LT1469AIDF-2#PBF

LT1469-2
7
14692f
TYPICAL PERFORMANCE CHARACTERISTICS
Input Bias Current
vs Temperature
Input Bias Current
vs Input Common Mode Voltage
Input Common Mode Range
vs Supply Voltage
TEMPERATURE (°C)
–50
0
10
I
B
I
B
+
30
25 75
14692 G07
–10
–20
–25 0
50 100 125
–30
–40
20
INPUT BIAS CURRENT (nA)
V
S
= ±15V
INPUT COMMON MODE VOLTAGE (V)
–15
INPUT BIAS CURRENT (nA)
–20
0
20
0
10
14692 G08
–40
–60
–80
–10 –5 5
40
I
B
I
B
+
60
80
15
V
S
= ±15V
T
A
= 25°C
SUPPLY VOLTAGE (±V)
0
V
COMMON MODE RANGE (V)
1.0
2.0
–2.0
3
6
912
14692 G09
15
–1.0
0.5
1.5
–1.5
V
+
–0.5
18
T
A
= 25°C
ΔV
OS
< 100µV
Output Voltage Swing
vs Supply Voltage
Output Voltage Swing
vs Load Current
Output Short-Circuit Current
vs Temperature
SUPPLY VOLTAGE (±V)
0
1
V
OUTPUT VOLTAGE SWING (V)
4
3
2
–4
–3
–2
V
+
–1
5
14692 G10
10 15 20
R
L
= 2k
R
L
= 10k
R
L
= 10k
T
A
= 25°C
R
L
= 2k
OUTPUT CURRENT (mA)
–20
V
0.5
OUTPUT VOLTAGE SWING (V)
1.0
2.0
2.5
V
+
–0.5
–2.0
–10
0
5
14692 G11
1.5
–1.5
–1.0
–2.5
–15 –5
10
15
20
V
S
= ±15V
85°C
85°C
25°C
25°C
–40°C
–40°C
TEMPERATURE (°C)
–50
10
OUTPUT SHORT-CIRCUIT CURRENT (mA)
15
25
30
35
60
45
0
50
75
14692 G12
20
50
55
40
–25
25
100
125
V
S
= ±15V
V
IN
= ±0.2V
SOURCE
SINK
Open-Loop Gain
vs Resistive Load
Open-Loop Gain
vs Temperature
LOAD RESISTANCE (Ω)
10
110
OPEN-LOOP GAIN (dB)
130
135
140
100 1k 10k
14692 G13
125
120
115
T
A
= 25°C
V
S
= ±5V
V
S
= ±15V
TEMPERATURE (°C)
–50
130
140
160
25 75
14692 G14
120
110
–25 0
50 100 125
100
90
150
OPEN-LOOP GAIN (dB)
R
L
= 2k
V
S
= ±5V
V
S
= ±15V
Warm-Up Drift vs Time
TIME AFTER POWER UP (s)
0 20 40 60 80 100 120 140
OFFSET VOLTAGE DRIFT (µV)
10
0
–10
–20
–30
–40
–50
–60
–70
–80
14692 G15
S0-8 ±15V
S0-8 ±5V
LT1469-2
8
14692f
TYPICAL PERFORMANCE CHARACTERISTICS
Open-Loop Gain and Phase
vs Frequency
Gain vs Frequency, A
V
= –1
Undistorted Output Swing
vs Frequency, V
S
= ±15V
Small-Signal Transient, A
V
= –1
Large-Signal Transient, A
V
= –1
Output Impedance vs Frequency
Undistorted Output Swing
vs Frequency, V
S
= ±5V
FREQUENCY (Hz)
0
GAIN (dB)
PHASE (DEG)
10
20
30
40
50
60
10k 1M 10M 100M
14692 G16
–10
100k
70
–40
–20
0
20
40
60
80
–60
100
T
A
= 25°C
A
V
= –1
R
F
= R
G
= 5.1k
C
F
= 5pF
R
L
= 2k
PHASE
GAIN
FREQUENCY (Hz)
GAIN (dB)
14692 G17
6
0
1
2
3
4
5
–4
–3
–2
–1
–5
100k 10M 100M1M
C
L
= 100pF
C
L
= 47pF
C
L
= 22pF
NO C
L
T
A
= 25°C
A
V
= –1
R
F
= R
G
= 2k
C
F
= 6.8pF
R
L
= 500Ω
FREQUENCY (Hz)
0.01
OUTPUT IMPEDANCE (Ω)
0.1
1
10
10k 1M 10M 100M
14692 G18
0.001
100k
100
V
S
= ±15V
T
A
= 25°C
A
V
= 100
A
V
= 10
A
V
= –1
FREQUENCY (kHz)
OUTPUT VOLTAGE SWING (V
P-P
)
14692 G19
30
5
10
15
20
25
0
1 100 100010
V
S
= ±15V
T
A
= 25°C
R
L
= 2k
THD<1%
A
V
= –1
FREQUENCY (kHz)
OUTPUT VOLTAGE SWING (V
P-P
)
14692 G20
10
5
4
3
2
1
6
7
8
9
0
1 100 1000 200010
V
S
= ±5V
T
A
= 25°C
R
L
= 2k
THD<1%
A
V
= –1
50ns/DIV
14692 G23
V
S
= ±15V
20mV/DIV
200ns/DIV
14692 G24
V
S
= ±15V
A
V
= –1
R
F
= R
G
= 2k
C
L
= 22pF
2V/DIV
10V
0V
Settling Time vs Output Step,
A
V
= –1
SETTLING TIME (ns)
0
OUTPUT STEP (V)
10
8
4
0
–4
–8
6
2
–2
–6
–10
400 800200 600
14692 G21
1000300 700100 500 900
V
S
= ±15V
T
A
= 25°C
R
F
= R
G
= 2.5k
R
L
= 2.5k
INTO DIODES
C
F
= 8pF
0.1%
0.1%
0.1%
0.01%
150µV
0.01%
0.1%
150µV
Settling Time vs Output Step,
A
V
= 2
SETTLING TIME (ns)
0
OUTPUT STEP (V)
10
8
4
0
–4
–8
6
2
–2
–6
–10
400 800200 600
14692 G22
1000300 700100 500 900
V
S
= ±15V
T
A
= 25°C
R
F
= R
G
= 1k
R
L
= 2.5k INTO DIODES
C
F
= 22pF
R
S
= 511//30pF
0.01%
0.01%
LT1469-2
9
14692f
APPLICATIONS INFORMATION
Gain of 2 Stable
The LT1469-2 is a decompensated version of the LT1469.
The DC precision performance is identical, but the internal
compensation capacitors have been reduced to a point
where the op amp needs a gain of 2 or greater in order
to be stable.
In general, for applications where the gain around the op
amp is ≥ 2, the decompensated version should be used,
because it will give the best AC performance. In applica-
tions where the gain is <2, the unity-gain stable version
should be used.
The appropriate way to defi ne the ‘gain’ is as the inverse
of the feedback ratio from output to differential input,
including all relevant parasitics. Moreover, as with all
feedback loops, the stability of the loop depends on the
value of that feedback ratio at frequencies where the total
loop-gain would cross unity. Therefore, it is possible to
have circuits in which the gain at DC is lower than the gain
at high frequency, and these circuits can be stable even
with a non unity-gain stable op amp. An example is many
current-output DAC buffer applications.
Layout and Passive Components
The LT1469 requires attention to detail in board layout
in order to maximize DC and AC performance. For best
AC results (for example, fast settling time) use a ground
plane, short lead lengths and RF quality bypass capacitors
(0.01µF to 0.1µF) in parallel with low ESR bypass capaci-
tors (1µF to 10µF tantalum). For best DC performance, use
“star” grounding techniques, equalize input trace lengths
and minimize leakage (e.g., 1.5G of leakage between an
input and a 15V supply will generate 10nA—equal to the
maximum I
B
– specifi cation).
Board leakage can be minimized by encircling the input
circuitry with a guard ring operated at a potential close
to that of the inputs: for inverting confi gurations tie the
ring to ground, in noninverting connections tie the ring
to the inverting input (note the input capacitance will
increase which may require a compensating capacitor as
discussed below).
Microvolt level error voltages can also be generated in
the external circuitry. Thermocouple effects caused by
temperature gradients across dissimilar metals at the
contacts to the inputs can exceed the inherent drift of
the amplifi er. Air currents over device leads should be
minimized, package leads should be short and the two
input leads should be as close together as possible and
maintained at the same temperature.
The parallel combination of the feedback resistor and gain
setting resistor on the inverting input can combine with the
input capacitance to form a pole which can cause peak-
ing or even oscillations. A feedback capacitor of value C
F
= R
G
• C
IN
/R
F
may be used to cancel the input pole and
optimize dynamic performance. For applications where
the DC noise gain is one, and a large feedback resistor is
used, C
F
should be less than or equal to one half of C
IN
.
An example would be a DAC I-to-V converter as shown on
the front page of the data sheet where the DAC can have
many tens of picofarads of output capacitance.
Figure 1. Nulling Input Capacitance
Figure 2. Input Stage Protection
+
V
OUT
R
F
C
F
C
IN
1/2 LT1469-2
V
IN
14692 F01
R
G
Q1
+IN
14692 F02
R1
100Ω
Q2
–IN
R1
100Ω
V
V
+

LT1469AIDF-2#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
High Speed Operational Amplifiers 2x 200MHz, 30V/ s 16-B Acc AV = 2 Op
Lifecycle:
New from this manufacturer.
Delivery:
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