innovations enabled by interconnected data and AI. Discover firsthand how organizations use relationships in data to uncover contextual insights and solve our most pressing challenges – from optimizing supply chains, detecting fraud, and improving customer experiences to accelerating drug discoveries.
Let's Integrate MuleSoft RPA, COMPOSER, APM with AWS IDP along with Slackshyamraj55
Discover the seamless integration of RPA (Robotic Process Automation), COMPOSER, and APM with AWS IDP enhanced with Slack notifications. Explore how these technologies converge to streamline workflows, optimize performance, and ensure secure access, all while leveraging the power of AWS IDP and real-time communication via Slack notifications.
Maruthi Prithivirajan, Head of ASEAN & IN Solution Architecture, Neo4j
Get an inside look at the latest Neo4j innovations that enable relationship-driven intelligence at scale. Learn more about the newest cloud integrations and product enhancements that make Neo4j an essential choice for developers building apps with interconnected data and generative AI.
Unlock the Future of Search with MongoDB Atlas_ Vector Search Unleashed.pdfMalak Abu Hammad
Discover how MongoDB Atlas and vector search technology can revolutionize your application's search capabilities. This comprehensive presentation covers:
* What is Vector Search?
* Importance and benefits of vector search
* Practical use cases across various industries
* Step-by-step implementation guide
* Live demos with code snippets
* Enhancing LLM capabilities with vector search
* Best practices and optimization strategies
Perfect for developers, AI enthusiasts, and tech leaders. Learn how to leverage MongoDB Atlas to deliver highly relevant, context-aware search results, transforming your data retrieval process. Stay ahead in tech innovation and maximize the potential of your applications.
#MongoDB #VectorSearch #AI #SemanticSearch #TechInnovation #DataScience #LLM #MachineLearning #SearchTechnology
Infrastructure Challenges in Scaling RAG with Custom AI modelsZilliz
Building Retrieval-Augmented Generation (RAG) systems with open-source and custom AI models is a complex task. This talk explores the challenges in productionizing RAG systems, including retrieval performance, response synthesis, and evaluation. We’ll discuss how to leverage open-source models like text embeddings, language models, and custom fine-tuned models to enhance RAG performance. Additionally, we’ll cover how BentoML can help orchestrate and scale these AI components efficiently, ensuring seamless deployment and management of RAG systems in the cloud.
Observability Concepts EVERY Developer Should Know -- DeveloperWeek Europe.pdfPaige Cruz
Monitoring and observability aren’t traditionally found in software curriculums and many of us cobble this knowledge together from whatever vendor or ecosystem we were first introduced to and whatever is a part of your current company’s observability stack.
While the dev and ops silo continues to crumble….many organizations still relegate monitoring & observability as the purview of ops, infra and SRE teams. This is a mistake - achieving a highly observable system requires collaboration up and down the stack.
I, a former op, would like to extend an invitation to all application developers to join the observability party will share these foundational concepts to build on:
Dr. Sean Tan, Head of Data Science, Changi Airport Group
Discover how Changi Airport Group (CAG) leverages graph technologies and generative AI to revolutionize their search capabilities. This session delves into the unique search needs of CAG’s diverse passengers and customers, showcasing how graph data structures enhance the accuracy and relevance of AI-generated search results, mitigating the risk of “hallucinations” and improving the overall customer journey.
1. Chapter 8
Problem Solutions
8.1
a.
b. i. VD D = 80 V
VD D
Maximum power at VDS = = 40 V
2
PT 25
ID = = = 0.625 A
VD S 40
80 − 40
RD = ⇒ RD = 64 Ω
0.625
ii. VD D = 50 V
VD D
Maximum power at VD S = = 25 V
2
PT 25
ID = = =1 A
VDS 25
50 − 25
RD = ⇒ RD = 25 Ω
1
8.2
a.
2. VC C
PQ (max) = I C Q ⋅
2
2 PQ (max) 2(20)
So I C Q = = = 1.67 A
VCC 24
VCC − (VCC / 2) 24 − 12
RL = = ⇒ RL = 7.2 Ω
I CQ 1.67
I CQ1.67
IB = = ⇒ 20.8 mA
β 80
24 − 0.7
RB = ⇒ RB = 1.12 kΩ
20.8
b.
I CQ ⋅ RL (1.67 )( 7.2 )
Av = g m RL = = = 462
VT 0.026
V0 (max) 12
V0 (max) = 12 V ⇒ VP = = ⇒ VP ≅ 26 mV
Av 462
8.3
VC C
a. For maximum power delivered to the load, set VC EQ =
2
Set VC C = 25 V = VCE ( sus )
VCC 25
Then I Cm = =
RL 0.1
I Cm = 250 mA < I C ,max
25 − 12.5
I CQ = = 125 mA
0.1
V
PQ ( max ) = I CQ ⋅ CC = ( 0.125 )(12.5 )
2
= 1.56 W < PD,max
125
I BQ = = 1.25 mA
100
25 − 0.7
RB = ⇒ RB = 19.4 kΩ
1.25
1 2 1
PL ( max ) = ⋅ I CQ ⋅ RL = ( 0.125 ) (100 ) ⇒ PL ( max ) = 0.781 W ( rms )
2
b.
2 2
8.4
Point (b): Maximum power delivered to load.
Point (a): Will obtain maximum signal current output.
Point (c): Will obtain maximum signal voltage output.
3. 8.5
a.
b.
VGG = 5 V, I D = 0.25 ( 5 − 4 ) = 0.25 A, VD S = 37.5 V, P = 9.375 W
2
VGG = 6 V, I D = 0.25 ( 6 − 4 ) = 1.0 A, VD S = 30 V, P = 30 W
2
VGG = 7 V, I D = 0.25 ( 7 − 4 ) = 2.25 A, VD S = 17.5 V, P = 39.375 W
2
VGG = 8 V, I D = 0.25 ⎡ 2 ( 8 − 4 )VD S − VD S ⎤
⎣
2
⎦
40 − VD S
= ⇒ VD S = 2.92
10
I D = 3.71 A, P = 10.8 W
VGG = 9 V, I D = 0.25 ⎡ 2 ( 9 − 4 ) VD S − VD S ⎤
⎣
2
⎦
40 − VD S
= ⇒ VD S = 1.88 V
10
I D = 3.81 A, P = 7.16 W
c. Yes, at VGG = 7 V, P = 39.375 W > PD ,max = 35 W
8.6
a.
VDD
Set VDSQ = = 25 V
2
50 − 25
I DQ = = 1.25 A
20
I DQ = K n (VGS − VTN )
2
1.25
+ 4 = VGS = 6.5 V
0.2
⎛ R2 ⎞
VGS = ⎜ ⎟ VDD
⎝ R1 + R2 ⎠
Let R1 + R2 = 100 kΩ
⎛ R ⎞
6.5 = ⎜ 2 ⎟ ( 50 ) ⇒ R2 = 13 kΩ
⎝ 100 ⎠
R1 = 87 kΩ
b. PD = I DQVDSQ = (1.25 )( 25 ) ⇒ PD = 31.25 W
c.
I D ,max = 2 I DQ ⇒ I D ,max = 2.5 A
VDS ,max = VDD ⇒ VDS ,max = 50 V
PD ,max = 31.25 W
d.
4. V0
= g m RL
Vi
g m = 2 K n I DQ = 2 ( 0.2 )(1.25) = 1 A / V
V0 = (1)( 20 )( 0.5 ) = 10 V
1 V02 1 (10 )
2
PL = ⋅ = ⋅ ⇒ PL = 2.5 W
2 RL 2 20
PQ = 31.25 − 2.5 ⇒ PQ = 28.75 W
8.7
(a)
(b) PD = PD ,max − ( Slope ) (T j − 25 )
60
At PD = 0, T j ,max = + 25 ⇒ T j ,max = 145°C
0.5
T j ,max − Tcase 145 − 25
(c) PD ,max = or θ dev − amb = ⇒ θ dev − amb = 2°C/W
θ dev − amb 60
8.8
T j ,max − Tamb
PD ,rated =
θ dev − case
T j ,max − Tamb
or θ dev − case =
PD ,rated
150 − 25
= = 2.5°C/W
50
Then Tdev − Tamb = PD (θ dev − case + θ case − amb )
150 − 25 = PD ( 2.5 + θ case − amb ) ⇒ 125 = PD ( 2.5 + θ case − amb )
8.9
PD = I D ⋅ VDS = ( 4 )( 5 ) = 20 W
Tdev − Tamb = PD (θ dev − case + θ case − snk + θ snk − amb )
Tdev − 25 = 20 (1.75 + 0.8 + 3) = 111 ⇒ Tdev = 136°C
Tdev − Tcase = PD ⋅θ dev − case = ( 20 )(1.75 ) = 35
Tcase = Tdev − 35 = 136 − 35 ⇒ Tcase = 101°C
Tcase − Tsink = PD ⋅θ case − snk = ( 20 )( 0.8 ) = 16°C
Tsink = Tcase − 16 = 101 − 16 ⇒ Tsink = 85°C
8.10
5. Tdev − Tamb = PD (θ dev − case + θ case − amb )
200 − 25 = 25 ( 3 + θ case − amb ) ⇒ θ case − amb = 4°C/W
8.11
T j ,max − Tamb 175 − 25
θ dev − case = = = 10°C/W
PD ,rated 15
T j ,max − Tamb
PD =
θ dev − case + θ case −snk + θ snk − amb
175 − 25
= ⇒ PD = 10 W
10 + 1 + 4
8.12
PL
η=
PS
PS = VCC ⋅ I Q
⎛V ⎞
PL = VP ⋅ I P = ⎜ CC ⎟ ( I Q )
⎝ 2 ⎠
1
⋅ VCC ⋅ I Q
η= 2 ⇒ η = 50%
VCC ⋅ I Q
8.13
vo ( max ) = 4.8 V
−0.7 − ( −5 )
iC 3 = iC 2 = = 4.3 mA
1
vS ( min )
vI = vo + 0.7 iL ( max ) = −4.3 mA =
1
so − 3.6 ≤ vI ≤ 5.5 V vo ( min ) = −4.3 V
8.14
6. 0 − VGS 3 − ( −5 )
I D 3 = K (VGS 3 − VTN ) =
2
R
12 (VGS 3 − 0.5 ) = 5 − VGS 3
2
2
2VGS 3 − 11VGS − 2 = 0
(11) + 4 (12 )( 2 )
2
11 ±
VGS 3 =
2 (12 )
VGS 3 = VGS 2 = 1.072 V
I D 3 = I D 2 = 12 (1.072 − 0.5 ) = 3.93 mA
2
VDS 2 ( sat ) = VGS 2 − VTN = 1.072 − 0.5 = 0.572 V
V0 ( min )
vo ( min ) : i2 ( max ) = −3.93 = ⇒ V0 ( min ) = −3.93 V
1
vI ( min ) = vo ( min ) + VTN = −3.93 + 0.5
vI ( min ) = −3.43 V
vo ( max ) = 5 − VDS ( sat ) = 5 − 0.572
vo ( max ) = 4.43 V
4.43
I D1 ( max ) = 3.93 + = 8.36 mA
1
I D1 = 8.36 = 12 (VGS 1 − 0.5 ) ⇒ VGS 1 = 1.33 V
2
vI ( max ) = vo + VGS1 = 4.43 + 1.33 ⇒ vI ( max ) = 5.76 V
8.15
a. Neglect base currents.
v0 ( max ) = V + − VCE (sat) = 10 − 0.2 = 9.8 V
9.8 9.8
iL (max) = I Q = = ⇒ I Q = 9.8 mA
RL 1
0 − 0.7 − ( −10 )
R= ⇒ R = 949 Ω
9.8
iE1 ( max ) = 2 I Q ⇒ iE1 ( max ) = 19.6 mA
iE1 ( min ) = 0
iL ( max ) = I Q = 9.8 mA
iL ( min ) = − I Q = −9.8 mA
b.
1 1
( iL ( max ) ) RL = 2 ( 9.8)2 (1) ⇒ PL = 48.02 mW
2
PL =
2
PS = I Q (V + − V − ) + I Q ( 0 − V − )
= 9.8 ( 20 ) + 9.8 (10 ) ⇒ PS = 294 mW
PL 48.02
η= = ⇒ η = 16.3%
PS 294
8.16
a.
v0 ( max ) 10
I Q ( min ) = = ⇒ I Q ( min ) = 100 mA
RL 0.1
0 − 0.7 − ( −12 )
R= ⇒ R = 113 Ω
100
b.
7. PQ1 = I Q ⋅ VCE1 = (100 )(12 ) ⇒ PQ1 = 1.2 W
P (source) = 2 I Q (12 ) = 2.4 W
c.
(10 )
2
1 VP2
PL = ⋅ = = 0.5 W
2 RL 2 (100 )
PS = 1.2 + 2.4 = 3.6 W
PL 0.5
η= = ⇒ η = 13.9%
PS 3.6
8.17
I D1 = K n (VGS − VTN ) = 12 ( 0 − ( −1.8 ) )
2 2
I D1 = 38.9 mA
(a)
For RL = ∞
vo ( max ) = 4.8 V
VDS ( sat ) = VGS − VTN = 1.8 V
vo ( min ) = −5 + 1.8 = −3.2 V
vI = vo + 0.7 ⇒ −2.5 ≤ vI ≤ 5.5 V
(b) For RL = 500 Ω vo ( max ) = 4.8 V
vo −3.2
For vo < 0, vo ( min ) = −3.2 V ′
I2 = = = −6.4 mA
RL 0.5
−2.5 ≤ vI ≤ 5.5 V
(c)
For vo = −2V , I 2 ( max ) = −38.9 mA
′
−2
R2 ( min ) = ⇒ RL ( min ) = 51.4 Ω
−38.9
1 v2 1 ( 2)
2
PL = ⋅ o = ⋅ ⇒ PL = 38.9 mW
2 RL 2 51.4
38.9
PL = 10 ( 38.9 ) = 389 mW % = = 10%
389
8.18
V 2 (V )
+ 2
PL = P =
RL RL
1 (V ) 1 (V )
+ 2 − 2
PS = ⋅ + ⋅ , V − = −V +
2 RL 2 RL
So PS =
(V )
+ 2
RL
PL
η= ⇒ η = 100%
PS
8.19
(a)
8. As maximum conversion efficiency
π V
η = , P = 0.785
4 VCC
⎛4⎞
So V p ( max ) = ( 0.785 )( 5 ) ⎜ ⎟
⎝π ⎠
V p ( max ) = 5 V
2VCC 2 ( 5)
(b) Maximum power dissipation occurs when V p = = = 3.183 V
π π
2
VCC
(c) P ( max ) =
θ
π RL
2
( 5)
2
2= ⇒ RL = 1.27 Ω
π 2 RL
8.20
2
1 Vp
(a) P= ⋅
2 RL
2
1 Vp
50 = ⋅ ⇒ V p = 49 V ⇒ V + = 52 V, V − = −52 V
2 24
V 49
(b) IP = P = = 2.04 A
RL 24
π VP π ⎛ 49 ⎞
(c) η= ⋅ = ⎜ ⎟
4 VCC 4 ⎝ 52 ⎠
η = 74.0%
8.21
(a)
VDS ≥ VDS ( sat ) = VGS − VTN = VGS
VDS = 10 − Vo ( max ) and I D = I L = K n (VGS )
2
Vo ( max )
= K n (VGS )
2
RL
Vo ( max )
VGS =
RL ⋅ K n
Vo ( max ) Vo ( max )
So 10 − Vo ( max ) = =
RL ⋅ K n ( 5 )( 0.4 )
2 V0 ( max )
⎡10 − V0 ( max ) ⎤ =
⎣ ⎦ 2
V0 ( max )
100 − 20V0 ( max ) + V02 ( max ) =
2
V02 ( max ) − 20.5V0 ( max ) + 100 = 0
( 20.5 ) − 4 (100 )
2
20.5 ±
V0 ( max ) = ⇒ V0 ( max ) = 8 V
2
8
iL = ⇒ iL = 1.6 mA
5
i 1.6
VGS = L = = 2 V ⇒ VI = 10 V
Kn 0.4
b.
9. 1 (8)
2
PL = ⋅ = 6.4 mW
2 5
20 (1.6 )
PS = = 10.2 mW
π
PL 6.4
η= = ⇒ η = 62.7%
PS 10.2
8.22
vO = iL RL and iL = iD = K n ( vGS − VTN ) or iL = K n ( vGS ) and vGS = vI − vO
2 2
Then
vO = K n RL ( vI − vO ) or vO = 2 ( vI − vO )
2 2
dv0 ⎛ dv ⎞
= ( 2 )( 2 )( vI − v0 ) ⎜ 1 − 0 ⎟
dvI ⎝ dvI ⎠
dv0
⎡1 + 4 ( vI − v0 ) ⎤ = 4 ( vI − v0 )
dvI ⎣ ⎦
dv0 4 ( vI − v0 )
or =
dvI 1 + 4 ( vI − v0 )
dv0 4 (10 − 8 ) dv
For vI = 10 V, v0 = 8 V ⇒ = ⇒ 0 = 0.889
dvI 1 + 4 (10 − 8 ) dvI
dv0
At vI = 0, v0 = 0 ⇒ =0
dvI
dv0
At vI = 1, v0 = 0.5 ⇒ = 0.667
dvI
8.23
a.
⎛i ⎞ ⎛ 5 × 10−3 ⎞
VBE = VT ln ⎜ C ⎟ = ( 0.026 ) ln ⎜ −13 ⎟
⎝ IS ⎠ ⎝ 5 × 10 ⎠
V
VBE = BB = 0.5987 V ⇒ VBB = 1.1973 V
2
PQ = iC ⋅ vCE = ( 5 )(10 ) ⇒ PQ = 50 mW
b.
10. v0 = −8 V
−8
iL = ⇒ iL = −80 mA
0.1
iCp ≈ 80 mA
⎛ iCp ⎞ ⎛ 80 × 10−3 ⎞
vEB = VT ln ⎜ ⎟ = ( 0.026 ) ln ⎜ −13 ⎟
⎝ IS ⎠ ⎝ 5 × 10 ⎠
vEB = 0.6708 V
VBB
vI = − vEB + v0 = 0.5987 − 0.6708 − 8⇒ vI = −8.072 V
2
VBE = VBB − vEB = 1.1973 − 0.6708 = 0.5265 V
⎛v ⎞ ⎛ 0.5265 ⎞
iCn = I S exp ⎜ BE ⎟ = 5 × 10−13 exp ⎜ ⎟ ⇒ iCn = 0.311 mA
⎝ VT ⎠ ⎝ 0.026 ⎠
PL = iL RL = ( 80 ) ( 0.1) ⇒ PL = 640 mW
2 2
PQn = iCn ⋅ vCE = ( 0.311) (10 − ( −8 ) ) ⇒ PQn = 5.60 mW
PQp = iCp ⋅ vEC = ( 80 )( 2 ) ⇒ PQp = 160 mW
8.24
iDn = K n ( vGSn − VTN )
2
(a)
0.5 V
+ 2 = vGSn = 2.5 V = BB ⇒ VBB = 5.0 V
2 2
Pn = ( 0.5 )(10 ) ⇒ Pn = Pp = 5 mW
(b) VDS = VGS − VTN ⇒ VDS = VGS − 2 VDS = 10 − vo ( max )
and
iL v ( max ) v ( max )
VGS = + VTN = O +2 = O +2
Kn RL K n ( 2 )(1)
so
v0 ( max ) v0 ( max )
10 − v0 ( max ) = +2−2 =
2 2
so v0 ( max ) = 8 V
8
iDn = iL = ⇒ iDn = iL = 8 mA
1
8
VGS = + 2 ⇒ VGS = 4 V
2
V
Then vI = vo + VGS − BB = 8 + 4 − 2.5 ⇒ vI = 9.5 V
2
⎛ VBB ⎞
vSGp = vo − ⎜ vI − ⎟ = 8 − ( 9.5 − 2.5 )
⎝ 2 ⎠
vSGp = 1 V ⇒ M p cutoff ⇒ iDp = 0
PL = iL RL = ( 8 ) (1) ⇒ PL = 64 mW
2 2
PMn = iDn ⋅ vDS = ( 8 )(10 − 8 ) ⇒ PMn = 16 mW
PMp = iDp ⋅ vSD ⇒ PMp = 0
8.25
a.
11. 24
v0 = 24 V ⇒ iL = ⇒ iL ≈ iN = 3 A
8
3
iBn = ⇒ iBn = 73.2 mA
41
For iD = 25 mA ⇒ iR1 = 25 + 73.2 = 98.2 mA
⎛i ⎞ ⎛ 3 ⎞
VBE = VT ln ⎜ N ⎟ = ( 0.026 ) ln ⎜ −12 ⎟
⎝ IS ⎠ ⎝ 6 × 10 ⎠
= 0.7004 V
30 − ( 24 + 0.7 ) 5.3
Then 98.2 = ⇒ R1 = ⇒ R1 = 53.97 Ω
R1 98.2
⎛ 25 × 10−3 ⎞
VD = ( 0.026 ) ln ⎜ −12 ⎟
= 0.5759 V
⎝ 6 × 10 ⎠
VEB = 2VD − VBE = 2 ( 0.5759 ) − 0.7004
= 0.4514 V
⎛V ⎞ ⎛ 0.4514 ⎞
iP = I S exp ⎜ EB ⎟ = ( 6 × 10−12 ) exp ⎜ ⎟ ⇒ iP = 0.208 mA
⎝ VT ⎠ ⎝ 0.026 ⎠
b. Neglecting base current
30 − 0.6 30 − 0.6
iD ≈ = ⇒ iD ≈ 545 mA
R1 53.97
⎛ 0.545 ⎞
VD = ( 0.026 ) ln ⎜ −12 ⎟
= 0.656 V
⎝ 6 × 10 ⎠
Approximation for iD is okay.
Diodes and transistors matched ⇒ iN = iP = 545 mA
8.26
(a)
I D1 = K1 (VGS 1 − VTN )
2
5
VGS1 = +1 = 2 V
5
I D 3 = K 3 (VGS 3 − VTN )
2
200 = K 3 ( 2 − 1) ⇒ K n3 = K p 4 = 200 μ A / V 2
2
(b)
vI + VSG 4 + VGS 3 − VGS1 = vO
For vo large, iL = i1 = K n1 (VGS1 − VTN )
2
iL vo
VGS1 = + VTN = + VTN
K n1 RL K n1
⎛ vo ⎞
So vI + 2 + 2 − ⎜ + 1⎟ = v0
⎜ ( 0.5)( 5) ⎟
⎝ ⎠
v0
vI = v0 + −3
2.5
dvI dv 1 1 dv
=1= 0 + ⋅ ⋅ 0
dvI dvI 2 2.5v0 dvI
⎡
dv0 1 ⎤
1= ⎢1 + ⎥
⎢ 2 2.5v0 ⎥
dvI
⎣ ⎦
For vO = 5 V :
12. dv0 ⎡ 1 ⎤ dv dv
1= ⎢1 + ⎥ = 0 (1.1414 ) ⇒ 0 = 0.876
dvI ⎢ 2 2.5 ( 5 ) ⎥ dvI dvI
⎣ ⎦
8.27
VBB I Dn
vO = vI + − VGS and VGS = + VTN
2 Kn
vO
For vO ≈ 0, I Dn = I DQ + iL = I DQ +
RL
VBB I DQ + ( vO / RL ) V I DQ v
Then vO = vI + − VTN − or vO = vI + BB − VTN − ⋅ 1+ O
2 Kn 2 Kn I DQ RL
VBB I DQ 1 v
For vO small, vO ≅ vI + − VTN − ⋅ 1+ ⋅ O
2 Kn 2 I DQ RL
⎡ 1 I DQ 1 ⎤ V I DQ
vO ⎢1 + ⋅ ⋅ ⎥ = vI + BB − VTN −
⎢ 2 Kn
⎣ I DQ RL ⎥
⎦ 2 Kn
Now
dvO 1
= = 0.95
dvI ⎡ 1 I DQ 1 ⎤
⎢1 + ⋅ ⋅ ⎥
⎢ 2
⎣ K n I DQ RL ⎥
⎦
1 I DQ 1 1
So ⋅ ⋅ = − 1 = 0.0526
2 K n I DQ RL 0.95
1
For RL = 0.1 k Ω, then = 0.01052
K n I DQ
Or K n I DQ = 95.1
We can write g m = 2 K n I DQ = 190 mA/V
This is the required transconductance for the output transistor. This implies a very large transistor.
8.28
Av = − g m RL
I CQ
So −12 = − g m ( 2 ) ⇒ g m = 6 mA/V=
VT
I CQ = ( 6 )( 0.026 ) ⇒ I CQ = 0.156 mA
VCC 10
But for maximum symmetrical swing, set I CQ = = = 5 mA ⇒ Av > 12
RL 2
Maximum power to the load:
1 VCC (10 )
2 2
PL ( max ) = ⋅ = ⇒ PL ( max ) = 25 mW
2 RL 2 ( 2)
PS = VCC ⋅ I CQ = (10 )( 5 ) = 50 mW
So η = 50%
13. 5
I CQ
I BQ = =
= 0.0278 mA
β 180
R1 = RTH = 6 kΩ
VTH = I BQ RTH + VBE ( on ) + (1 + β ) I BQ RE
Set RE = 20 Ω
VTH = ( 0.0278 )( 6 ) + 0.7 + (181)( 0.0278 )( 0.020 )
VTH = 0.967 V
1
VTH = ⋅ RTH ⋅ VCC
R1
1
0.967 = ( 6 )(10 ) ⇒ R1 = 62.0 kΩ
R1
R2 = 6.64 kΩ
8.29
VCC 15
I CQ = = = 15 mA
RL 1
15
I BQ = = 0.15 mA
100
(15)
2
1 V2
PL ( max ) = ⋅ CC = ⇒ PL ( max ) = 112.5 mW
2 RL 2 (1)
Let RTH = 10 kΩ
VTH = I BQ RTH + VBE + (1 + β ) I BQ RE
= ( 0.15 )(10 ) + 0.7 + (101)( 0.15 )( 0.1)
1 1
VTH = 3.715 = ⋅ RTH ⋅ VCC = ⋅ (10 )(15 )
R1 R1
R1 = 40.4 kΩ
R2 = 13.3 kΩ
8.30
⎛ R2 ⎞ ⎛ 1.55 ⎞
VTH = ⎜ ⎟ VCC = ⎜ ⎟ (10 )
⎝ R1 + R2 ⎠ ⎝ 1.55 + 0.73 ⎠
= 6.80 V
RTH = R1 R2 = 0.73 1.55 = 0.496 kΩ
VTH − VBE 6.80 − 0.70
I BQ = =
RTH + (1 + β ) RE 0.496 + ( 26 )( 0.02 )
I BQ = 6.0 mA, I CQ = 150 mA
Av = − g m RL and RL = a 2 RL = ( 3) ( 8 ) = 72 Ω
2
′ ′
I CQ 150
gm = = ⇒ 5.77 A/V
VT 0.026
14. Av = − ( 5.77 )( 72 ) = −415
Vo ′ = Av ⋅ Vi = ( 415 )( 0.017 ) = 7.06 V
7.06
Vo = = 2.35 V
3
7.06
Vo = = 2.35 V
3
7.06
Vo = = 2.35 V
3
PS = I CQ ⋅ VCC = ( 0.15 )(10 ) = 1.5 W
PL 0.345
η= = ⇒ η = 23%
PS 1.5
8.31
a. Assuming the maximum power is being delivered, then
36 9
Vo′ ( peak ) = 36 V ⇒ Vo = = 9 V ⇒ Vrms = ⇒ Vrms = 6.36 V
4 2
36
b. Vo = ⇒ Vo = 25.5 V
2
PL 2
c. Secondary I rms = = ⇒ I rms = 0.314 A
Vrms 6.36
0.314
Primary I P = ⇒ I P = 78.6 mA
4
d.
PS = I CQ .VCC = ( 0.15 )( 36 ) = 5.4 W
2
η= ⇒ η = 37%
5.4
8.32
a.
15. ⎛V ⎞ ⎛1 ⎞
ve = ⎜ π + g mVπ ′
⎟ RE = Vπ ′
⎜ + g m ⎟ RE
⎝ rπ ⎠ ⎝ rπ ⎠
⎛1+ β ⎞
= Vπ ⎜ ′
⎟ RE
⎝ rπ ⎠
vi = Vπ + ve ⇒ Vπ = vi − ve
⎛ 1+ β ⎞
ve = (vi − ve ) ⎜ ′
⎟ RE
⎝ rπ ⎠
1+ β
⋅ RE′
(1 + β ) RE
2
ve rπ ′ v ⎛n ⎞
= = ′
= e where RE = ⎜ 1 ⎟ RL
vi 1 + 1 + β ⋅ R ′ rπ + (1 + β ) RE vi ′ ⎝ n2 ⎠
E
rπ
ve ⎛n ⎞
v0 = so ve − v0 ⎜ 1 ⎟
⎛ n1 ⎞ ⎝ n2 ⎠
⎜ ⎟
⎝ n2 ⎠
v 1 (1 + β ) RE′
so 0 = ⋅
vi ⎛ n1 ⎞ rπ + (1 + β ) RE ′
⎜ ⎟
⎝ n2 ⎠
b.
1 2 n1 I 1
PL = ⋅ I P RL , a = , I CQ = P so PL = .a 2 I CQ RL
2
2 n2 a 2
PS = I CQ .VCC
For η = 50% :
1 2 2
⋅ a I CQ RL a 2 I R
PL VCC VCC V
= 0.5 = 2 = so a 2 = = ⇒ a 2 = CC
CQ L
PS I CQ ⋅ VCC 2VCC I CQ ⋅ RL ( 0.1)( 50 ) 5
c.
r β VT 49 ( 0.026 )
R0 = π = = ⇒ R0 = 0.255 Ω
1 + β (1 + β ) I CQ ( 50 )( 0.1)
8.33
a. With a 10:1 transformer ratio, we need a current gain of 8 through the transistor.
⎛ R1 R2 ⎞ ie ⎛ R1 R2 ⎞
ie = (1 + β ) ib and ib = ⎜ ⎟ ii so we need = 8 = (1 + β ) ⎜ ⎟ where
⎜R R +R ⎟ ii ⎜R R +R ⎟
⎝ 1 2 ib ⎠ ⎝ 1 2 ib ⎠
Rib = rπ + (1 + β ) RL ≈ (1 + β ) RL = (101)( 0.8 ) = 80.8
′ ′
16. ⎛ R1 R2 ⎞
Then 8 = (101) ⎜
⎜ R R + 80.8 ⎟
⎟
⎝ 1 2 ⎠
R1 R2
= 0.0792 or R1 R2 = 6.95 kΩ
R1 R2 + 80.8
2VCC V 12
Set = RL ⇒ I CQ = CC =
′ = 15 mA
2 I CQ ′
RL 0.8
15
I BQ = = 0.15 mA
100
VTH = I BQ RTH + VBE
1
⋅ RTH ⋅ VCC = I BQ RTH + VBE
R1
1
( 6.95)(12 ) = ( 0.15)( 6.95) + 0.7 ⇒ R1 = 47.9 kΩ then R2 = 8.13 kΩ
R1
b.
I
I e = 0.9 I CQ = 13.5 mA = L ⇒ I L = 135 mA
a
1
PL = ( 0.135 ) ( 8 ) ⇒ PL = 72.9 mW
2
2
PS = VCC I CQ = (12 )(15 ) ⇒ PS = 180 mW
PL
η= ⇒ η = 40.5%
PS
8.34
a.
VP = 2 RL PL
VP = 2 ( 8 )( 2 ) = 5.66 V = peak output voltage
VP 5.66
IP = = = 0.708 A = peak output current
RL 8
Set Ve = 0.9VCC = aVP to minimize distortion
( 0.9 )(18)
Then a = ⇒ a = 2.86
5.66
b.
1 ⎛ I P ⎞ 1 ⎛ 0.708 ⎞
Now I CQ = = ⎜ ⎟ ⇒ I CQ = 0.275 A
0.9 ⎜ a ⎟ 0.9 ⎝ 2.86 ⎠
⎝ ⎠
Then PQ = VCC I Q = (18 )( 0.275 ) ⇒ PQ = 4.95 W Power rating of transistor
8.35
a. Need a current gain of 8 through the transistor.
17. ib ⎛ R1 R2 ⎞
= 8 = (1 + β ) ⎜ ⎟ where Rib ≈ (1 + β )( 0.9 ) = 90.9 kΩ
ii ⎜R R +R ⎟
⎝ 1 2 ib ⎠
8 ⎛ R1 R2 ⎞
=⎜ = 0.0792 or R1 R2 = 7.82 kΩ
⎜ R R + 90.9 ⎟
101 ⎝ 1 2 ⎟
⎠
2VCC 12
Set = 0.9 kΩ ⇒ I CQ = = 13.3 mA
2 I CQ 0.9
13.3
I BQ = = 0.133 mA
100
1
Then ( 7.82 )(12 ) = ( 0.133)( 7.82 ) + 0.7 ⇒ R1 = 53.9 kΩ and R 2 = 9.15 kΩ
R1
b.
I
I e = ( 0.9 ) I CQ = 12 mA = L ⇒ I L = 120 mA
a
1
PL = ( 0.12 ) ( 8 ) ⇒ PL = 57.6 mW
2
2
PS = VCC I CQ = (12 )(13.3) ⇒ PS = 159.6 mW
PL 57.6
η= = ⇒ η = 36.1%
PS 159.6
8.36
a. All transistors are matched.
⎛1+ β ⎞ iC
3 mA = iE1 + iB 3 = ⎜ ⎟ iC +
⎝ β ⎠ β
⎛ 61 1 ⎞
3 = ⎜ + ⎟ iC ⇒ iC = 2.90 mA
⎝ 60 60 ⎠
b.
For vo = 6 V , let RL = 200 Ω.
6
io = = 0.03 A = 30 mA ≅ iE 3
200
30
iB 3 = = 0.492 mA
61
iE1 = 3 − 0.492 = 2.508 mA
2.508
iB1 = ⇒ iB1 = 41.11 μ A
61
3
iE 2 ≅ 3 mA ⇒ iB 2 = ⇒ 49.18 μ A
61
iI = iB 2 − iB1 = 49.18 − 41.11 ⇒ iI = 8.07 μ A
Current gain
30 × 10−3
Ai = ⇒ Ai = 3.72 × 103
8.07 × 10−6
⎛i ⎞ ⎛ 30 × 10−3 ⎞
VBE 3 = VT ln ⎜ E 3 ⎟ = ( 0.026 ) ln ⎜ −13 ⎟
⎝ IS ⎠ ⎝ 5 × 10 ⎠
VBE 3 = 0.6453 V
⎛i ⎞ ⎛ 2.508 × 10−3 ⎞
VEB1 = VT ln ⎜ E1 ⎟ = ( 0.026 ) ln ⎜ −13 ⎟
⎝ IS ⎠ ⎝ 5 × 10 ⎠
VEB1 = 0.5807 V
18. vI = v0 + VBE 3 − VEB1 = 6 + 0.6453 − 0.5807
vI = 6.0646 V
Voltage gain
v0 6
Av = = ⇒ Av = 0.989
vI 6.0646
8.37
1
a. For i0 = 1 A, I B 3 ≅ ⇒ 20 mA
50
10 − VEB1 ⎡10 − ( v0,max + VBE 3 ) ⎤
We can then write = 2⎢ − 20 ⎥
R1 ⎢
⎣ R1 ⎥
⎦
10 − VBE 2vo,max
If, for simplicity, we assume VEB1 = VBE 3 = 0.7 V, then = + 40
R1 R1
9.3 2 ( 4 )
If we assume v0,max = 4 V, then = + 40 which yields R1 = R2 = 32.5 Ω
R1 R1
9.3
b. For vI = 0, I E1 = ⇒ I E1 = 0.286 A = I E 2
32.5
Since I S 3,4 = 10 I S1,2 , then I E 3 = I E 4 = 2.86 A
c.
We can write
⎧ rπ 1 ⎫
⎪ rπ 3 + R1 ⎪
1⎪ 1 + β1 ⎪
R0 = ⎨ ⎬
2⎪ 1 + β3 ⎪
⎪ ⎪
⎩ ⎭
βV ( 50 )( 0.026 )
Now rπ 3 = 3 T = = 0.4545 Ω
IC 3 2.86
β1VT (120 )( 0.026 )
rπ 1 = = = 10.91 Ω
I C1 0.286
So
⎧ 10.91 ⎫
0.4545 + 32.5
1⎪⎪ 121 ⎪⎪
R0 = ⎨ ⎬
2⎪ 51 ⎪
⎪
⎩ ⎪
⎭
10.91
32.5 = 32.5 0.0902 = 0.0900
121
1 ⎧ 0.4545 + 0.0900 ⎫
Then R0 = ⎨ ⎬ or R 0 = 0.00534 Ω
2⎩ 51 ⎭
8.38
19. Ri =
1
2
{ ⎣ }
rπ 1 + (1 + β ) ⎡ R1 ( rπ 3 + (1 + β ) 2 RL ) ⎤
⎦
iC1 ≈ 7.2 mA and iC 3 ≈ 7.2 mA
( 60 )( 0.026 )
Then rπ = = 0.217 kΩ
7.2
So Ri =
1
2
{
0.217 + ( 61) ⎡ 2 ( 0.217 + ( 61)( 0.2 ) ) ⎤
⎣ ⎦ }
1
2
{ ⎣ ⎦ }
= 0.217 + 61 ⎡ 2 12.4 ⎤ or Ri = 52.6 kΩ
8.39
a.
b.
V + − VSG
I1 = K1 (VSG + VTP ) =
2
R1
5 = 10 (VSG − 2 ) ⇒ VSG = 2.707 V
2
10 − 2.707
5= ⇒ R1 = R2 = 1.46 kΩ
R1
c. RL = 100 Ω For a sinusoidal output signal:
20. 1 (v ) 1 ( 5)
2 2
PL = ⋅ o = ⋅ ⇒ PL = 125 mW
2 RL 2 0.1
( vo ) ( 5 )
iD 3 ≈ = ⇒ iD 3 = 50 mA
RL 0.1
50
VGS 3 = + 2 = 4.236 V
10
10 − ( 4.236 + 5 )
I1 = ⇒ I D1 = 0.523 mA
1.46
0.523
VSG1 = + 2 = 2.229 V
10
vI = 5 + 4.236 − 2.229 ⇒ vI = 7.007 V
(VI − VGS ) − ( −10 )
= 10 (VGS − 2 )
2
I D2 =
1.46
17.007 − VGS
= 10 (VGS − 4VGS + 4 )
2
1.46
2
14.6VGS − 57.4VGS + 41.4 = 0
( 57.4 ) − 4 (14.6 )( 41.4 )
2
57.4 ±
VGS =
2 (14.6 )
VGS 2 = 2.98 V
I D 2 = 10 ( 2.98 − 2 ) ⇒ I D 2 = 9.60 mA
2
VG 4 = vI − VGS 2 = 7 − 2.98 = 4.02 V
VSG 4 = 5 − 4.02 = 0.98 V ⇒ I D 4 = 0
8.40
For v0 = 0
I Q = I C 3 + I C 2 + I E1
⎛ 1+ βn ⎞ IC 3
I B3 = I E 2 = ⎜ ⎟ IC 2 =
⎝ βn ⎠ βn
I C 3 = (1 + β n ) I C 2
⎛ β ⎞ I
I B 2 = I C 1 = ⎜ P ⎟ I E1 = C 2
⎝ 1+ βP ⎠ βn
⎛ β ⎞
I C 2 = β n ⎜ P ⎟ I E1
⎝ 1+ βP ⎠
⎛ β ⎞
I C 3 = (1 + β n ) β n ⎜ P ⎟ I E1
⎜1+ β ⎟
⎝ p ⎠
⎛ β ⎞ ⎛ β ⎞
I Q = (1 + β n ) β n ⎜ P ⎟ I E1 + β n ⎜ P ⎟ I E1 + I E1
⎝1+ βP ⎠ ⎝ 1+ βP ⎠
⎛ 10 ⎞ ⎛ 10 ⎞
= ( 51)( 50 ) ⎜ ⎟ I E1 + ( 50 ) ⎜ ⎟ I E1 + I E1
⎝ 11 ⎠ ⎝ 11 ⎠
I Q = 2318.18I E1 + 45.45 I E1 + I E1
I E1 = 1.692 μ A ⇒ I C1 = 1.534 μ A
⎛ 10 ⎞
I C 2 = ( 50 ) ⎜ ⎟ (1.692 ) ⇒ I C 2 = 76.9 μ A
⎝ 11 ⎠
⎛ 10 ⎞
I C 3 = ( 51)( 50 ) ⎜ ⎟ (1.692 ) ⇒ I C 3 = 3.92 mA
⎝ 11 ⎠
21. Because of rπ 1 and Z, neglect effect of r0. Then neglecting r01, r02 and r03, we find
VX
I X = g m 3Vπ 3 + g m 2Vπ 2 + g m1Vπ 1 +
rπ 1 + Z
Now
⎛ r ⎞
Vπ 1 = ⎜ π 1 ⎟ VX , Vπ 2 ≅ g m1Vπ 1rπ 2
⎝ rπ 1 + Z ⎠
and
Vπ 3 = ( g m1Vπ 1 + g m 2Vπ 2 ) rπ 3
= ⎡ g m1Vπ 1 + g m 2 ( g m1Vπ 1rπ 2 ) ⎤ rπ 3
⎣ ⎦
⎛ r ⎞
Vπ 3 = ⎜ π 1 ⎟ [ g m1 + g m1 g m 2 rπ 2 ] rπ 3 ⋅ VX
⎝ rπ 1 + Z ⎠
( β + β1 β 2 ) rπ 3
Vπ 3 = 1 ⋅ VX
rπ 1 + Z
⎛ r ⎞ ⎛ βr ⎞
and Vπ 2 = g m1 ⎜ π 1 ⎟ rπ 2VX = ⎜ 1 π 2 ⎟ VX
⎝ rπ 1 + Z ⎠ ⎝ rπ 1 + Z ⎠
( β + β1 β 2 ) β 3 ββ β1 VX
Then I X = 1 ⋅ V X + 1 2 ⋅ VX + ⋅ VX +
rπ 1 + Z rπ 1 + Z rπ 1 + Z rπ 1 + Z
Then
VX rπ 1 + Z
R0 = =
I X 1 + β1 + β1 β 2 + ( β1 + β1 β 2 ) β 3
(10 )( 0.026 )
rπ 1 = = 0.169 MΩ
1.534
Z = 25 kΩ
Then
169 + 25
R0 =
1 + (10 ) + (10 )( 50 ) + ⎡10 + (10 )( 50 ) ⎤ ( 50 )
⎣ ⎦
194
R0 = = 0.00746 kΩ or Ro = 7.46 Ω
26, 011
8.41
a Neglect base currents.
⎛I ⎞
VBB = 2VD = 2VT ln ⎜ Bias ⎟
⎝ IS ⎠
⎛ 5 × 10−3 ⎞
= 2 ( 0.026 ) ln ⎜ −13 ⎟
⇒ VBB = 1.281 V
⎝ 10 ⎠
22. VBE1 + VEB 3 = VBB
I E1 = I E 3 + I C 2
⎛ β ⎞
I B2 = IC 3 = ⎜ P ⎟ I E 3
⎝ 1+ βP ⎠
⎛ β ⎞
IC 2 = β n I B 2 = β n ⎜ P ⎟ I E 3
⎝ 1+ βP ⎠
⎛ β ⎞
I E1 = I E 3 + β n ⎜ P ⎟ IE3
⎝ 1+ βP ⎠
⎡ ⎛ β ⎞⎤
I E1 = I E 3 ⎢1 + β n ⎜ P ⎟⎥
⎣ ⎝ 1+ βP ⎠⎦
⎛ 1+ βn ⎞ ⎛ 1+ βP ⎞ ⎡ ⎛ βP ⎞⎤
⎜ ⎟ I C1 = ⎜ ⎟ I C 3 ⎢1 + β n ⎜ ⎟⎥
⎝ βn ⎠ ⎝ βP ⎠ ⎣ ⎝ 1+ βP ⎠⎦
⎡I ⎤ ⎡I ⎤
VBE1 = VT ln ⎢ C1 ⎥ , VEB 3 = VT ln ⎢ C 3 ⎥
⎣ IS ⎦ ⎣ IS ⎦
⎡ ⎛ 20 ⎞ ⎤
(1.01) I C1 = ⎛
21 ⎞
⎜ ⎟ IC 3 ⎢1 + (100 ) ⎜ 21 ⎟ ⎥
⎝ 20 ⎠ ⎣ ⎝ ⎠⎦
⎡ 21 ⎤
= I C 3 ⎢ + 100 ⎥ = 101.05 I C 3
⎣ 20 ⎦
I C1 = 100.05 I C 3
⎛ 100.05 I C 3 ⎞ ⎛ IC 3 ⎞
VT ln ⎜ ⎟ + VT ln ⎜ ⎟ = VBB
⎝ IS ⎠ ⎝ IS ⎠
⎛ 100.05 I C 3 ⎞
2
VT ln ⎜ 2 ⎟ = VBB
⎝ IS ⎠
2
100.05 I C 3 ⎛V ⎞
2
= exp ⎜ BB ⎟
I S ⎝ VT ⎠
IS ⎛V ⎞
IC 3 = exp ⎜ BB ⎟ = 0.4995 mA = I C3
100.05 ⎝ VT ⎠
Then I E 3 = 0.5245 mA
Now I C1 = 100.05 I C 3 = 49.97 mA = I C1
⎛ 20 ⎞
I C 2 = (100 ) ⎜ ⎟ ( 0.5245 ) = 49.95 mA = I C 2
⎝ 21 ⎠
⎛I ⎞ ⎛ 49.97 × 10−3 ⎞
VBE1 = VT ln ⎜ C1 ⎟ = 0.026 ln ⎜ −13 ⎟
⎝ IS ⎠ ⎝ 10 ⎠
= 0.70037
⎛I ⎞ ⎛ 0.4995 × 10−3 ⎞
VEB 3 = VT ln ⎜ C 3 ⎟ = 0.026 ln ⎜ ⎟
⎝ IS ⎠ ⎝ 10−13 ⎠
= 0.58062
Note: VBE1 + VEB 3 = 0.70037 + 0.58062 = 1.28099
= VBB
b.
23. 10
v0 = 10 V ⇒ iE1 ≈ = 0.10 A = iC1
100
100
iB1 = = 1 mA
100
⎛ 4 × 10−3 ⎞
VBB = 2 ( 0.026 ) ln ⎜ −13 ⎟
= 1.2694 V
⎝ 10 ⎠
⎛ 0.1 ⎞
VBE1 = ( 0.026 ) ln ⎜ −13 ⎟ = 0.7184
⎝ 10 ⎠
VEB 3 = 1.2694 − 0.7184 = 0.55099 V
⎛ 0.55099 ⎞
I C 3 = 10−13 exp ⎜ ⎟ = 0.1598 mA
⎝ 0.026 ⎠
V 2 (10 )
2
PL = 0 = ⇒ PL = 1 W
RL 100
PQ1 = iC1 ⋅ vCE1 = ( 0.1)(12 − 10 ) ⇒ PQ1 = 0.2 W
PQ 3 = iC 3 ⋅ vEC 3 = ( 0.1598 ) (10 − [ 0.7 − 12]) ⇒ PQ 3 = 3.40 mW
iC 2 = (100 )( iC 3 ) = (100 )( 0.1598 ) = 15.98 mA
PQ 2 = iC 2 ⋅ vCE 2 = (15.98 ) (10 − [ −12]) ⇒ PQ 2 = 0.352 W
8.42
a.
⎛ 10 × 10−3 ⎞
VBB = 3 ( 0.026 ) ln ⎜ −12 ⎟
⇒ VBB = 1.74195 V
⎝ 2 × 10 ⎠
VBE1 + VBE 2 + VEB 3 = VBB
IC 2 IC 2
I C1 ≈ , IC 3 ≈
βn β n2
⎛I ⎞ ⎛I ⎞ ⎛I ⎞
VT ln ⎜ C1 ⎟ + VT ln ⎜ C 2 ⎟ + VT ln ⎜ C 3 ⎟ = VBB
⎝ IS ⎠ ⎝ IS ⎠ ⎝ IS ⎠
⎡ IC ⎤
3
VT ln ⎢ 3 2 3 ⎥ = VBB
⎣ βn IS ⎦
⎛V ⎞
I C 2 = β n I S 3 exp ⎜ BB ⎟
⎝ VT ⎠
⎛ 1.74195 ⎞
= ( 20 ) ( 20 × 10−12 ) 3 exp ⎜ ⎟
⎝ 0.026 ⎠
I C 2 = 0.20 A, I C1 ≈ 10 mA, I C 3 ≈ 0.5 mA
⎛ 10 × 10−3 ⎞
VBE1 = ( 0.026 ) ln ⎜ −12 ⎟
⇒ VBE1 = 0.58065 V
⎝ 2 × 10 ⎠
⎛ 0.2 ⎞
VBE 2 = ( 0.026 ) ln ⎜ −12 ⎟
⇒ VBE 2 = 0.6585 V
⎝ 2 × 10 ⎠
⎛ 0.5 × 10−3 ⎞
VEB 3 = ( 0.026 ) ln ⎜ −12 ⎟
⇒ VEB 3 = 0.50276 V
⎝ 2 × 10 ⎠
b.
1 V2 1 V2
PL = 10 W= ⋅ 0 = ⋅ 0 ⇒ V0 ( max ) = 20 V
2 RL 2 20
For v0 ( max ) :
24. v0 ( 20 )
2 2
PL = = ⇒ PL = 20 W
RL 20
20
i0 ( max ) = − = −1 A
20
iC 5 + iC 4 + iE 3 = −io ( max ) = 1 A
iC 5 ⎛ β n ⎞ iC 4 ⎛ 1 + β p
⎞
iC 5 + ⋅⎜ ⎟+ ⎜ ⎟ =1
βn ⎝ 1 + βn ⎠ βn ⎜ β p
⎝
⎟
⎠
i ⎛ β ⎞ i ⎛ β ⎞ ⎡ 1 ⎛ 1+ β p ⎞⎤
iC 5 + C 5 ⎜ n ⎟ + C 5 ⎜ n ⎟ ⎢ ⎜ ⎟⎥ = 1
βn ⎝ 1 + βn ⎠ βn ⎝ 1 + βn ⎠ ⎣ βn ⎜ β p
⎢ ⎝ ⎟⎥
⎠⎦
⎡ 1 ⎛ 20 ⎞ ⎤ ⎛ 1 ⎞ ⎡ 1 ⎛ 6 ⎞ ⎤
iC 5 ⎢1 + ⎜ ⎟ ⎥ + ⎜ ⎟ ⎢ ⎜ ⎟ ⎥ = 1
⎣ 20 ⎝ 21 ⎠ ⎦ ⎝ 21 ⎠ ⎣ 20 ⎝ 5 ⎠ ⎦
iC 5 (1.05048 ) = 1 iC 5 = 0.952 A
iC 4 = 0.0453 A
iE 3 = 0.00272 A
⎛5⎞
iC 3 = 0.00272 ⎜ ⎟
⎝6⎠
= 0.002267 A
⎛ 2.267 × 10−3 ⎞
VEB 3 = ( 0.026 ) ln ⎜ −12 ⎟ = 0.54206 V
⎝ 2 × 10 ⎠
VBE1 + VBE 2 = 1.74195 − 0.54206 = 1.19989
⎛ I ⎞ ⎛I ⎞
VT ln ⎜ C 2 ⎟ + VT ln ⎜ C 2 ⎟ = 1.19989
⎝ βn IS ⎠ ⎝ IS ⎠
⎛ 1.19989 ⎞
iC 2 = β n ⋅ I S exp ⎜ ⎟
⎝ 0.026 ⎠
= 20 (18.83) mA
iC 2 = 93.9 mA
iC 2 ⎛ β n ⎞ 93.9
iC1 = ⎜ ⎟= = 4.47 mA
β n ⎝ 1 + β n ⎠ 21
PQ 2 = I C 2 ( 24 − ( −20 ) ) = ( 0.0939 ) ( 44 ) = 4.13 W
PQ 5 = ( 0.952 ) ( −10 − ( −24 ) ) = 13.3 W