AD8029/AD8030/AD8040 Data Sheet
Rev. B | Page 16 of 24
THEORY OF OPERATION
03679-0-051
IN–
IN+
R
5
R
6
R
7
R
8
R
1
R
2
R
3
R
4
M
TOP
I
TAIL
M
BOT
OUTPUT
BUFFER
–V
S
R
TH
I
TH
+V
S
–1.2V
+V
S
V
OUT
Q
10
Q
11
C
MT
C
MB
–V
S
AD8029 ONLY
TO DISABLE
CIRCUITRY
DISABLE
Q
3
Q
4
Q
2
Q
1
Q
9
Q
8
Q
7
Q
6
Q
5
OUT IN
COM
SPD
Figure 50. Simplified Schematic
The AD8029 (single), AD8030 (dual), and AD8040 (quad) are
rail-to-rail input and output amplifiers fabricated using Analog
Devices’ XFCB process. The XFCB process enables the
AD8029/ AD8030/AD8040 to operate on 2.7 V to 12 V supplies
with a 120 MHz bandwidth and a 60 V/µs slew rate. A
simplified sche-matic of the AD8029/AD8030/AD8040 is
shown in Figure 50.
INPUT STAGE
For input common-mode voltages less than a set threshold
(1.2 V below V
CC
), the resistor degenerated PNP differential
pair (comprising Q
1
toQ
4
) carries the entire I
TAIL
current,
allowing the input voltage to go 200 mV below –V
S
. Conversely,
input common-mode voltages exceeding the same threshold
cause I
TAIL
to be routed away from the PNP differential pair and
into the NPN differential pair through transistor Q
9
. Under this
condition, the input common-mode voltage is allowed to rise
200 mV above +V
S
while still maintaining linear amplifier
behavior. The transition between these two modes of operation
leads to a sudden, temporary shift in input stage transconduc-
tance, g
m
, and dc parameters (such as the input offset voltage
V
OS
), which in turn adversely affect the distortion performance.
The SPD block shortens the duration of this transition, thus
improving the distortion performance. As shown in Figure 50,
the input differential pair is protected by a pair of two series
diodes, connected in anti-parallel, which clamp the differential
input voltage to approximately ±1.5 V.
OUTPUT STAGE
The currents derived from the PNP and NPN input differential
pairs are injected into the current mirrors M
BOT
and M
TOP
, thus
establishing a common-mode signal voltage at the input of the
output buffer.
The output buffer performs three functions:
1. It buffers and applies the desired signal voltage to the
output devices, Q
10
and Q
11
.
2. It senses the common-mode current level in the output
devices.
3. It regulates the output common-mode current by
establishing a common-mode feedback loop.
The output devices Q
10
and Q
11
work in a common-emitter
configuration, and are Miller-compensated by internal
capacitors, C
MT
and C
MB
.
The output voltage compliance is set by the output devices’
collector resistance R
C
(about 25 Ω), and by the required load
current I
L
. For instance, a light equivalent load (5 kΩ) allows the
output voltage to swing to within 40 mV of either rail, while
heavier loads cause this figure to deteriorate as R
C
× I
L
.
Data Sheet AD8029/AD8030/AD8040
Rev. B | Page 17 of 24
APPLICATIONS
WIDEBAND OPERATION
+V
S
–V
S
C2
10µF
C1
0.1µF
C4
0.1µF
C3
10µF
V
OUT
+
AD8029
R
G
R1
R
F
DISABLE
V
IN
R1 = R
F
||R
G
03679-0-052
Figure 51. Wideband Non-inverting Gain Configuration
+V
S
–V
S
C1
0.1µF
C4
0.1µF
C3
10µF
R1
V
OUT
+
AD8029
R
G
R1 = R
F
||R
G
R
F
V
IN
03679-0-053
C2
10µF
DISABLE
Figure 52. Wideband Inverting Gain Configuration
OUTPUT LOADING SENSITIVITY
To achieve maximum performance and low power dissipation,
the designer needs to consider the loading at the output of
AD8029/AD8030/AD8040. Table 5 shows the effects of output
loading and performance.
When operating at unity gain, the effective load at the amplifier
output is the resistance (R
L
) being driven by the amplifier. For
gains other than 1, in noninverting configurations, the feedback
network represents an additional current load at the amplifier
output. The feedback network (R
F
+ R
G
) is in parallel with R
L
,
which lowers the effective resistance at the output of the
amplifier. The lower effective resistance causes the amplifier to
supply more current at the output. Lower values of feedback
resistance increase the current draw, thus increasing the
amplifier’s power dissipation.
For example, if using the values shown in Table 5 for a gain of 2,
with resistor values of 2.5 kΩ, the effective load at the output is
1.67 kΩ. For inverting configurations, only the feedback resistor
R
F
is in parallel with the output load. If the load is greater than
that specified in the data sheet, the amplifier can introduce
nonlinearities in its open-loop response, which increases
distortion. Figure 53 and Figure 54 illustrate effective output
loading and distortion performance. Increasing the resistance of
the feedback network can reduce the current consumption, but
has other implications.
FREQUENCY (MHz)
HARMONIC DISTORTION (dBc)
0.01
–120
0.1 1.0 10
03679-A-008
–40
–50
–60
–70
–80
–90
–100
–110
V
S
= 5V
V
OUT
= 0.1V p-p
R
L
= 5k
R
L
= 2.5k
V
S
= 5V
V
OUT
= 2.0V p-p
SECOND HARMONIC – SOLID LINES
THIRD HARMONIC – DOTTED LINES
R
L
= 1k
Figure 53. Gain of 1 Distortion
FREQUENCY (MHz)
HARMONIC DISTORTION (dBc)
0.01
–120
0.1 1.0 10
03679-A-009
–40
–50
–60
–70
–80
–90
–100
–110
V
S
= 5V
V
OUT
= 0.1V p-p
R
F
= R
L
= 1k
V
S
= 5V
V
OUT
= 2.0V p-p
SECOND HARMONIC – SOLID LINES
THIRD HARMONIC – DOTTED LINES
R
F
= R
L
= 5k
R
F
= R
L
= 2.5k
Figure 54. Gain of 2 Distortion
AD8029/AD8030/AD8040 Data Sheet
Rev. B | Page 18 of 24
Table 5. Effect of Load on Performance
Noninverting
Gain
R
F
(kΩ)
R
G
(kΩ)
R
LOAD
(kΩ)
3 dB SS BW
(MHz)
Peaking
(dB)
HD2 at 1 MHz,
2 V p-p (dB)
HD3 at 1 MHz,
2 V p-p (dB)
Output Noise
(nV/√Hz)
1 0 N/A 1 120 0.02 –80 –72 16.5
1 0 N/A 2 130 0.6 –84 –83 16.5
1
0
N/A
5
139
1
–87.5
–92.5
16.5
2 1 1 1 36 0 –72 –60 33.5
2 2.5 2.5 2.5 44.5 0.2 –79 –72.5 34.4
2 5 5 5 43 2 –84 –86 36
–1 1 1 1 40 0.01 –68 –57 33.6
–1 2.5 2.5 2.5 40 0.05 –74 –68 34
–1 5 5 5 34 1 –78 –80 36
The feedback resistance (R
F
|| R
G
) combines with the input
capacitance to form a pole in the amplifier’s loop response. This
can cause peaking and ringing in the amplifier’s response if the
RC time constant is too low. Figure 55 illustrates this effect.
Peaking can be reduced by adding a small capacitor (1 pF–4 pF)
across the feedback resistor. The best way to find the optimal
value of capacitor is to empirically try it in your circuit. Another
factor of higher resistance values is the impact it has on noise
performance. Higher resistor values generate more noise. Each
application is unique and therefore a balance must be reached
between distortion, peaking, and noise performance. Table 5
outlines the trade-offs that different loads have on distortion,
peaking, and noise performance. In gains of 1, 2, and 10,
equivalent loads of 1 k, 2 kΩ, and 5 kare shown.
With increasing load resistance, the distortion and 3 dB
bandwidth improve, while the noise and peaking degrade
slightly.
R
L
= 5k
FREQUENCY (MHz)
NORMALIZED CLOSED-LOOP GAIN (dB)
1
–8
10 100 1000
03679-A-007
2
1
0
–1
–2
–3
–4
–5
–6
R
L
= 2.5k
–7
R
F
= R
L
= 5k
R
F
= R
L
= 2.5k
R
F
= R
L
= 1k
G = +2
G = +1
R
L
= 1k
V
S
= 5V
V
OUT
= 0.1V p-p
Figure 55. Frequency Response for Various Feedback/Load Resistances
DISABLE PIN
The AD8029 disable pin allows the amplifier to be shut down
for power conservation or multiplexing applications. When in
the disable mode, the amplifier draws only 150 µA of quiescent
current. The disable pin control voltage is referenced to the
negative supply. The amplifier enters power-down mode any
time the disable pin is tied to the most negative supply or within
0.8 V of the negative supply. If left open, the amplifier will
operate normally. For switching levels, refer to Table 6.
Table 6. Disable Pin Control Voltage
Disable Pin
Voltage
Supply Voltage
+3 V +5 V
±
5 V
Low
(Disabled)
0 V to <0.8 V 0 V to <0.8 V 5 V to <4 .2 V
High
(Enabled)
1.2 V to 3 V 1.2 V to 5 V 3.8 V to +5 V

AD8030ARJZ-REEL7

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
High Speed Operational Amplifiers Lo Pwr Hi Spd RRIO
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