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Basic BJT Small-Signal Model
VC VE VB VC VE rp + V - gmV ro VB VB VE VC rp= b UT / IC gm = IC / UT ro = VA / IC Key Terms: gm rp= b ; gm ro = VA / UT Current Gain Voltage Gain
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Computing Small-Signal Models
Forward-Active Model: (Exponential Form) VBE/UT VCE/VA IC = IC0 e e dIC VBE/UT VCE/UT gm = = IC0 e e (1 / UT) = IC / UT dVBE dIC VBE/UT VCE/VA 1/ ro = = IC0 e e (1 / VA) = IC / VA dVCE
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Basic BJT Small-Signal Model
Current Gain Voltage Gain Iout Vdd GND ro Iref Iin Vin Vout GND Vout + V - GND Vin rp Iout gmV + V - rp Iin GND GND gmV GND GND GND AV = gm ro = VA / UT AI = gm rp= b
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Basic Frequency Effects
Cje = base-emitter depletion capacitance (forward biased) Cjbc = base-collector depletion capacitance (reversed biased) Cb = Base-Charging Capacitance of the Small Signal BJT Model Modifying Charge from the Base when changing Base voltage: Cb = tF gm Cp = Cje + Cb; Cm = Cjbc
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BJT Small-Signal Model
Cm VB VC + V - ro Cp rp gmV VE Basic measures of Frequency Characteristics: fT
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Frequency Dependence of a BJT
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Current Gain versus Frequency
2 10 1 b0 10 Collector current / Base current 10 fT 3 4 5 6 7 8 9 10 10 10 10 10 10 10 Frequency (Hz)
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Frequency Dependence of a BJT
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Complete Small-Signal Model
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Additional Effects Series Resistance (rb, rc, re)
---- Finite conductivity of doped regions Collector-Base Resistance of the Small Signal BJT Model (rµ) In general, rµ ³ 10 boro for the npn BJT and about 2-5 boro for the lateral pnp BJT
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Complete Circuit Element Model
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