AD8615/AD8616/AD8618 Data Sheet
Rev. G | Page 10 of 20
0
2
4
6
8
10
12
14
16
18
OUTPUT S
A
TUR
A
TION VOLTAGE (mV)
–40 –25 –10 5 20 35 50 65 80 95 110 125
TEMPERATURE (°C)
V
S
= 2.7V
V
OH
@ 1mA LOAD
V
OL
@ 1mA LOAD
0
4648-030
Figure 30. Output Saturation Voltage vs. Temperature
1M 10M
100
80
60
40
20
0
–20
–40
–60
–80
–100
GAIN (dB)
225
180
135
90
45
0
–45
–90
–135
–180
–225
PHASE (Degrees)
V
S
= ±1.35V
T
A
= 25°C
Ø
m
= 42°
60M
FREQUENCY (Hz)
04648-031
Figure 31. Open-Loop Gain and Phase vs. Frequency
0
0.3
0.6
0.9
1.2
1.5
1.8
2.1
2.4
2.7
OUTPUT SWIN
G
(
V
p-p)
FREQUENCY (Hz)
10k1k 100k 1M 10M
V
S
= 2.7V
V
IN
= 2.6V p-p
T
A
= 25°C
R
L
= 2k
A
V
= 1
04648-032
Figure 32. Closed-Loop Output Voltage Swing vs. Frequency
5
0
10
15
20
25
30
35
40
45
50
SM
A
LL SIGN
A
L OVERSHOOT (%)
CAPACITANCE (pF)
10 100 1000
V
S
= ±1.35V
R
L
=
T
A
= 25°C
A
V
= 1
+OS
–O
S
04648-033
Figure 33. Small Signal Overshoot vs. Load Capacitance
VOLTAGE (50mV/DIV)
TIME (1µs/DIV)
V
S
= 2.7V
R
L
= 10k
C
L
= 200pF
A
V
= 1
0
4648-034
Figure 34. Small Signal Transient Response
VOLTAGE (500mV/DIV)
TIME (1µs/DIV)
V
S
= 2.7V
R
L
= 10k
C
L
= 200pF
A
V
= 1
04648-035
Figure 35. Large Signal Transient Response
Data Sheet AD8615/AD8616/AD8618
Rev. G | Page 11 of 20
APPLICATIONS INFORMATION
INPUT OVERVOLTAGE PROTECTION
If the voltage applied at either input exceeds the supplies, place
external resistors in series with the inputs. The resistor values
can be determined by the equation
mA5
V
SY
S
IN
R
V
The extremely low input bias current allows the use of larger
resistors, which allows the user to apply higher voltages at the
inputs. The use of these resistors adds thermal noise, which
contributes to the overall output voltage noise of the amplifier.
For example, a 10 kΩ resistor has less than 13 nV/√Hz of
thermal noise and less than 10 nV of error voltage at room
temperature.
OUTPUT PHASE REVERSAL
The AD8615/AD8616/AD8618 are immune to phase inversion,
a phenomenon that occurs when the voltage applied at the input of
the amplifier exceeds the maximum input common mode.
Phase reversal can cause permanent damage to the amplifier
and can create lock ups in systems with feedback loops.
VOL
T
AGE (2V/DIV)
TIME (2ms/DIV)
V
IN
V
OUT
V
S
= ±2.5V
V
IN
= 6V p-p
A
V
= 1
R
L
= 10k
04648-036
Figure 36. No Phase Reversal
DRIVING CAPACITIVE LOADS
Although the AD8615/AD8616/AD8618 are capable of driving
capacitive loads of up to 500 pF without oscillating, a large amount
of overshoot is present when operating at frequencies above
100 kHz. This is especially true when the amplifier is configured
in positive unity gain (worst case). When such large capacitive
loads are required, the use of external compensation is highly
recommended.
This reduces the overshoot and minimizes ringing, which in
turn improves the frequency response of the AD8615/AD8616/
AD8618. One simple technique for compensation is the snubber,
which consists of a simple RC network. With this circuit in place,
output swing is maintained and the amplifier is stable at all gains.
Figure 38 shows the implementation of the snubber, which
reduces overshoot by more than 30% and eliminates ringing
that can cause instability. Using the snubber does not recover
the loss of bandwidth incurred from a heavy capacitive load.
VOLT
A
GE
(
100mV/DIV)
TIME (2µs/DIV)
V
S
= ±2.5V
A
V
= 1
C
L
= 500pF
0
4648-037
Figure 37. Driving Heavy Capacitive Loads Without Compensation
V+
200
500pF
500pF
V–
V
EE
V
CC
200mV
+
04648-038
Figure 38. Snubber Network
VOLT
A
GE
(
100mV/DIV)
TIME (10µs/DIV)
V
S
2.5V
A
V
= 1
R
S
= 200
C
S
= 500pF
C
L
= 500pF
04648-039
Figure 39. Driving Heavy Capacitive Loads Using the Snubber Network
AD8615/AD8616/AD8618 Data Sheet
Rev. G | Page 12 of 20
OVERLOAD RECOVERY TIME
Overload recovery time is the time it takes the output of the
amplifier to come out of saturation and recover to its linear region.
Overload recovery is particularly important in applications where
small signals must be amplified in the presence of large transients.
Figure 40 and Figure 41 show the positive and negative overload
recovery times of the AD8616. In both cases, the time elapsed
before the AD8616 comes out of saturation is less than 1 μs. In
addition, the symmetry between the positive and negative recovery
times allows excellent signal rectification without distortion to the
output signal.
TIME (1µs/DIV)
V
S
= ±2.5V
R
L
= 10k
A
V
= 100
V
IN
= 50mV
–50mV
+2.5V
0
V
0
V
0
4648-040
Figure 40. Positive Overload Recovery
TIME (1µs/DIV)
V
S
2.5V
R
L
= 10k
A
V
= 100
V
IN
= 50mV
+50mV
2.5V
0V
0V
04648-041
Figure 41. Negative Overload Recovery
D/A CONVERSION
The AD8616 can be used at the output of high resolution DACs.
The low offset voltage, fast slew rate, and fast settling time make
the part suitable to buffer voltage output or current output
DACs.
Figure 42 shows an example of the AD8616 at the output of the
AD5542. The AD8616s rail-to-rail output and low distortion
help maintain the accuracy needed in data acquisition systems
and automated test equipment.
AD5542
V
OUT
UNIPOLAR
OUTPUT
AGNDDGND
REFS
1/2
AD8616
REFFV
DD
SERIAL
INTERFACE
0.1
µF
0.1µF
10µF
5
V
2.5
V
+
CS
DIN
SCLK
LDAC
0
4648-042
Figure 42. Buffering DAC Output
LOW NOISE APPLICATIONS
Although the AD8618 typically has less than 8 nV/√Hz of voltage
noise density at 1 kHz, it is possible to reduce it further. A simple
method is to connect the amplifiers in parallel, as shown in
Figure 43. The total noise at the output is divided by the square
root of the number of amplifiers. In this case, the total noise is
approximately 4 nV/√Hz at room temperature. The 100 Ω
resistor limits the current and provides an effective output
resistance of 50 Ω.
V–
R3
100
R1
10
V+
V
IN
3
2
1
R2
1k
V–
R6
100
R4
10
V+
3
2
1
R5
1k
V–
R9
100
R7
10
V+
3
2
1
R8
1k
V–
R12
100
R10
10
V+
3
2
1
R11
1k
V
OUT
04648-043
Figure 43. Noise Reduction

AD8618ARZ-REEL

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Precision Amplifiers Prec 20MHz CMOS Quad RR
Lifecycle:
New from this manufacturer.
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