Differential Amplifier Offset Causes of dc voltage and current offset

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ESE319 Introduction to Microelectronics
Differential Amplifier Offset
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Causes of dc voltage and current offset
Modeling dc offset
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RC mismatch
IS mismatch
transistor mismatch
β mismatch
dc offsets in differential amplifiers due to component
mismatch can be modeled as differential phenomena
Kenneth R. Laker update KRL25Oct13
1
ESE319 Introduction to Microelectronics
IC1
VCC
IC2
VCC
VOdm
- V +
RC1
RC2
O
Q1
Q2
1. Let the ac sources be zero, i.e. the bases
of matched Q1 & Q2 are connected to
ground.
2. To further simplify, let there be no external
base RB and emitter resistors RE.
3. Let the mismatch be in RC where RC1 ≠ RC2.
II
VEE
Since Q1=Q2 and I is fixed,
currents are matched i.e.
I C1=I C2=
 I
I
=
2
1 2
Kenneth R. Laker update KRL25Oct13
V Odm=V C2−V C1= RC1 I C1−RC2 I C2
If V Odm=0⇒ RC1 I C1=R C2 I C2
I
I C1= I C2= ⇒ RC1= RC2
2
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ESE319 Introduction to Microelectronics
Let: RC1≠ RC2 s.t. RC2 RC1
Split the mismatch between both
collector resistors, and decompose into
common and differential components:
VOdm
I
2
I
2
I
RC2 RC1
(common)
RC =
2
 RC = RC2− RC1 (differential - mismatch)
Solving for RC1 & RC2:
VEE
v id /2
 RC
1  RC
RC2 =RC 
=RC 1

2
2 RC
v
Assume matched currents:
ic
I
−v id /2
 RC
1  RC
I C1= I C2=
RC1= RC −
= RC 1−

2
2
2 RC
Kenneth R. Laker update KRL25Oct13
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ESE319 Introduction to Microelectronics
Hence
:
 RC
 RC
V Odm= RC 
I C2− RC −
I C1
2
2
VOdm
I
2
I
2
I


Recall:
V Odm=RC2 I C2−R C1 I C1
I
I C1= I C2=
RC1≠ RC2
2
Kenneth R. Laker update KRL25Oct13


 RC
 RC
I
I
V Odm= RC 
 − RC −

2
2
2
2
or:
VEE
 
 
random variable (rv)
I
V Odm=  RC output offset voltage
2
Iff balanced, RC1 = RC2: V Odm=0V
4
VEE
ESE319 Introduction to Microelectronics
Collector-collector voltage due to
resistor mismatch:
VOdm
I
2
I
2
I
VEE
0V
-VOS
I
2
I
2
I
VEE
Kenneth R. Laker update KRL25Oct13
I
V Odm=  RC
2
Define the input offset voltage
as that input voltage that will cancel
VOdm. If the amplifier differential gain
is Avdm:
V Odm
VOS is highly variable,
V OS ≡
rv & can be + or Avdm
Input offset voltage is the output offset
voltage referred to the input due to
mismatch  RC .
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ESE319 Introduction to Microelectronics
I
  RC
2
V OS =
g m RC
0V
-VOS
I
2
I
2
IC
I 1
g m = =
VT
2 VT
I
Input referred offset due to ΔRC
V
mismatch:
random
 RC
variable
I
V OS  R =V T
V Odm =  RC
RC
2
where
EE
V Odm
V OS =
A vdm
C
Avdm=g m R C
Kenneth R. Laker update KRL25Oct13
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ESE319 Introduction to Microelectronics
Offset Voltage From Transistor Mismatch
Perfect balance requires:
V Odm =0⇒ RC1 I C1=RC2 I C2
RC
V+Odm -
RC
I
VEE
Kenneth R. Laker update KRL25Oct13
Previous case considered RC1 ≠ RC2
& Q1 = Q2 => IC1 = IC2.
Consider now Q1 ≠ Q2 => IC1 ≠ IC2.
ASSUME: 1. RC1 = RC2 = RC
2. VBE1 = VBE2
3. VT1=VT2
Only difference is in the saturation
currents of the transistors, i.e.
I S1≠ I S2
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ESE319 Introduction to Microelectronics
Again using common and differential
mode concepts:
+
-
V Odm
I S2 I S1
I S=
2
 I S = I S2− I S1
I
VEE
Kenneth R. Laker update KRL25Oct13
The two transistor saturation currents
are:
v ic
v id /2
IS
I S2= I S 
2
−v id /2
 IS
I S1= I S −
2
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ESE319 Introduction to Microelectronics
I C≈ I S e
ICdm/2
I C2
I C1≈ I S1 e
V BE
VT
I C2≈ I S2 e




IS
= I S−
e
2
V BE
VT
V BE
VT
V BE
 IS V
= I S
e
2
Kenneth R. Laker update KRL25Oct13
ICdm/2
I C1
V BE /V T
IS e
V BE /V T
IS V
e
2
− I S V
e
2
IS e
BE
BE
/V T
/VT
Vee
V BE /V T
T
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ESE319 Introduction to Microelectronics
IS e
ICdm/2
V BE /V T
IS V
e
2
I C2
ICdm/2
− I S V
e
2
IS e
I C1
I C1≈ I S1 e
V BE /V T
I C2≈ I S2 e
V BE /V T
BE
Large signal Model:

I C1≈ I S e
BE
V BE
VT
/VT
V BE /V T
Kenneth R. Laker update KRL25Oct13

 IS
I C1≈ I S −
e
2
/V T
Vee
also

V BE
VT
 IS
−
e
2

V BE
 IS V
I C2≈ I S 
e
2
V BE
VT
V BE
VT
T
V BE
VT
IS
I C2≈ I S e 
e
2
The parallel current sources are
illustrated in the schematic.
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ESE319 Introduction to Microelectronics
Note: differential IC components
cause current flow in opposite
directions through the RC's
resulting in an offset voltage. The
common IC components cause no
offset voltage.
I C≈ I S e
I C2≈ I S e
V BE
VT
V BE
VT
≈
 IS

e
2
 IS
I
I C2≈ 1

2
2IS
IS
I
I C1≈ 1−

2
2IS
I
2
V BE
VT
≈IS e
Kenneth R. Laker update KRL25Oct13
V BE
VT
IS
1

2IS
I IS
V Odm=R C I C2−RC I C1≈
RC
2 IS
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ESE319 Introduction to Microelectronics
I IS
V Odm≈
RC
2 IS
I VT IS
V Odm≈
RC
2 VT IS
IS
V Odm≈ g m V T
RC
IS
V OS   I
Recall:
IC I 1
g m= ≈
VT 2 VT
Kenneth R. Laker update KRL25Oct13
S
V Odm V Odm
IS
=
≈V T
=
Avdm g m RC
IS
V OS  I
S
IS
≈V T
IS
random
variable
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ESE319 Introduction to Microelectronics
Offset Voltage Summary
1. We considered two sources of offset voltage:
a. Unbalanced collector resistors
b. Unbalanced saturation currents
i. Due to mismatched transistor geometries
2. We ignored base or emitter circuit unbalance
3. Since the relationship between resistor and current unbalances are
random and assumed independent, we combine their effect as an
rms quantity:

2
2
V OS rms= V OS − R  V OS − I  =V T
Kenneth R. Laker update KRL25Oct13
C
S

 
2
 RC
 IS

RC
IS
2
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ESE319 Introduction to Microelectronics
Average & Offset Base (input) Bias Currents
Consider the case where the base currents
differ IB1 ≠ IB2.
Since IB1 & IB2 are related to bias current I,
I B2
I B1
I
I E2 =
2
I
I E1 =
2
VEE
Kenneth R. Laker update KRL25Oct13
their mismatch may be due to β1 ≠ β2.
Let's represent β1 & β2 in terms of differential
& common components:
v i−cm

1 =
2

2=−
2
v id /2
−v id /2
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ESE319 Introduction to Microelectronics
Using this notation, the two base currents are:
1
I 1
1
=
 2 


1

2
2
I 1 I
1
I 1
1
I B2≈
=
=
2 2 2
 2 

−
1−

2
2
I B1≈
I 1 I
=
2 1 2
nonlinear
f(Δβ)
For x << 1 we can expand the fraction as the series:
1
=1− x x 2 −x 3 ...≈1−x
1x
where

x≈ ±
2
Kenneth R. Laker update KRL25Oct13
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ESE319 Introduction to Microelectronics
Using the expansion and approximating 1≈:

I 1
1 
I B1≈
1−
2
2 


I 1
1 
I B2≈
1
2
2 
∣ ∣
I 
I OS  ≡∣I B1− I B2∣=
2 
¿

(input offset current)
I B1 I B2 I
Since the input bias current IB is defined as: I B =
=
2
2
The base or input offset current can also be written as:
I OS  = I B
Kenneth R. Laker update KRL25Oct13
∣ ∣


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ESE319 Introduction to Microelectronics
DC Offset Voltage & Current Summary
1. DC offset voltage and current occur due to mismatches in the BJT
differential amplifier external resistors and transistor parameters (Is
and β).
2. These mismatches are imperfections that are inherent to all differential amplifiers and their applications (e.g. op amps).
3. DC offset voltage and current are statistical quantities, i.e. no two
differential amplifiers will have the same offset voltage and current.
4. MOS differential amplifiers have zero input offset current.
Kenneth R. Laker update KRL25Oct13
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