Steady current established by a dc supply Effect of a control element on
small-signal ac analysis
\
The Importance Parameters
Two-port system
Input impedance:
Voltage Gain
Phase relationship
For the typical transistor amplifier, the input and output signals are either 180° out
of phase or in phase
.THE r
eTRANSISTOR MODEL
BJT transistor amplifiers are referred to as current-controlled devices.
Common Base Configuration
Typical values of the Zo are in the mega ohm range
Defining Zo.
If the applied signal is set to zero, then Ic is 0 A,resulting
(Vo and Vi are 18 out of phase)
00
Two-port system
The term “term” or h-parameter was chosen because the mixture of variables( V and I)
Complete hybrid equivalent circuit
Short-circuit input–impedance parameter:
Open-circuit reverse transfer voltage ratio parameter:
Short-circuit forward transfer current ratio parameter:
Open-circuit output admittance parameter:
The common emitter configuration: Ii =Ib, Io=Ic,Vi=Vbe,Vo=Vce
Ie= Ib + Ic
Common-emitter configuration
Common base configuration
Since h
ris normally a relatively small quantity and resistance determined by 1/h
ois often large
enough, resulting
Hybrid versus r
e
model
The current source of the standard hybrid equivalent circuit is pointing down rather than in
the actual direction as shown in the re model
Complete hybrid equivalent circuit for a transistor
W
k
5
.
1
1 0 0Ib33
m
A
/
V
Effect of ro
Zo= ro
||
Rc
Io=
1
Rc
1
Rc
+
1
ro
βIb
=
ro
ro
+
Rc
βIb →
Io
Ib
=
R’=R1||R2=
R
1
+
R
2
¿
R
1.
R
2
¿
Ib =
1
βre
1
βre
+
1
R '
Ii →
Ib
Ii
=
R '
R
'+
βre
Zi=R’||
βre
Io =
βIb →
Io
Ib
=
β
Zo = Rc
Ai =
Io
Ii
=
Io
Ib
Ib
Ii
=
βR'
R
'+
βre
Av =
ℜ
¿
−Rc
¿
Effect of r
oZo = r
o||Rc
Av =
−
ro
∨
¿
Rc
ℜ
ro
+
Rc
¿
Io
Ib
=
ro. β
¿
Ai =
Io
Ii
=
Io
Ib
Ib
Io
=
ro
+
Rc
¿
R '
R
'+
βre
ro . β
¿
Or
Ai =
Rc
¿
Unbypassed
Vi = Ib
β
re +Ie RE = Ibβ
re + β¿ +1)Ib RE = (
β
r
e + β¿ +1) RE)IbZb =
Vi
Ib
=
β
r
e +( β +1)RE =¿
β
¿
r
e + RE) (for β >>1)Ib =
RB
+
Zb
¿
1
Zb
+
1
RB
¿
Ii →
Ib
Ii
=
RB
¿
1
Zb
¿
≅
β
RE (for RE >>r
e)Io =
βIb →
Io
Ib
=
β
Zi = RB || Zb Ai =
Io
Ii
=
Io
Ib
Ib
Ii
=
β . RB
RB
+
Zb
or
Zb =
β .r
eAv =
−
ℜ
Rc
Vo
=
Io Rc
=
(
Ic )Rc
=
αIe.Rc =
α
(
Vi
r e
)
Rc → Av
(since
α≅1¿Ie
≅Ii(
for R
E>>
r
e)
Io =
−
Ic
=−
α
Ie
¿
−
α
Ii
→ Ai
=−
α
≅
−
1
Effect of
r
o
For typical parameter values the effect of r
ocan be ignored
APPROXIMATE HYBRID EQUIVALENT CIRCUIT
common-emitter
common-base
h
ie = βr
eh
ie = βr
eh
oe =1/r
oh
fb = αh
ib =Zi =RB
||
hieZo=RC
VO = -IoRC = hfe Ib RC = - hfe
(
Vi
hie
)
RC AV = -h fe Rc
hie
Ib
≅
Ii ( for RB >> hie Io = hfe Ii hfeEffect of ro
Hoe =
1
ro
Zo =
1
hoe
|| Rcre =
hie
hfe
Av = -
hfe
(
1
hoe
∨
¿
Rc
)
hie
CE Emitter –Bias Configuration
Unbypassed
Common Base Configuration
Zi = R
E||h
ibZo = R
cIe =
hib
Vi
Vo =
h ib
¿
−Io . Rc=−
(
hfb. Ie)
Rc=¿−hfb(
Vihib
)
Rc → Av=−hfb. Rc
¿
Zi = R
B||
βr
eVi =
Zi
+
Zi
Rs
Vs →
Vs
Vi
=
Zi
Zi
+
Rs
Zo = R
cAv =
Vo
Vi
=
−
RL
∨
¿
Rc
r e
Avs =
Vo
Vs
=
¿
Vi
Vs
Vo
Vi
=
Zi
Zi
+
Rs
Av
Ii = Is
→ Ai=
Io
Ii
=−
Av
Zi
RL
Voltage Divider Bias
R’E = RE||RL
Vs –
Ib.Rs
– Ib βre
β
−
¿
+1)Ib R’E= 0
→ Ib=
Vs
Rs
+
βre
+
(
β
+
1
)
R ' E
≅
Vs
Rs
+
β
( ℜ+
R
'E
)
Ie
βI b=
Rs
β
+ ℜ+
R
'E
Vs
¿
¿
Vo =
R
'E
Rs
β
+ ℜ+
R
'E
v
s→
Av
s =R
'E
Rs
β
+ ℜ+
R
'E
Zb =
βre
+(
β
+
1
)
R
'E
≅
β
(
ℜ+
R
'E
)
Zo = R
E|| (
Rs
Philips Semiconductors Product specification
NPN general purpose transistors
BC
107;BC 108;BC;109
PINNING
FEATURES
Low current (max. 100mA) Low voltage ( max. 45 V)
APPLICATIONS
General purpose switching and amplificationPIN DESCRIPTION
1 emitter
2 base
DESCRIPTIONS
NPN transistor in a TO-18;SOT 18 metal package PNP complement : BC177
Characteristic
T = 25 C, unless other wise specified
symbol parameters conditions min type max unit
IcBc Collector cut-off current IE = 0; VCB
= 20 V
IE = 0; VCB
= 20 V; T = 125
C
-- -- 1515 nA
μA
IeBc Emitter cut-off current Ic = 0; VEB = 5 V - - 50 nA hFE DC current gain
BC 107A; BC108A
BC107B; BC108B; BC109B BC109C; BC109C
Ic =
10
μA
;VcE = 5 V-40 10 0 90 15 0 27 0
-hFE DC current gain BC 107A; BC108A
BC107B; BC108B;BC109B BC109C; BC109C
Ic = 2
mA
;VcE = 5 V11 0 20 0 42 0 18 0 29 0 52 0 22 0 45 0 80 0 VCEsat Collector emitter saturation
voltage Ic = 10 mA; IIc = 100 mA; IB = B =
0,5 mA
5 mA
-- 9020 0 25 0 60 0 mV mVVBEsat Base emitter saturation
voltage Ic = 10 mA; I
mA;note 1
B =0,5
Ic = 100 mA; IB =
5 mA;note
1
-- 700 90 0
-- mVmV
VBE Base emitter voltage Ic = 2 mA; VcE = 5 V; note 2 Ic = 10 mA; VcE = 5 V; note 2 55 0 -62 0 -70 0 77 0 mV mV