Esercizi Svolti e Commentati:
Microelectronics (B. Razavi, Wiley 2014)
Capitolo 5 Bipolar Amplifiers
Parte III
38
Av=? Z=10? VA=oo
RIN = rpi + (beta+1) RE
ROUT = RQ || ROOUT
Rup = (routQ || 1/gmu2) + R1
ROOUT = oo
Av = |Vout/Vin| = - Rup / (1/gmu1 + RE)
RIN = rpi + (beta+1) (1/gmu2 || rout2)
ROUT = RC
Av = - RC / (1/gmu1 + (1/gmu2 || rout2))
RIN = rpi1 + (1/gmu2 || rout2)(beta+1)
ROUT = RC
Av = - RC / (1/gmu1 + (1/gmu2 || rout2))
RIN = RB + rpi1 + (1/gmu2 || rout2)(1+beta)
ROUT = RC
Av = - RC / (1/gmu1 + (1/gmu2 || rout2)) . (rpi1 + (1/gmu2 || rout2)) / (RB + rpi1 + (1/gmu2 || rout2))
Vx = RIN / (RB + RIN)
Av = - RC / (1/gmu1 + RE + RB/(beta+1))
e
Vin RB
Vcc
RC
Vout
VB
Rin = RB + ru1 + (p+1)(1/gu2 || ru2)
Rout = RC
Av ≃ -RC / (1/gu1 + 1/gu2 || ru2 + RS/(beta+1))
N.B. Av,Beq = -gu1RC / (1 + (1/ru1 + gu1)RE)
gu1 >> 1/ru1
= -RC / (1/gu1 + RE)
39. VA = oo
A
RIN = ru1 + RE(beta+1)
Rout = RC + (1/gu2 || ru2)
Av ≃ -Rout / (1/gu1 + RE)
B
RIN = ru1 + RE(beta+1)
Rout = (1/gu2 || ru2)
Av ≃ -Rout / (1/gu1 + RE)
(C)
RIN = re1 + (1/gm3) || rpi3
ROUT = RC + (1/gm2) || rpi2
Av = - ROUT / (1/gm1 + (1/gm3) || rpi3)
(D)
RIN = rpi1 + (beta + 1)RE
ROUT = RC || rpi2
Av = - RC || rpi2 / (1/gm1 + RE)
ROUT = ro + (1 + gm1ro)RE ≈ (1 + gmRE)ro
ROUT,A = ro2 + (1 + gm2ro2)RE
RE = 1/gm2
ROUT,B = ro2 + (1 + gm2ro2)ro2
ROUT,A < ROUT,B -> CASCODE TOPOLOGY
41.
(A)
ROUT = ro1 + (1 + gm1ro1)(1/gm2 || ro2)
(B)
ROUT = ro1 + (1 + gm1ro1)RE
RE = (1/gm + RB/(beta + 1)) || ro2 ?
Rout = ro1 + (1 + gu1ra)(R1 || rpi2)
42.
(A)
Vcc = 2.5V DC-ANALYSIS beta = 100
C1 = OPEN IS = 8.10-16A Va = oo
Ib = (Vcc - (VBE + VE))/RB = (Vcc - VBE - IERE)/RB = (Vcc - VBE)/((beta+1)RE + RB)
VBE = 0.750V => Ib = 15.86 uA => Ie = 1.586 uA
VBE = 0.736V => Ib = 16.02 uA => Ie = 1.602 uA
VBE = 0.736V => OK
gm = Ic/Vt = (16.23,2)-1
rpi = beta/gu = 1.63kOhm
from small-sig. C1 short.
|Av| = vout/vin = vx/vin = 8.6
|vout/vx| = Rcgu/(1 + guRE)
vx/vin = 1
(RB || Rin)
(B)
DC-ANALYSIS. C1, C2 OPEN.
Ib = (Vcc - VBE - IERE)/RB
=> Ib = (Vcc - VBE)/((beta+1)RE + RB) = 252K
VBE = 0.750 => Ia = 6.94 uA => Ic = 0.69 uA => VBE = 0.715 => Ib = 7.08 uA
=> Ic = 0.708 uA VBE = 0.717 V
gm = (36.72)-1 = 0.027 S
rpi = 370kOhm
RE = 0 C2 BIased
|Av| = Rcgu/(1 + guRE) . Req/(Req + Rig)
Req = RB || rpi.
c
VIN 1k C1 34k VCC1k1kRC = 10k500 2kC2
DC ANALYSIS
VCCReqVrefVref = 1,1VReq = 6,16kQ
RC = 10kVoutRE = 2,900
IB = (Vref - VBE) / ((beta+1)RE + Req) = 23,9uA
VBE = 0,7 V => IB = 6,9 uA => IC = 0,69 uAVBE = 0,715V => IB = 6,89 uA => IC = 0,689 uAVBE = 0,676 => IB = 7,00 uA => IC = 0,700 uAVBE = 0,745 => IB = 6,89 uA => IC = 0,689 uA
VBE = 0,687 V IC = 0,69 uAIB = 1,16 uA
gm = 0,00631 S = (158,5Q)-1rpi = 15,87k
AC ANALYSIS
VIN Rsig X RthevSRthevVCC600
|Vx| / |VIN| = 5,63k / (5,63k + 1k) = 0,85
|Vout| / |Vx| = RCeq / (1 + gmRE) = 15,8
|Vx| / |VIN| = Rthev || Rin / (Rthev || Rin + Rsig)
Rin = rpi + (beta+1)RE = 65,87k
=> |Av| = 13,43.
43.
IB = 20uAbeta = 100VA = 00
IC = beta IB = 2uA
gm = IC / VT = 0,0769(32V)-1VT = 1,307K
Av = gm RC = 38,25Rin = 1/gm = 13QRout = RC = 500Q
44. VA = oo
IC = 2 mA
betanpn = betapnp = 100.
Rin = (1/gm1 || rpi1)
Rout = RC + (1/gm2 || rpi2)
Av = gm1 [RC + (1/gm2 || rpi2)]
B
Rin = (1/gm1 || rpi1)
Rout = oo.
Av = 90
C
Rin = RE || rpi1
Rout = RC + (1/gm2 || rpi2)
|Av| = gm1 (RC + 1/gm2 || rpi2)
45. A
IC = 2 mA beta = 100 VA = oo.
B
Rin = 1/gm1 || rpi1 + R2/(beta + 1)
46.
Re = 75
Rc = 1k
Rin = RE + (1/gm || rct)
47.
R1 = 10k
R2 = 2k
RC = 1k
RE = 330
VCC = 2.5V
beta = 100
Is = 8 10^-16A
VA = 00
a) Bias
b) Voltage gain
DE analysis -> CB open.
Vth = R2/(R1+R2) Vcc = 1.1V
Req = 6.67k
Req Ib = Vth - VBE - IERE
IC = (Vth - VBE)/(Req/beta + RE) = 400
VBE = 0.7V => IC = 1uA
VBE = 0.720V => IC = 0.94uA
VBE = 0.722V => IC = 0.945uA
VBE = 0.7220V
VCE = 0.722V
VCE = 0.722V
VCE = 0.7220V
VCE > VB => Q1 forward.
gm = 0.0365 = (27.5mV)^-1
rpi = 2.77k
Bias point:
VBE = 0.722V
IC = 0.945mA
IB = 9.45uA
VC = VCC - IC RC = 1.555V
VB = VBE + IERE = 1.032V
AC analysis CB short.
Av = gm RC = 36
48.
VA = oo
CB large => AC short circuit.
R2 shorted
RIN = 1/gm || rpi1
ROUT = R1
AV = gm R1
49.
VA = oo. CB large => AC gnd. R2 shorted
RIN = 1/gm1 || rpi2
ROUT = R2 || (1/gm2 || rpi2)
AV = gm1 (R2 || (1/gm2 || rpi2))
50.
VCC = 2.0V
RC = 1K
RB = 10K
RE = 500
VA < oo
beta = 100
gm = (26u)-1
Vout/Vin = (Vout/Vx)(Vx/Vin)
|Vout/Vx| = ?
Vout = - (I1 + gm vpi)RC
I1 = (Vout - Ve)/ro
Vout = - ((Vout - Ve)/ro + gm vpi)RC
Ve = IE RE = Vx - vpi
vpi = Vx - Ve = IE rpi = (Ve/RE - Vout/RC)rpi
=> Ve = (Vx - Vout vpi)RE/(rpi + RE)
51.
VA = oo
IS = 2IS2
|Av1| = |VOUT1 / VIN| = RC / (1 / gm1 + RE)
|Av2| = |VOUT2 / VIN| = RC / (1 / gm + RE)
gm1 = IC1 / VT
gm2 = IC2 / VT => gm1 = gm2 / 2 => |Av1| = |Av2| / 2.
gmvTC = -Vout / RC => vTC = -Vout / (gmRC)
IE = RE + VIN = -vTC
(gmvTC + vTC / rTC)RE + VIN = vTC
=> - (gm + 1 / rTC)RE (VOUT / gmRC) + VIN = -VOUT / (gmRC)
[(gm + 1 / rTC)RE + 1] VOUT / (gmRC) + VIN = 0
VOUT / VIN = - gmRC / ((gm + 1 / rTC)RE + 1) ~ RC / (1 / gm + RE).
52
Vout = -(Ic + gmvpi)RC Ic = (Vout - Ve) / ro
Ve = - gm vpi / beta (rpi + RB)
Vout = p(vi)
vi = A Vout
Vin = VE - IERE
Vout / Vin = [gm(rpi + RB)RC / beta ro + gmRC] / [gm(1 + RC/ro)(rpi + RB)(1 + RE/ro) + (1 + 1/beta)gm(1 + RC/ro)RE - RE/ro[gm(rpi + RB)RC / beta ro + gmRC]
ro -> ∞
Av = gmRC / gm(rpi + RB) + (beta + 1)/beta gmRE = RC / (rpi + RB + RE)
= RC / (RE + RB/(beta + 1) + 1/gm)
52.
Vcc
R1 = 10k
R2 = 10k
RE = 600
IC: Av = 0,9
Vcc
VA =∞
RB = R1 || R2
RB has no effect on the voltage since X so long as vin remains ideal
RB != input source impedance
Vout / Vin = Vout / Vx · Vx / Vin
Vi / Vin = [rpi + (beta + 1)RE] / [R1 || R2 + rpi + (beta + 1)RE]
-Vout / Vx = RE
Av = RE / (1/gm + RE) = RE / [1 + REu]
1/gm = RE / |Av| - RE |A| = RE(1 - Av2 / Av)
gm = Av / RE · 1 / (1 - Av2) = (0,00795) = (126 Ω)-1 = IC / VT
⇒ IC = gmVT = 0,2054 µA.
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Esercizi di Elettronica analogica sugli amplificatori bipolari - Parte I
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