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AD8571ARMZ-R2 数据表(PDF) 15 Page - Analog Devices

部件名 AD8571ARMZ-R2
功能描述  Zero-Drift, Single-Supply, Rail-to-Rail Input/Output Operational Amplifiers
PDF  24 Pages
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制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

AD8571ARMZ-R2 数据表(HTML) 15 Page - Analog Devices

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AD8571/AD8572/AD8574
Rev. C | Page 15 of 24
VIN+
VIN–
VOUT
AB
AA
ΦA1
ΦB
VOSA
+
VOSB
+
BB
CM2
CM1
ΦA2
VNB
VNA
–BA
VOA
ΦB
variation or long-term wear time, both of which are much
slower than the auto-zero clock frequency of the AD857x,
which effectively makes the VOS time invariant, and Equation 5
can be rewritten as
[]
[ ]
(
)
A
OSA
A
A
OSA
A
A
IN
A
OA
B
V
B
A
V
B
A
t
V
A
t
V
+
−
+
+
=
1
1
(6)
or
[]
[ ]
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛
+
+
=
A
OSA
IN
A
OA
B
V
t
V
A
t
V
1
(7)
Figure 50. Auto-Zero Phase of the Amplifier
AMPLIFICATION PHASE
Here, the auto-zeroing becomes apparent. Note that the VOS
term is reduced by a 1 + B
When the φB switches close and the φA switches open for the
amplification phase, the offset voltage remains on C
A
factor, which shows how the nulling
amplifier has greatly reduced its own offset voltage error even
before correcting the primary amplifier. Therefore, the primary
amplifier output voltage is the voltage at the output of the
AD857x amplifier. It is equal to
M1
and
essentially corrects any error from the nulling amplifier. The
voltage across CM1 is designated as VNA. The potential difference
between the two inputs to the primary amplifier is designated as
V , or V = (V
− V
IN
IN
IN+
IN–
). The output of the nulling amplifier
can then be expressed as
[ ]
[ ]
(
)
NB
B
OSB
IN
B
OUT
V
B
V
t
V
A
t
V
+
+
=
(8)
[]
[]
[ ]
[]
t
V
B
t
V
t
V
A
t
V
NA
A
OSA
IN
A
OA
−
−
=
(
(3)
= V , so this can be rewritten as
In the amplification phase, VOA
NB
[ ]
[]
[]
⎥
⎥
⎦
⎤
⎢
⎢
⎣
⎡
⎟⎟
⎠
⎞
⎜⎜
⎝
⎛
+
+
+
+
=
A
OSA
IN
A
B
OSB
B
IN
B
OUT
B
V
t
V
A
B
V
A
t
V
A
t
V
1
VIN+
VIN–
VOUT
AB
AA
ΦA
ΦB
VOSA
+
VOSB
+
BB
CM2
CM1
ΦA
VNB
VNA
–BA
VOA
ΦB
(9)
combining terms yields
[ ]
[]
()
OSB
B
A
OSA
B
A
B
A
B
IN
OUT
V
A
B
V
B
A
B
A
A
t
V
t
V
+
+
+
+
=
1
(10)
The AD857x architecture is optimized in such a way that
A
Figure 51. Output Phase of the Amplifier
= AB, B
Because φA is now open and there is no place for CM1 to
discharge, the voltage (VNA) at the present time (t) is equal to
the voltage at the output of the nulling amp (VOA) at the time
when φA was closed. If the period of the autocorrection
switching frequency is designated as TS, the amplifier switches
between phases every 0.5 × TS. Therefore, in the amplification
phase
[]
⎥⎦
⎤
⎢⎣
⎡ −
=
S
NA
NA
T
t
V
t
V
2
1
(4)
and substituting Equation 4 and Equation 2 into Equation 3 yields
[]
[]
[ ]
A
S
OSA
A
A
OSA
A
IN
A
OA
B
T
t
V
B
A
t
V
A
t
V
A
t
V
+
⎥⎦
⎤
⎢⎣
⎡ −
−
+
=
1
2
1
(5)
For the sake of simplification, it can be assumed that the
autocorrection frequency is much faster than any potential
change in VOSA or VOSB. This is a good assumption because
changes in offset voltage are a function of temperature
B
A
B
A
= BB
B
, and BA >> 1. In addition, the gain product to
A B
A
B
B
is much greater than AB
B
. Therefore, Equation 10 can be
simplified to
[ ]
[ ]
)
(
OSB
OSA
A
A
A
IN
OUT
V
V
A
B
A
t
V
t
V
+
+
=
(11)
Most obvious is the gain product of both the primary and
nulling amplifiers. This A B
A
B
A
term is what gives the AD857x its
extremely high open-loop gain. To understand how VOSA and
VOSB
B
relate to the overall effective input offset voltage of the
complete amplifier, set up the generic amplifier equation of
)
(
,
EFF
OS
IN
OUT
V
V
k
V
+
×
=
(12)
where:
k is the open-loop gain of an amplifier.
VOS, EFF is its effective offset voltage.
Putting Equation 12 into the form of Equation 11 gives
[ ]
[ ]
A
A
EFF
OS
A
A
IN
OUT
B
A
V
B
A
t
V
t
V
,
+
=
(13)



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