3/10/2015 Chapter 5 Represents the AC characteristics of the transistor. re model Hybrid model Hybrid equivalent model ECET 257 Consumer Power Electronics, PNC 2 1 3/10/2015 ECET 257 Consumer Power Electronics, PNC 3 Uses circuit elements that approximate the behavior of the transistor. ECET 257 Consumer Power Electronics, PNC 4 2 3/10/2015 1. 2. 3. 4. Replace all DC sources with short circuits Replace all capacitors with open circuits Remove all components bypassed by 1 & 2 Redraw final circuit ECET 257 Consumer Power Electronics, PNC 5 BJTs are basically current-controlled devices; therefore the re model uses a diode and a current source to duplicate the behavior of the transistor. One disadvantage to this model is its sensitivity to the DC level. This model is designed for specific circuit conditions. ECET 257 Consumer Power Electronics, PNC 6 3 3/10/2015 The diode (B-E) can be replaced by the resistor re. re is resistor equivalent, not to be confused with RE, or resistance of the emitter ECET 257 Consumer Power Electronics, PNC 7 ECET 257 Consumer Power Electronics, PNC 8 Input impedance: Output impedance: 4 3/10/2015 Voltage gain: Current gain: Current: Phase Shift: ECET 257 Consumer Power Electronics, PNC 9 ECET 257 Consumer Power Electronics, PNC 10 Input impedance: Output impedance: 5 3/10/2015 Voltage gain: Current gain: Current: Phase shift: ECET 257 Consumer Power Electronics, PNC Find ◦ ◦ ◦ ◦ Zi Vo Av Zo 11 Vi=10 mV∠0 IE=0.5 mA ∠0 α=0.980 RL = 1.2 kΩ Ro =∞Ω ECET 257 Consumer Power Electronics, PNC 12 6 3/10/2015 ECET 257 Consumer Power Electronics, PNC 13 Input impedance: Output impedance: Voltage gain: Current gain: Phase Shift: ECET 257 Consumer Power Electronics, PNC 14 7 3/10/2015 The input is applied to the base The output is taken from the collector High input impedance Low output impedance High voltage and current gain Phase shift between input and output is 180 ECET 257 Consumer Power Electronics, PNC 15 AC equivalent re,model ECET 257 Consumer Power Electronics, PNC 16 8 3/10/2015 Input impedance: Output impedance: Current gain: Voltage gain: Current gain from voltage gain: ECET 257 Consumer Power Electronics, PNC 17 Find ◦ ◦ ◦ ◦ re Zi Zo Av ECET 257 Consumer Power Electronics, PNC 18 9 3/10/2015 re model requires you to determine , re, and ro. ECET 257 Consumer Power Electronics, PNC Input impedance Voltage gain Output impedance 19 Current gain Current gain from Av ECET 257 Consumer Power Electronics, PNC 20 10 3/10/2015 Find ◦ ◦ ◦ ◦ re Zi Zo Av Vcc = 16 V R1 =39 kΩ R2= 4.7 k Ω RC=3.9 k Ω RE=1.2 k Ω β=100 Ro = 50 k Ω ECET 257 Consumer Power Electronics, PNC 21 ECET 257 Consumer Power Electronics, PNC 22 11 3/10/2015 No capacitor parallel to RE. If capacitor is present, RE is bypassed and normal CE format is used ECET 257 Consumer Power Electronics, PNC 23 Input impedance: Output impedance: ro can be ignored if ≥ 10( + ) ECET 257 Consumer Power Electronics, PNC 24 12 3/10/2015 Voltage gain: Current gain: Current gain from Av: ECET 257 Consumer Power Electronics, PNC Find ◦ ◦ ◦ ◦ re Zi Zo Av 25 Vcc = 10 V RB= 390 kΩ RC= 2.2 k Ω RE=1.2 k Ω β=140 ro= 100 k Ω ECET 257 Consumer Power Electronics, PNC 26 13 3/10/2015 Base input (high Z), Emitter output (low Z) Input and output are in phase Opposite Z configuration of FB, commonly used for Z matching ECET 257 Consumer Power Electronics, PNC 27 ECET 257 Consumer Power Electronics, PNC 28 Input impedance: Output impedance: 14 3/10/2015 Voltage gain: Current gain: Current gain from voltage gain: ECET 257 Consumer Power Electronics, PNC re βre Zi Zo Av 29 Vcc = 10V RB=300 kΩ RE=3 kΩ β=150 RO=100 k Ω ECET 257 Consumer Power Electronics, PNC 30 15 3/10/2015 ECET 257 Consumer Power Electronics, PNC 31 The input is applied to the emitter The output is taken from the collector Low input impedance. High output impedance Current gain less than unity Very high voltage gain No phase shift between input and output ECET 257 Consumer Power Electronics, PNC 32 16 3/10/2015 Input impedance: Output impedance: Voltage gain: Current gain: ECET 257 Consumer Power Electronics, PNC • • • • 33 A variation of the common-emitter fixed-bias configuration Input is applied to the base Output is taken from the collector There is a 180 phase shift between the input and output ECET 257 Consumer Power Electronics, PNC 34 17 3/10/2015 Input impedance: Output impedance: Voltage gain: Current gain: ECET 257 Consumer Power Electronics, PNC Unloaded amp will always have the highest gain ◦ 35 > > Ideal amp ◦ Low input Z ◦ High output Z ECET 257 Consumer Power Electronics, PNC 36 18 3/10/2015 Amplitude of the applied signal that reaches the input of the amplifier Internal source impedance effect on gain ECET 257 Consumer Power Electronics, PNC 37 ECET 257 Consumer Power Electronics, PNC 38 19 3/10/2015 ECET 257 Consumer Power Electronics, PNC 39 Must have load impedance Formula applies to all configurations =− ECET 257 Consumer Power Electronics, PNC 40 20 3/10/2015 Find AVL for ◦ RL = 4.7K ◦ RL = 0.5K ECET 257 Consumer Power Electronics, PNC 41 β = 120 Av = - 3.1 Find Vcc ECET 257 Consumer Power Electronics, PNC 42 21 3/10/2015 When using the chart on Pages 292-295, ensure the circuit meets the requirements for the equation when ro and re are involved. Requirements are noted in the sections covering the configurations. ECET 257 Consumer Power Electronics, PNC ECET 257 Consumer Power Electronics, PNC 43 44 22 3/10/2015 Useful when individual measurements are impossible or impractical With Vi set to 0 V: The voltage across the open terminals: where AvNL is the noload voltage gain 45 ECET 257 Consumer Power Electronics, PNC 46 No-load ◦ ECET 257 Consumer Power Electronics, PNC = To solve ◦ Find RT using II ◦ Find Vi 23 3/10/2015 Vs = 20 mV Rs= 30 Ω II = 50 uA Vo = 3.6 V Find AVNL ECET 257 Consumer Power Electronics, PNC Given Amp PCB specs, find 47 RS=0.2 kΩ AVNL=-480 Zi= 4 kΩ Zo = 2 kΩ ◦ AVL with RL = 5.6 kΩ ◦ Ai with RL = 5.6 kΩ ECET 257 Consumer Power Electronics, PNC 48 24 3/10/2015 1. 2. 3. 4. 5. The output of one amplifier is the input to the next amplifier Overall voltage gain is determined by the product of gains of the individual stages The DC bias circuits are isolated from each other by the coupling capacitors The DC calculations are independent of the cascading The AC calculations for gain and impedance are interdependent = × × ECET 257 Consumer Power Electronics, PNC 49 ECET 257 Consumer Power Electronics, PNC 50 ⋯ =− 25 3/10/2015 Voltage gain: Input impedance, first stage: Output impedance, second stage: ECET 257 Consumer Power Electronics, PNC 51 ECET 257 Consumer Power Electronics, PNC 52 This example is a CE–CB combination. This arrangement provides high input impedance but a low voltage gain. The low voltage gain of the input stage reduces the input capacitance, making this combination suitable for highfrequency applications. 26 3/10/2015 The Darlington circuit provides very high current gain, equal to the product of the individual current gains: D = 1 2 The practical significance is that the circuit provides a very high input impedance. ECET 257 Consumer Power Electronics, PNC 53 Base current: Emitter current: Emitter voltage: Base voltage: AC analysis based on circuit configuration ECET 257 Consumer Power Electronics, PNC 54 27 3/10/2015 Find DC Bias voltages and currents ◦ ◦ ◦ ◦ ◦ ◦ IB1 IC2 VC1 VE2 VB1 VCE2 ECET 257 Consumer Power Electronics, PNC 55 This is a two-transistor circuit that operates like a Darlington pair, but it is not a Darlington pair. It has similar characteristics: • High current gain • Voltage gain near unity • Low output impedance • High input impedance The difference is that a Darlington uses a pair of like transistors, whereas the feedback-pair configuration uses complementary transistors (PNP and NPN). ECET 257 Consumer Power Electronics, PNC 56 28 3/10/2015 Q. 18, 38 ◦ Use exact analysis Q. 44b ◦ Rewrite as “Find the total AVL and AVS for the system” ECET 257 Consumer Power Electronics, PNC 57 29