LTC1152CS8#TRPBF

4
LTC1152
TYPICAL PERFORMANCE CHARACTERISTICS
UW
POWER SUPPLY VOLTAGE (±V)
12
COMMON-MODE RANGE LIMIT (V)
354
6
7
1152 G01
8
6
4
2
0
–2
–4
–6
–8
Common-Mode Range vs
Supply Voltage
TOTAL SUPPLY VOLTAGE (V)
02
SUPPLY CURRENT (mA)
3.0
2.5
2.0
1.5
1.0
4
6810
1152 G02
12 14
T
A
= 25°C
Supply Current vs Supply Voltage
TEMPERATURE (°C)
50 –25
POWER SUPPLY CURRENT (mA)
2.0
1.9
1.8
1.7
1.6
1.5
1.4
02550
1152 G03
75 100
V
S
= 5V
Output Swing vs Load Resistance
LOAD RESISTANCE (k)
0.2
OUTPUT SWING (±V)
1
5
10 200
1152 G04
0.5 2
20
50
100
6
5
4
3
2
1
0
T
A
= 25°C
V
S
= SINGLE 5V
V
S
= SINGLE 3V
V
S
= ±2.5V
V
S
= ±1.5V
TOTAL SUPPLY VOLTAGE (V)
2
OUTPUT SHORT-CIRCUIT CURRENT (mA)
40
30
20
10
0
46810
1152 G05
12 14
SOURCE
SINK
T
A
= 25°C
Output Short-Circuit Current vs
Supply Voltage
TOTAL SUPPLY VOLTAGE (V)
2
OPEN-LOOP OUTPUT RESISTANCE ()
300
250
200
150
100
46810
1152 G06
12 14
T
A
= 25°C
Open-Loop Output Resistance vs
Supply Voltage
Charge Pump Voltage vs
Supply Voltage
Charge Pump Voltage vs
Load Current Input Bias Current vs Temperature
TEMPERATURE (°C)
–50
INPUT BIAS CURRENT (±pA)
1000
100
10
2525 0 50 75 100
1152 G09
V
S
= 5V
Supply Current vs Temperature
TOTAL SUPPLY VOLTAGE (V)
2
CHARGE PUMP VOLTAGE, V
CP
– V
+
(V)
3
2
1
0
4
6810
1152 G07
12 14
T
A
= 25°C
LOAD CURRENT (µA)
0
CHARGE PUMP VOLTAGE, V
CP
– V
+
(V)
40 60 10020 80
120 140
160
1152 G08
3
2
1
0
T
A
= 25°C
V
S
= 5V
5
LTC1152
TYPICAL PERFORMANCE CHARACTERISTICS
UW
V
S
= ±2.5V
A
V
= 1 1152 G16
FREQUENCY (Hz)
POWER SUPPLY REJECTION RATIO (dB)
80
70
60
50
40
30
20
10
0
–10
10 1k 10k 1M
1152 G14
100 100k
+PSRR
PSRR
T
A
= 25°C
FREQUENCY (kHz)
0.01
VOLTAGE GAIN (dB)
0.1 1 10
1152 G12
60
50
40
30
20
10
0
10
20
30
–40
PHASE SHIFT (DEG)
180
160
140
120
100
80
60
40
20
0
–20
T
A
= 25°C
V
S
= ±2.5V
C
COMP
= 0.1µF
PHASE
GAIN
Gain and Phase Shift vs
Frequency
Gain and Phase Shift vs
Frequency
FREQUENCY (Hz)
VOLTAGE GAIN (dB)
PHASE SHIFT (DEG)
70
60
50
40
30
20
10
0
10
–20
120
100
80
60
40
20
0
1k 100k 1M 10M
1152 G10
10k
T
A
= 25°C
V
S
= ±2.5V
PIN 5 = NC
PHASE
GAIN
Gain and Phase Shift vs
Frequency
Common-Mode Rejection Ratio vs
Frequency
Power Supply Rejection Ratio vs
Frequency
0.1Hz to 10Hz Input Noise
TIME (SEC)
0
(µV)
2
1
0
–1
–2
8
1152 G18
2
4
6
10
Voltage Noise vs Frequency
FREQUENCY (Hz)
150
125
100
75
50
25
0
1 100 1k 10k
1152 G15
10
VOLTAGE NOISE (nV/Hz)
Large-Signal Transient Response
V
S
= ±2.5V
A
V
= 1 1152 G17
Small-Signal Transient Response
FREQUENCY (kHz)
COMMON-MODE REJECTION RATIO (dB)
110
100
90
80
70
60
50
40
30
0.1 10 100 1000
1152 G13
1
T
A
= 25°C
V
S
= ±2.5V
FREQUENCY (Hz)
VOLTAGE GAIN (dB)
PHASE SHIFT (DEG)
1k 100k 1M 10M
1152 G11
10k
T
A
= 25°C
V
S
= ±2.5V
C
COMP
= 1000pF
PHASE
GAIN
70
60
50
40
30
20
10
0
10
–20
120
100
80
60
40
20
0
20
40
–60
6
LTC1152
U
S
A
O
PP
L
IC
AT
I
WU
U
I FOR ATIO
Rail-to-Rail Operation
The LTC1152 is a rail-to-rail input common-mode range,
rail-to-rail output swing op amp. Most CMOS op amps,
including the entire LTC zero-drift amplifier line, and even
a few bipolar op amps, can and do, claim rail-to-rail output
swing. One obvious use for such a device is to provide a
unity-gain buffer for 0V to 5V signals running from a single
5V power supply. This is not possible with the vast
majority of so-called “rail-to-rail” op amps; although the
output can swing to both rails, the negative input (which
is connected to the output) will exceed the common-mode
input range of the device at some point (generally about
1.5V below the positive supply), opening the feedback
loop and causing unpredictable and sometimes bizarre
behavior.
The LTC1152 is an exception to this rule. It features both
rail-to-rail output swing and rail-to-rail input common-
mode range (CMR); the input CMR actually extends be-
yond either rail by about 0.3V. This allows unity-gain
buffer circuits to operate with any input signal within the
power supply rails; input signal swing is limited only by the
output stage swing into the load. Additionally, signals
occurring at either rail (power supply current sensing, for
example) can be amplified without any special circuitry.
Internal Charge Pump
The LTC1152 achieves its rail-to-rail input CMR by using
a charge pump to generate an internal voltage approxi-
mately 2V higher than V
+
. The input stages of the op amp
are run from this higher voltage, making signals at V
+
appear to be 2V below the front end’s power supply (Figure
1). The charge pump is contained entirely within the
LTC1152; no external components are required.
About 100µV
P-P
of residual charge pump switching noise
will be present on the output of the LTC1152. This
feedthrough is at 4.7MHz, higher than the gain-bandwidth
of the LTC1152, and will generally not cause any prob-
lems. Very sensitive applications can reduce this
feedthrough by connecting a capacitor from the CP pin
(pin 8) to V
+
(pin 7); a 0.1µF capacitor will reduce charge
pump feedthrough to negligible levels. The LTC1152 in-
cludes an internal diode from pin 8 to pin 7 to prevent
external parasitic capacitance from lengthening start-up
+
OUT
OUTPUT
RAIL TO RAIL
INPUT
0.1µF*
*OPTIONAL EXTERNAL
CAPACITOR TO REDUCE
CHARGE PUMP FEEDTHROUGH
V
CC
+ 2V
V
CC
(PIN 7)
CP (PIN 8)
+IN
–IN
1152 F01
INTERNAL
CHARGE
PUMP
Figure 1. LTC1152 Internal Block Diagram
time. This diode can stand short-term peak currents of
about 50mA, allowing it to quickly charge external capaci-
tance to ground or V
. Large capacitors (>1µF) should not
be connected between pin 8 and ground or V
to prevent
excessive diode current from flowing at start-up. The
LTC1152 can withstand continuous short circuits be-
tween pin 8 and V
+
; however, short circuiting pin 8 to
ground or V
will cause large amounts of current to flow
through the diode, destroying the LTC1152. Don’t do it.
Output Drive
The LTC1152 features an enhanced output stage that can
sink and source 10mA with a single 5V supply while
maintaining rail-to-rail output swing under most loading
conditions. The output stage can be modeled as a perfect
rail-to-rail voltage source with a resistor in series with it;
this open-loop output resistance limits the output swing
by creating a resistor divider with the output load.
The output resistance drops as total power supply voltage
increases, as shown in the typical performance curves. It
is typically 140 with a single 5V supply, allowing a 4.4V
output swing into a 1k resistor with a single 5V supply.
OUT (PIN 6)
140 AT 5V SUPPLY
LTC1152
OUTPUT
DRIVER
V
CC
(PIN 7)
R
LOAD
R
OUT
1152 F02
Figure 2. LTC1152 Output Resistance Model

LTC1152CS8#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Precision Amplifiers R2R In R2R Out Zero-Drift Op Amp
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
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