9/12/2013 In this chapter, we will: Microelectronics Discuss the physical structure and operation of the bipolar junction transistor. Circuit Analysis and Design Donald A. Neamen Understand the dc analysis and design techniques of bipolar transistor circuits. Chapter 5 Examine three basic applications of bipolar transistor circuits. The Bipolar Junction Transistor Neamen Microelectronics, 4e McGraw-Hill Chapter 5-1 Neamen Cross Section of Integrated Circuit npn Transistor Microelectronics, 4e McGraw-Hill Chapter 5-2 Modes of Operation Forward-Active B-E junction is forward biased B-C junction is reverse biased Saturation B-E and B-C junctions are forward biased Cut-Off B-E and B-C junctions are reverse biased Inverse-Active (or Reverse-Active) B-E junction is reverse biased B-C junction is forward biased Neamen Microelectronics, 4e McGraw-Hill Chapter 5-3 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-4 1 9/12/2013 npn BJT in Forward-Active Neamen Microelectronics, 4e McGraw-Hill Chapter 5-5 Electrons and Holes in npn BJT Neamen Microelectronics, 4e McGraw-Hill Chapter 5-6 Circuit Symbols and Current Conventions Electrons and Holes in npn BJT With a + potential across the C-E terminals. If a positive voltage is applied to the base (>0.6V), the B-E pn junction is forward biased. The E side electrons cross the pn junction and many electrons are swept to the positive C side voltage (since the p base material is thin). This results in electron flow from E to C. (Conventional current flow from C to E). Neamen Microelectronics, 4e McGraw-Hill Chapter 5-7 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-8 2 9/12/2013 Current Relationships Common-Emitter Configurations iE = iC + iB iC = βiB iE = (1 + β iB ) iC = αiE β= Neamen α 1−α Microelectronics, 4e McGraw-Hill Chapter 5-9 Neamen Current-Voltage Characteristics of a Common-Emitter Circuit Neamen Microelectronics, 4e McGraw-Hill Chapter 5-11 Microelectronics, 4e McGraw-Hill Chapter 5-10 Early Voltage/Finite Output Resistance Neamen Microelectronics, 4e McGraw-Hill Chapter 5-12 3 9/12/2013 DC Equivalent Circuit for npn Common Emitter Neamen Microelectronics, 4e McGraw-Hill DC Equivalent Circuit for pnp Common Emitter Chapter 5-13 Neamen Load Line Microelectronics, 4e McGraw-Hill Chapter 5-14 Problem-Solving Technique: Bipolar DC Analysis 1. Assume that the transistor is biased in forward active mode a. VBE = VBE(on), IB > 0, & IC = βIB 2. Analyze ‘linear’ circuit. 3. Evaluate the resulting state of transistor. a. If VCE > VCE(sat), assumption is correct b. If IB < 0, transistor likely in cutoff c. If VCE < 0, transistor likely in saturation 4. If initial assumption is incorrect, make new assumption and return to Step 2. Neamen Microelectronics, 4e McGraw-Hill Chapter 5-15 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-16 4 9/12/2013 Voltage Transfer Characteristic for npn Circuit Neamen Microelectronics, 4e McGraw-Hill Chapter 5-17 Voltage Transfer Characteristic for pnp Circuit Neamen Common Emitter with Voltage Divider Biasing and Emitter Resistor Microelectronics, 4e McGraw-Hill Chapter 5-18 Microelectronics Circuit Analysis and Design Donald A. Neamen Chapter 6 Basic BJT Amplifiers VTH = [ R2 /( R1 + R2 )]VCC Neamen Microelectronics, 4e McGraw-Hill Chapter 5-19 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-20 5 9/12/2013 Common Emitter with Time-Varying Input In this chapter, we will: Understand the concept of an analog signal and the principle of a linear amplifier. Investigate how a transistor circuit can amplify a small, time-varying input signal. Discuss and compare the three basic transistor amplifier configurations. Neamen Microelectronics, 4e McGraw-Hill Chapter 5-21 Neamen Neamen Chapter 5-22 ac Equivalent Circuit for Common Emitter IB Versus VBE Characteristic iB ≅ I BQ (1 + Microelectronics, 4e McGraw-Hill vbe ) = I B + ib VT Microelectronics, 4e McGraw-Hill Chapter 5-23 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-24 6 9/12/2013 Small-Signal Hybrid π Model for npn BJT gm = rπ = Small-Signal Equivalent Circuit Using Common-Emitter Current Gain I CQ VT βVT I CQ g m rπ = β Phasor signals are shown in parentheses. Neamen Microelectronics, 4e McGraw-Hill Chapter 5-25 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-26 Problem-Solving Technique: BJT AC Analysis Small-Signal Equivalent Circuit for npn Common Emitter circuit 1. Analyze circuit with only dc sources to find Q point. 2. Replace each element in circuit with smallsignal model, including the hybrid π model for the transistor. 3. Analyze the small-signal equivalent circuit after setting dc source components to zero. Av = −( g m RC )( Neamen Microelectronics, 4e McGraw-Hill rπ ) rπ + RB Chapter 5-27 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-28 7 9/12/2013 Hybrid π Model for npn with Early Effect ro = Neamen Hybrid p Model for pnp with Early Effect VA I CQ Microelectronics, 4e McGraw-Hill Chapter 5-29 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-30 h-Parameter Model for npn Expanded Hybrid π Model for npn ܸ = ℎ ܫ + ℎ ܸ ܫ = ℎ ܫ + ℎ ܸ hie = rb + rπ rµ h fe = β Neamen Microelectronics, 4e McGraw-Hill Chapter 5-31 Neamen Microelectronics, 4e McGraw-Hill hre ≅ rπ rµ hoe = 1+ β 1 + rµ ro Chapter 5-32 8 9/12/2013 Common Emitter with Voltage-Divider Bias and a Coupling Capacitor Neamen Microelectronics, 4e McGraw-Hill Chapter 5-33 npn Common Emitter with Emitter Resistor Small-Signal Equivalent Circuit – Coupling Capacitor Assumed a Short Neamen Microelectronics, 4e McGraw-Hill Chapter 5-34 Small-Signal Equivalent Circuit: Common Emitter with RE ܸ = −ߚܫ ܴ ܸ ܫ = ൘( ݎ+ ߚ + 1 ܴ ) గ ா ܴ ܸ = ܸ௦ ( ) ܴ + ܴ௦ Rib = rπ + (1 + β ) RE Ri = R1 R 2 Rib Av = Neamen Microelectronics, 4e McGraw-Hill Chapter 5-35 Neamen Microelectronics, 4e McGraw-Hill − βRC Ri ( ) rπ + (1 + β ) RE Ri + RS Chapter 5-36 9 9/12/2013 RE and Emitter Bypass Capacitor Neamen Microelectronics, 4e McGraw-Hill Chapter 5-37 dc AND ac Load Lines: RE and Emitter Bypass Capacitor Neamen Problem-Solving Technique: Maximum Symmetrical Swing Microelectronics, 4e McGraw-Hill Chapter 5-38 Common-Collector or Emitter-Follower Amplifier 1. Write dc load line equation that relates ICQ and VCEQ. 2. Write ac load line equations that relates ic and vce 3. In general, ic = ICQ – IC(min), where IC(min) is zero or other minimum collector current. 4. In general, vce = VCEQ – VCE(min), where VCE(min) is some specified minimum collector-emitter voltage. 5. Combine above 4 equations to find optimum ICQ and VCEQ. Neamen Microelectronics, 4e McGraw-Hill Chapter 5-39 Neamen Microelectronics, 4e McGraw-Hill Chapter 5-40 10 9/12/2013 Small-Signal Equivalent Circuit: Emitter Follower Output Resistance: Emitter Follower Ro = Neamen Microelectronics, 4e McGraw-Hill Chapter 5-41 Neamen rπ RE ro 1+ β Microelectronics, 4e McGraw-Hill Chapter 5-42 11