BJT 1 Examples
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Transcript of BJT 1 Examples
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BJT’s
pn
Collector
CiC
BiB
n
Base
EiE
Active Base Region
Emitter
Emitter-BaseJunction Collector-Base
Junction
Figure 5.1(a) - Simplifie cross-section of an npn transistor !it" currents t"at occur uring
#normal# operation
p$
p$
p$
p$
p
p
Active %ransistor
Region
iB
iC
iE
p
p
p
p
Figure 5.1(&) - Cross-section of an integrate npn &ipolar 'unction transistor
(&)
Base (B)
Collector (C)
Emitter (E)
iC
iE
iB
n
Collector
pBase
n
Emitter
vBC
vBE
iC
iB
iE(a)
Figure 5 . - (a) eali*e npn tr ansis tor s tr ucture for a general &ias conition
(&) Circuit s+m&ol for t"e npn transistor
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Forward Characteristics
n
p
n
Collector
Base
Emitter
iE
iB
iC
vBE
iF
C
B
E
Fβ
iF
n
p
n
Collector
Base
Emitter
iE
iB
iC
vBE
iF
C
B
E
Fβ
iF
n
p
n
Collector
Base
Emitter
iE
iB
iC
vBE
iF
C
B
E
Fβ
i F
Figure 5., - npn transistor !it" vBE applie an vBC .
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Reverse Characteristics
n
p
n
Collector
Base
Emitter
iE
i B
iR
i C
vBC
C
E
B
i R
R β
Figu re 5./ - %ran sistor !it" vBC ap plie an vBE .
Table 5.1
Common-Emitter and Common-Base
Current Gain Comparison
αF or αR
.1 .11
.5 1
.0 0
.05 10
.00 00
.00 /00
βF = αF
1 − αF or βR =
αR
1 − αR
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ENGR 311 – Electronic Devices and Circuits Octoer !"# !$$$
Transistor %odel& Current '()li*ier
A Summar+ For Clarification (assume npn for t"e follo!ing general rules2properties 3 for pnp reverse
polarities)
Rules 2 4roperties
1 3 %"e collector must &e positive t"an t"e emitter.
3 %"e &ase-emitter an &ase-collector circuits &e"ave lie ioes. 6ormall+ t"e &ase-emitter ioe isconucting an t"e &ase-collector ioe is reverse-&iase
, 3 7"en 1 an are o&e+e c is proportional to & (c &eta . &)Bot" & an c follo! to t"e emitter.
6ote8 t"e collector current is not ue to for!ar conuction of t"e &ase-collector ioe9 t"at ioe is reverse-
&iase. Just t"in of it as :transistor action.;
4ropert+ , gives t"e transistor its usefulness8 a small current flo!ing into t"e &ase controls a muc" larger
current flo!ing into t"e collector.
6ote t"e effect of propert+ . %"is means +ou can (?& ?e $ ?&e) (for an npn).
et me emp"asi*e again t"at +ou s"oul not tr+ to t"in of t"e collector current as ioe conuction. t isn
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+c – ,ce Characteristic *or an n)n Transistor
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+c- ,e Characteristics
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Biasin.
For common emitter amplifier
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ENGR 311 - BJTs – E/ercises - Octoer !0# !$$1
Eamples Solution
Eample 1 - Beta 1= vBE .? atiC 1mA. Design circuit so t"at a
current of mA flo!s t"roug" t"e
collector an a voltage of $5? appears att"e collector.
Eample - n t"e circuit &elo! vC -.?. f Beta 5= fin E= B= C an
?C.
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Eample , 3 n t"e circuit &elo!= ?&
1?= ?E 1.?. 7"at are alfa an &etafor t"is transistor 7"at voltage ?C o
+ou epect at t"e collector.
Eample / - Beta 1 3 Determine all
noe voltages an &ranc" currents.
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Eample 5
Determine t"e voltages at all noes an current t"roug" all &ranc"es.
Assume &eta 1 an &eta . Assume 1 is in t"e active moe.
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ENGR 311 - Gra)hical Re)resentation o* Transistor Characteristics - Octoer 31# !$$1
Conceptual circuit for measuring t"e iC -vCE c"aracteristics of t"e BJ%. 2 %"e iC -vCE c"aracteristics of a practical BJ%.
%"e iC -vCB c"aracteristics for an npn transistor in t"e active moe
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Determine t"e voltages at all noes an t"e currents at all &ranc"es in t"e circuit &elo!.
Solution
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The Transistor 's 'n '()li*ier – DC Conditions
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The Collector Current and The Transconductance
The Base Current and the +n)ut Resistance at the Base
(a) Conceptual circuit to illustrate t"e operation of t"e transistor of an amplifier. 2 %"e circuit of
(a) !it" t"e signal source vbe eliminate for c (&ias) anal+sis.
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Transistor as 'n '()li*ier - (all i.nal '))ro/i(ation
%ransconuctance (gm)= nput Resistance at t"e Base (r π)= nput Resistance at t"e Emitter (re)= ?oltage Gain
Eercise /. an /.,
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Small-Signal EHuivalent Circuits Ioels
Amplifier Circuit 7it"out DC Sources
+&ri-π
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%"e % Ioel
Application of t"e Small-Signal EHuivalent Circuits
1
,
/
5
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Eample /.0
DC Anal+sis
Small-Signal Anal+sis
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Eample /.11
Determine voltage gain in t"e circuit &elo!
DC Anal+sis
Small-Signal Ioel Small-Signal Anal+sis Directl+ on Circuit
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Grap"ical Anal+sis
Grap"ical etermination of t"e signal components vbe= ib= ic= an vce !"en a signal component vi is
superimpose on t"e c voltage V BB.
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Biasing %"e BJ% For Discrete-Circuit Design
Basic Single-Stage BJ% Amplifier Configurations
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%inorit4-Carrier Trans)ort +n the Base Re.ion
(&)
7
n( )
i%= + H A D n
n
n()
n(7)
6 6
iC
Collector BaseEmitter
4
Space C"arge Regions
iE &o
&o(p = n )
i%
vBE
vBC
Fβ
F β
R
R
$ $iB
(a)
REC
Figure 5.15 - (a) Curren ts in t" e &ase region of a n pn tr an sistor
(&) Iin orit+ carrier concen tra tion in t" e &ase of t" e npn tra ns istor
i% HADn. n2 -HADnn. (n&o27&). Kep(v&e2?t) 3 ep(v&c2?t)L
s HADn.(n&o27&) (HADn.niM )26a&.7&
n&o eHuili&rium electron ensit+
A cross-sectional area of t"e &ase region
7& &ase !it"Dn iffusit+ (cmM2s)
6a& oping concentration in &ase of transistor<
ni intrinsic-carrier concentration (1M1.cmM,)
n&o niM 2 6a&
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Base Transit Ti(e
%o turn t"e BJ% minorit+-carrier c"arge must &e introuce into t"e &ase to esta&lis" t"e graient.
%"e for!ar transit time tau-f represents t"e time constant associate !it" storing t"e reHuire c"arge in t"e &ase region an is efine &+
2%
Di**usion Ca)acitance
For t"e &ase-emitter voltage an "ence t"e collector current in t"e BJ% to c"ange= t"e c"arge store in t"e &ase
region also must c"ange.
7
n( )
n()
n(7) n &on &o
Figure 5.1>(a) - Ecess minorit+ c"arge store in t"e &ipolar &ase region
7
n( )
n(7) n &o
n &o
n(= ? )BE1
n(= ? )BE
∆
Figure 5.1>(&) - Store c"arge c"an ges as vBE c"an ges
%"is c"ange in c"arge !it" v&e can &e moele &+ a capacitance CD
CD (c2?%). τf
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Fre5uenc4 De)endence o* the Co((on-E(itter Current Gain
B
C
E
iB
iC
iE
B
iB
E
vBE
C
$
-
i β iC F B
E Fi ( β $ 1) i
B
ep ( )S
vBE
?%i
C
Figure 5. - Simplifie moel for t"e npn transistor for t"e for!ar-active region
B
i B
iE
E
C
i β iC F B$-. ? vBE
i C
Figure 5.1 - Furt"er simplification of t"e npn moel for t"e for!ar-active region
Beta-cutoff FreHuenc+
1 01 1 1 >1 51 /1
-1
1
11
1
1,
FreHuenc+ (J*)
C o m m o n -
E m i t t e r C u r r e n t G a i n
f %
Figure 5. - Common-emitter current gain β vs. freHue nc+
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Transconductance
Relates c"anges in ic to c"anges in v&e
gm ic2v&e (N-point)
gm c 2?%
CD gm.τf
The Earl4 E**ect (James Earl+ form Bell a&s)
Eperimentall+ emonstrate t"at !"en t"e output curves are etrapolate &ac to a point of *ero collector
current= t"e curves all intersect at a constant voltage point vce -?A
-15? -1? -5? ? 5? 1? 15?
Collector-Emitter ?oltage
/.mA
.mA
A
Collector
Cur
r ent
1 uA
uA
> uA
/ uA
uA
A-?
B
B
B
B
B
Figure - 5 ., %ransistor outp ut c "aracter ist ics ientif+ing t" e ear l+ voltage ?A
Ioeling t"e Earl+ Effect
ic
Betaf
i&
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Tolerances in Bias Circuits
7orst Case Anal+sis
R C
R E
R 1
R ,> Ω
1 Ω
Ω
1> Ω
? $1 ?CC
1
)C
?EF
R EF
$1( ?
)B
R E
1> 5 Ω
1( 5 Ω
R C
((5 Ω
/ ?
)E
?CC
Stu+ t"e operation of t"e transistor consiering tolerances (!orst case ana+sis) in t"e circuit. Assume t"at t"e
1? po!er suppl+ "as a 5O tolerance an t"e resistors "ave 1O tolerance. Assume also t"at t"e voltage rop
in R E can &e neglecte= an &eta is large.
?E (ma= min)
C (ma= min)
?CE (ma= min)
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%onte Carlo 'nal4sis
4erform Ionte Carlo Anal+sis on previous circuit assuming t"e ranom values to
?cc= R1= R= Rc= Re= an &eta. (Pse Ecel an2or 4spice).
Calculate
?E
R E
B
C
E
?C ?CC 3 C.R C 3 E.R E
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Electronic Devices and Circuits – 11676$$
%onte Carlo 'nal4sis – 8sin. 9s)ice
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4ro&e Qutput
c()= &()= ?ce