LT1223
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1223fb
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TYPICAL PERFOR A CE CHARACTERISTICS
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does in a voltage feedback op amp, the closed-loop
bandwidth does not change. This is because the equiva-
lent gain bandwidth product of the current feedback am-
plifier is set by the Thevenin equivalent resistance at the
inverting input and the internal compensation capacitor.
By keeping R
F
constant and changing the gain with R
G
, the
Thevenin resistance changes by the same amount as the
change in gain. As a result, the net closed-loop bandwidth
of the LT1223 remains the same for various closed-loop
gains.
Voltage Gain and Phase vs Total Harmonic Distortion vs 2nd and 3rd Harmonic
Frequency Frequency Distortion vs Frequency
Noninverting Amplifier Settling Noninverting Amplifier Settling Inverting Amplifier Settling
Time to 10mV vs Output Step Time to 1mV vs Output Step Time vs Output Step
Current Feedback Basics
The small-signal bandwidth of the LT1223, like all current
feedback amplifiers, isn’t a straight inverse function of the
closed-loop gain. This is because the feedback resistors
determine the amount of current driving the amplifier’s
internal compensation capacitor. In fact, the amplifier’s
feedback resistor (R
F
) from output to inverting input
works with internal junction capacitances of the LT1223 to
set the closed-loop bandwidth.
Even though the gain set resistor (R
G
) from inverting input
to ground works with R
F
to set the voltage gain just like it
FREQUENCY (Hz)
1M
–30
VOLTAGE GAIN (dB)
–15
5
20
10M 100M 1G
LT1223 • TPC20
R 1k
L
GAIN
–25
–20
–10
–5
0
10
15
PHASE SHIFT (DEGREES)
–225
–90
90
225
–180
–135
–45
0
45
135
180
PHASE
R = 100
L
R 1k
L
R = 100
L
V = 15V
R
F
= R
G
= 1k
S
±
FREQUENCY (Hz)
TOTAL HARMONIC DISTORTION (%)
0.01
0.1
10 1k 10k 100k
LT1223 • TPC21
0.001
100
THD
V = 15V
V = 7V
R = 400
R
F
= R
G
=1k
S
O
L
±
RMS
FREQUENCY (MHz)
1
–70
DISTORTION (dBc)
–20
10 100
LT1223 • TPC22
–60
–50
–40
–30
2ND
3RD
V = 15V
V = 2V
P-P
R = 100
R
F
= 1k
A = 10dB
S
±
O
L
V
SETTLING TIME (ns)
0
–10
OUTPUT STEP (V)
–4
10
LT1223 • TPC23
20 40 60 80 100
–8
–6
–2
0
2
4
6
8
TO 10mV
TO 10mV
V
S
L
±
A = +1
R
F
= 1k
V = 15V
R = 1k
SETTLING TIME ( s)
0
–10
OUTPUT STEP (V)
–4
10
LT1223 • TPC24
12
–8
–6
–2
0
2
4
6
8
TO 1mV
µ
TO 1mV
A = +1
R = 1k
V = 15V
R = 1k
F
S
±
V
L
SETTLING TIME (ns)
0
–10
OUTPUT STEP (V)
–4
10
LT1223 • TPC25
100
–8
–6
–2
0
2
4
6
8
TO 1mV
TO 10mV
A = –1
R = 1k
V = 15V
R = 1k
F
S
±
V
20 40 60 80
L
TO 10mV
TO 1mV
LT1223
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The curve on the first page shows the LT1223 voltage gain
versus frequency while driving 100, for five gain settings
from 1 to 100. The feedback resistor is a constant 1k and
the gain resistor is varied from infinity to 10. Shown for
comparison is a plot of the fixed 100MHz gain bandwidth
limitation that a voltage feedback amplifier would have. It
is obvious that for gains greater than one, the LT1223
provides 3 to 20 times more bandwidth. It is also evident
that second order effects reduce the bandwidth somewhat
at the higher gain settings.
Feedback Resistor Selection
Because the feedback resistor determines the compensa-
tion of the LT1223, bandwidth and transient response can
be optimized for almost every application. To increase the
bandwidth when using higher gains, the feedback resistor
(and gain resistor) can be reduced from the nominal 1k
value. The Minimum Feedback Resistor versus Voltage
Gain curve shows the values to use for ±15V supplies.
Larger feedback resistors can also be used to slow down
the LT1223 as shown in the –3dB Bandwidth versus
Feedback Resistor curve.
Capacitive Loads
The LT1223 can be isolated from capacitive loads with a
small resistor (10 to 20) or it can drive the capacitive
load directly if the feedback resistor is increased. Both
techniques lower the amplifier’s bandwidth about the
same amount. The advantage of resistive isolation is that
the bandwidth is only reduced when the capacitive load is
present. The disadvantage of resistor isolation is that
resistive loading causes gain errors. Because the DC
accuracy is not degraded with resistive loading, the de-
sired way of driving capacitive loads, such as flash con-
verters, is to increase the feedback resistor. The Maximum
Capacitive Load versus Feedback Resistor curve shows
the value of feedback resistor and capacitive load that
gives 5dB of peaking. For less peaking, use a larger
feedback resistor.
Power Supplies
The LT1223 may be operated with single or split supplies
as low as ±4V (8V total) to as high as ±18V (36V total). It
is not necessary to use equal value split supplies, how-
ever, the offset voltage will degrade about 350µV per volt
of mismatch. The internal compensation capacitor de-
creases with increasing supply voltage. The –3dB Band-
width versus Supply Voltage curve shows how this affects
the bandwidth for various feedback resistors. Generally,
the bandwidth at ±5V supplies is about half the value it is
at ±15V supplies for a given feedback resistor.
The LT1223 is very stable even with minimal supply
bypassing, however, the transient response will suffer if
the supply rings. It is recommended for good slew rate and
settling time that 4.7µF tantalum capacitors be placed
within 0.5 inches of the supply pins.
Input Range
The noninverting input of the LT1223 looks like a 10M
resistor in parallel with a 3pF capacitor until the common
mode range is exceeded. The input impedance drops
somewhat and the input current rises to about 10µA when
the input comes too close to the supplies. Eventually,
when the input exceeds the supply by one diode drop, the
base collector junction of the input transistor forward
biases and the input current rises dramatically. The input
current should be limited to 10mA when exceeding the
supplies. The amplifier will recover quickly when the input
is returned to its normal common mode range unless the
input was over 500mV beyond the supplies, then it will
take an extra 100ns.
Offset Adjust
Output offset voltage is equal to the input offset voltage
times the gain plus the inverting input bias current times
the feedback resistor. For low gain applications (3 or less)
a 10k pot connected to Pins 1 and 5 with wiper to V
+
will
trim the inverting input current (±10µA) to null the output;
it does not change the offset voltage very much. If the
LT1223 is used in a high gain application, where input
offset voltage is the dominate error, it can be nulled by
pulling approximately 100µA from Pin 1 or 5. The easy
way to do this is to use a 10k pot between Pin 1 and 5 with
a 150k resistor from the wiper to ground for 15V supply
applications. Use a 47k resistor when operating on a 5V
supply.
LT1223
9
1223fb
Shutdown
Pin 8 activates a shutdown control function. Pulling more
than 200mA from Pin 8 drops the supply current to less
than 3mA, and puts the output into a high impedance state.
The easy way to force shutdown is to ground Pin 8, using
an open collector (drain) logic stage. An internal resistor
limits current, allowing direct interfacing with no addi-
tional parts. When Pin 8 is open, the LT1223 operates
normally.
Slew Rate
The slew rate of a current feedback amplifier is not inde-
pendent of the amplifier gain configuration the way it is in
a traditional op amp. This is because the input stage and
the output stage both have slew rate limitations. Inverting
amplifiers do not slew the input and are therefore limited
only by the output stage. High gain, noninverting amplifi-
ers are similar. The input stage slew rate of the LT1223 is
about 350V/µs before it becomes nonlinear and is en-
hanced by the normally reverse-biased emitters on the
input transistors. The output slew rate depends on the size
of the feedback resistors. The peak output slew rate is
about 2000V/µs with a 1k feedback resistor and drops
proportionally for larger values. At an output slew rate of
1000V/µs or more, the transistors in the “mirror circuits”
will begin to saturate due to the large feedback currents.
This causes the output to have slew induced overshoot and
is somewhat unusual looking; it is in no way harmful or
dangerous to the device. The photos show the LT1223 in
a noninverting gain of three (R
F
= 1k, R
G
= 500) with a
20V peak-to-peak output slewing at 500V/µs, 1000V/µs
and 2000V/µs.
Settling Time
The Inverting Amplifier Settling Time versus Output Step
curve shows that the LT1223 will settle to within 1mV of
final value in less than 100ns for all output changes of 10V
or less. When operated as an inverting amplifier there is
less than 500µV of thermal settling in the amplifier.
However, when operating the LT1223 as a noninverting
amplifier, there is an additional thermal settling compo-
nent that is about 200µV for every volt of input common
mode change. So a noninverting gain of one amplifier will
Output Slew Rate at 2000V/µs Shows Aberrations (See Text)
Output Slew Rate of 1000V/µs
Output Slew Rate of 500V/µs
1223 A01
1223 A02
1223 A03
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LT1223CS8#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
High Speed Operational Amplifiers 100MHz C F Amp
Lifecycle:
New from this manufacturer.
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