LT1812
10
1812fb
TYPICAL PERFORMANCE CHARACTERISTICS
Small-Signal Transient,
A
V
= –1
Small-Signal Transient,
A
V
= 1
Small-Signal Transient,
A
V
= 1, C
L
= 1000pF
Large-Signal Transient,
A
V
= –1
Large-Signal Transient,
A
V
= 1
Large-Signal Transient,
A
V
= 1, C
L
= 1000pF
2nd and 3rd Harmonic Distortion
vs Frequency
Differential Gain and Phase
vs Supply Voltage Capacitive Load Handling
FREQUENCY (Hz)
–100
–70
–80
–90
–30
–40
–50
–60
1812 G28
HARMONIC DISTORTION (dB)
100k
10M
1M
T
A
= 25°C
A
V
= 2
V
S
= ±5V
V
O
= 2V
P-P
2ND HARMONIC
3RD HARMONIC
R
L
= 100Ω
2ND HARMONIC
R
L
= 500Ω
3RD HARMONIC
TOTAL SUPPLY VOLTAGE (V)
4
DIFFERENTIAL PHASE (DEG)
DIFFERENTIAL GAIN (%)
0
0.25
T
A
= 25°C
0.10
8
10
1812 G29
0.15
0.20
0.05
0
0.25
0.10
0.15
0.20
0.05
6
12
DIFFERENTIAL GAIN
R
L
= 150Ω
DIFFERENTIAL PHASE
R
L
= 150Ω
DIFFERENTIAL PHASE
R
L
= 1k
DIFFERENTIAL GAIN
R
L
= 1k
CAPACITIVE LOAD (pF)
10
40
OVERSHOOT (%)
50
60
70
80
100 1000 10000
1812 G30
30
20
10
0
90
100
T
A
= 25°C
V
S
= ±5V
A
V
= 1
A
V
= –1
LT1812
11
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Layout and Passive Components
The LT1812 amplifi er is more tolerant of less than ideal
layouts than other high speed amplifi ers. For maximum
performance (for example, fast settling) use a ground
plane, short lead lengths and RF-quality bypass capacitors
(0.01μF to 0.1μF). For high drive current applications, use
low ESR bypass capacitors (1μF to 10μF tantalum).
The parallel combination of the feedback resistor and gain
setting resistor on the inverting input combine with the
input capacitance to form a pole that can cause peaking
or even oscillations. If feedback resistors greater than 2k
are used, a parallel capacitor of value
C
F
> R
G
• C
IN
/R
F
should be used to cancel the input pole and optimize
dynamic performance. For applications where the DC
noise gain is 1 and a large feedback resistor is used, C
F
should be greater than or equal to C
IN
. An example would
be an I-to-V converter.
Input Considerations
Each of the LT1812 amplifi er inputs is the base of an NPN
and PNP transistor whose base currents are of opposite
polarity and provide fi rst-order bias current cancellation.
Because of variation in the matching of NPN and PNP
beta, the polarity of the input bias current can be positive
or negative. The offset current does not depend on beta
matching and is well controlled. The use of balanced source
resistance at each input is recommended for applications
where DC accuracy must be maximized. The inputs can
withstand differential input voltages of up to 3V without
damage and need no clamping or source resistance for
protection.
The device should not be used as a comparator because
with sustained differential inputs, excessive power dissi-
pation may result.
Capacitive Loading
The LT1812 is stable with a 1000pF capacitive load,
which is outstanding for a 100MHz amplifi er. This is
accomplished by sensing the load induced output pole
and adding compensation at the amplifi er gain node. As
APPLICATIONS INFORMATION
the capacitive load increases, both the bandwidth and
phase margin decrease so there will be peaking in the
frequency domain and in the transient response. Coaxial
cable can be driven directly, but for best pulse fi delity, a
resistor of value equal to the characteristic impedance of
the cable (i.e., 75Ω) should be placed in series with the
output. The other end of the cable should be terminated
with the same value resistor to ground.
Slew Rate
The slew rate is proportional to the differential input
voltage. Highest slew rates are therefore seen in the lowest
gain confi gurations. For example, a 5V output step in a
gain of 10 has a 0.5V input step, whereas in unity gain
there is a 5V input step. The LT1812 is tested for slew
rate in a gain of –1. Lower slew rates occur in higher
gain confi gurations.
Shutdown
The LT1812 has a shutdown pin (SHDN, Pin 8) for
conserving power. When this pin is open or biased at
least 2V above the negative supply, the part operates
normally. When pulled down to V
, the supply current
drops to about 50μA. Typically, the turn-off delay is
1μs and the turn-on delay 0.5μs. The current out of the
SHDN pin is also typically 50μA. In shutdown mode, the
amplifi er output is not isolated from the inputs, so the
LT1812 shutdown feature cannot be used for multiplexing
applications. The 50μA typical shutdown current is
exclusive of any output (load) current. In order to prevent
load current (and maximize the power savings), either
the load needs to be disconnected, or the input signal
needs to be 0V. Even in shutdown mode, the LT1812 can
still drive signifi cant current into a load. For example, in
an A
V
= 1 confi guration, when driven with a 1V DC input,
the LT1812 drives 2mA into a 100Ω load. It takes about
500μs for the load current to reach this value.
Power Dissipation
The LT1812 combines high speed and large output drive
in a small package. It is possible to exceed the maximum
junction temperature under certain conditions. Maximum
LT1812
12
1812fb
SIMPLIFIED SCHEMATIC
1812 SS
OUT
+IN
–IN
BIAS
CONTROL
R
B
V
+
V
SHDN
R1
300Ω
C
C
R
C
C
APPLICATIONS INFORMATION
junction temperature (T
J
) is calculated from the ambient
temperature (T
A
) and power dissipation (P
D
) as follows:
T
J
= T
A
+ (P
D
θ
JA
) (Note 9)
Power dissipation is composed of two parts. The fi rst is due
to the quiescent supply current and the second is due to
on-chip dissipation caused by the load current. The worst-
case load induced power occurs when the output voltage
is at 1/2 of either supply voltage (or the maximum swing
if less than 1/2 supply voltage). Therefore P
DMAX
is:
P
DMAX
= (V
+
– V
)(I
SMAX
) + (V
+
/2)
2
/R
L
or
P
DMAX
= (V
+
– V
)(I
SMAX
) + (V
+
– V
OMAX
)(V
OMAX
/R
L
)
Example: LT1812CS5 at 70°C, V
S
= ±5V, R
L
= 100Ω
P
DMAX
= (10V)(4.5mA) + (2.5V)
2
/10 0Ω = 108mW
T
JMAX
= 70°C + (108mW)(250°C/W) = 97°C
Circuit Operation
The LT1812 circuit topology is a true voltage feedback
amplifi er that has the slewing behavior of a current feedback
amplifi er. The operation of the circuit can be understood
by referring to the Simplifi ed Schematic. The inputs are
buffered by complementary NPN and PNP emitter followers
that drive a 300Ω resistor. The input voltage appears across
the resistor generating currents that are mirrored into the
high impedance node. Complementary followers form an
output stage that buffers the gain node from the load. The
bandwidth is set by the input resistor and the capacitance
on the high impedance node. The slew rate is determined by
the current available to charge the gain node capacitance.
This current is the differential input voltage divided by R1,
so the slew rate is proportional to the input. Highest slew
rates are therefore seen in the lowest gain confi gurations.
The RC network across the output stage is bootstrapped
when the amplifi er is driving a light or moderate load
and has no effect under normal operation. When driving
capacitive loads (or a low value resistive load) the network
is incompletely bootstrapped and adds to the compensation
at the high impedance node. The added capacitance slows
down the amplifi er which improves the phase margin by
moving the unity-gain cross away from the pole formed
by the output impedance and the capacitive load. The zero
created by the RC combination adds phase to ensure that
the total phase lag does not exceed 180 degrees (zero
phase margin) and the amplifi er remains stable. In this
way, the LT1812 is stable with up to 1000pF capacitive
loads in unity gain, and even higher capacitive loads in
higher closed-loop gain confi gurations.

LT1812CS5#TRMPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
High Speed Operational Amplifiers 3mA Hi Speed OA in SOT-23 5
Lifecycle:
New from this manufacturer.
Delivery:
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