Low Voltage and Current Noise Instrumentation
Amplifier Front Ends
■
Two and Three Op Amp Instrumentation Amplifiers
■
Active Filters
The LT®1113 achieves a new standard of excellence in noise
performance for a dual JFET op amp. The 4.5nV/√Hz 1kHz
noise combined with low current noise and picoampere
bias currents makes the LT1113 an ideal choice for amplifying low level signals from high impedance capacitive
transducers.
The LT1113 is unconditionally stable for gains of 1 or more,
even with load capacitances up to 1000pF. Other key features are 0.4mV VOS and a voltage gain of 4 million. Each
individual amplifier is 100% tested for voltage noise, slew
rate and gain bandwidth.
The design of the LT1113 has been optimized to achieve
true precision performance with an industry standard
pinout in the S0-8 package. A set of specifications are
provided for ±5V supplies and a full set of matching specifications are provided to facilitate the use of the LT1113 in
matching dependent applications such as instrumentation amplifier front ends.
, LTC and LT are registered trademarks of Linear Technology Corporation.
TYPICAL APPLICATIO
Low Noise Hydrophone Amplifier with DC Servo
2
3
–5V TO –15V
R8
100M
R7
1M
< 70°C
A
5V TO 15V
–
1/2
LT1113
+
R6
100k
8
1
4
7
R3
R1*
3.9k
100M
C1*
R2
200Ω
C
HYDRO-
PHONE
DC OUTPUT ≤ 2.5mV FOR T
OUTPUT VOLTAGE NOISE = 128nV/√Hz AT 1kHz (GAIN = 20)
≈ 100pF TO 5000pF; R4C2 > R8CT; *OPTIONAL
C1 ≈ C
T
T
U
C2
0.47µF
1/2
LT1113
1kHz Input Noise Voltage Distribution
5.0
VS = ±15V
T
A
5.2
5.4
= 25°C
5.6
1113 TA02
40
OUTPUT
R4
1M
–
6
R5
1M
5
+
1113 TA01
30
20
PERCENT OF UNITS (%)
10
0
4.04.4
3.8
4.2
INPUT VOLTAGE NOISE (nV/√Hz)
138 S8
276 OP AMPS TESTED
4.85.8
4.6
1
Page 2
LT1113
1
2
3
4
8
7
6
5
TOP VIEW
S8 PACKAGE
8-LEAD PLASTIC SO
B
A
OUT A
–IN A
+IN A
V
–
V
+
OUT B
–IN B
+IN B
A
W
O
LUTEXI TIS
S
A
WUW
U
(Note 1)
ARB
G
Supply Voltage
–55°C to 105°C ............................................... ±20V
105°C to 125°C ............................................... ±16V
Differential Input Voltage ...................................... ±40V
Input Voltage (Equal to Supply Voltage)............... ±20V
Output Short Circuit Duration .......................... 1 Minute
Storage Temperature Range................ –65°C to 150°C
∆V
∆I
∆CMRR Common Mode Rejection Match (Note 11)●75927392dB
∆PSRRPower Supply Rejection Match(Note 11)●76917491dB
Large-Signal Voltage GainVO = ±12V, RL = 10k●80027007002500V/mV
= ±10V, RL = 1k●40015003001000V/mV
V
O
Output Voltage SwingRL = 10k●±13.0±12.5±12.5±12.5V
= 1k●±11.5±12.0±11.0±12.0V
R
L
Supply Current Per Amplifier●5.306.355.306.55mA
= ±5V●5.256.305.256.50mA
V
S
Offset Voltage Match●1.05.01.05.5mV
OS
+
Noninverting Bias Current Match●1.8122.020nA
B
ICS
LT1113AMLT1113M
Note 1: Absolute Maximum Ratings are those values beyond which the
life of the device may be impaired.
Note 2: The LT1113C is guaranteed functional over the Operating
Temperature Range of –40°C to 85°C. The LT1113M is guaranteed
functional over the Operating Temperature Range of –55°C to 125°C.
Note 3: The LT1113C is guaranteed to meet specified performance from
0°C to 70°C. The LT1113C is designed, characterized and expected to
meet specified performance from –40°C to 85°C but is not tested or QA
sampled at these temperatures. For guaranteed I grade parts, consult the
factory. The LT1113M is guaranteed to meet specified performance from
–55°C to 125°C.
Note 4: Typical parameters are defined as the 60% yield of parameter
distributions of individual amplifiers, i.e., out of 100 LT1113s (200 op
amps) typically 120 op amps will be better than the indicated
specification.
Note 5: Warmed-up I
temperature of 50°C from 25°C measurements and 50°C characterization
data.
Note 6: Current noise is calculated from the formula:
i
= (2qIB)
n
where q = 1.6 • 10
swamps the contribution of current noise.
and IOS readings are extrapolated to a chip
B
1/2
–19
coulomb. The noise of source resistors up to 200M
Note 7: Input voltage range functionality is assured by testing offset
voltage at the input voltage range limits to a maximum of 2.3mV
(A grade) to 2.8mV (C grade).
Note 8: This parameter is not 100% tested.
Note 9: Slew rate is measured in A
measured at ±2.5V.
Note 10: The LT1113 is designed, characterized and expected to meet
these extended temperature limits, but is not tested at –40°C and 85°C.
Guaranteed I grade parts are available. Consult factory.
Note 11: ∆CMRR and ∆PSRR are defined as follows:
(1) CMRR and PSRR are measured in µV/V on the individual
amplifiers.
(2) The difference is calculated between the matching sides in µV/V.
(3) The result is converted to dB.
Note 12: The LT1113 is measured in an automated tester in less than
one second after application of power. Depending on the package used,
power dissipation, heat sinking, and air flow conditions, the fully
warmed-up chip temperature can be 10°C to 50°C higher than the
ambient temperature.
= –1; input signal is ±7.5V, output
V
5
Page 6
LT1113
0.1Hz to 10Hz Voltage Noise
LPER
UW
R
F
O
ATYPICA
CCHARA TERIST
E
C
1kHz Output Voltage Noise
Density vs Source Resistance
10k
+
1k
R
SOURCE
–
ICS
Voltage Noise vs Frequency
100
V
N
TA = 25°C
= ±15V
V
S
VOLTAGE NOISE (1µV/DIV)
2
0
Voltage Noise vs
Chip Temperature
10
VS = ±15V
9
8
7
6
5
4
3
2
VOLTAGE NOISE (AT1kHz)(nV/√Hz)
1
0
–75
–5025
4
TIME (SEC)
0
–25
TEMPERATURE (°C)
100
10
V
N
SOURCE
RESISTANCE
TOTAL 1kHz VOLTAGE NOISE DENSITY (nV/√Hz)
6
8
10
1113 G01
1
10010k 100k 1M1k
ONLY
SOURCE RESISTANCE (Ω)
TA = 25°C
V
10M
= ±15V
S
100M
1G
1113 G02
Input Bias and Offset Currents vs
Chip Temperature
100n
VS = ±15V
30n
10n
3n
1n
300p
100p
30p
10p
3p
INPUT BIAS AND OFFSET CURRENTS (A)
125
50
100
75
1113 G04
1p
IB, VCM = 10V
–75
–5025
IB, VCM = 0V
IOS, VCM = 10V
0
–25
TEMPERATURE (°C)
IOS, VCM = 0V
50
75
100
125
1113 G04
10
1/f CORNER
120Hz
RMS VOLTAGE NOISE DENSITY (nV/√Hz)
1
1
101k
10010k
FREQUENCY (Hz)
Input Bias and Offset Currents
Over the Common-Mode Range
400
TA = 25°C
= ±15V
V
S
NOT WARMED UP
300
200
BIAS CURRENT
100
INPUT BIAS AND OFFSET CURRENTS (pA)
0
–15
OFFSET CURRENT
–10–505
COMMON-MODE RANGE (V)
TYPICAL
1113 G03
1015
1113 G06
Common-Mode Limit vs
Temperature
V+ –0
–0.5
–1.0
–1.5
–2.0
4.0
3.5
COMMON-MODE LIMIT (V)
3.0
REFERRED TO POWER SUPPLY
2.5
–
V
+2.0
–60
–20
6
V+ = 5V TO 20V
V– = –5V TO –20V
60
20
TEMPERATURE (°C)
100
1113 G07
Common-Mode Rejection Ratio
vs Frequency
120
100
80
60
40
20
COMMON-MODE REJECTION RATIO (dB)
0
140
1k100k1M10M
10k
FREQUENCY (Hz)
TA = 25°C
V
= ±15V
S
1113 G08
Power Supply Rejection Ratio
vs Frequency
120
100
80
60
40
20
POWER SUPPLY REJECTION RATIO (dB)
0
10
–PSRR
100
1k10k100k
FREQUENCY (Hz)
+PSRR
TA = 25°C
1M10M
1113 G09
Page 7
LPER
TEMPERATURE (°C)
–75
6
5
4
3
2
1
0
–25
50
75
1113 G18
–5025
100
125
0
SLEW RATE (V/µs)
SLEW RATE
GBW
12
10
8
6
4
2
0
GAIN-BANDWIDTH PRODUCT (f
O
= 100kHz)(MHz)
LT1113
UW
R
F
O
ATYPICA
CCHARA TERIST
E
C
ICS
Voltage Gain vs Frequency
180
140
100
60
VOLTAGE GAIN (dB)
20
–20
0.01
1
100
FREQUENCY (Hz)
10k
Small-Signal Transient Response
20mV/DIV
TA = 25°C
= ±15V
V
S
1M
100M
1113 G10
Voltage Gain vs
Chip Temperature
10
9
8
7
6
5
4
3
VOLTAGE GAIN (V/µV)
2
1
0
–75
–5025
–25
CHIP TEMPERATURE (°C)
RL = 1k
0
VS = ±15V
= ±10V, RL = 1k
V
O
= ±12V, RL = 10k
V
O
RL =10k
50
Large-Signal Transient Response
5V/DIV
Gain and Phase Shift vs
Frequency
50
TA = 25°C
= ±15V
V
40
30
20
10
VOLTAGE GAIN (dB)
0
–10
125
100
75
1113 G11
0.1
GAIN
110100
FREQUENCY (MHz)
S
= 10pF
C
L
PHASE
60
80
PHASE SHIFT (DEG)
100
120
140
160
180
1113 G12
Supply Current vs Supply Voltage
6
25°C
5
–55°C
125°C
A
= 1
V
= 10pF
C
L
= ±15V, ± 5V
V
S
1µs/DIV
1113 G13
A
V
C
L
V
S
= 1
= 10pF
= ±15V
Output Voltage Swing vs
Load CurrentCapacitive Load Handling
V+ –0.8
–1.0
–1.2
–1.4
–1.6
1.4
1.2
1.0
0.8
OUTPUT VOLTAGE SWING (V)
0.6
–
V
+0.4
–8
–10
I
SINK
25°C
–55°C
VS = ±5V TO ±20V
125°C
048
–2
–6 –4
OUTPUT CURRENT (mA)
–55°C
25°C
125°C
2
6
10
I
SOURCE
1113 G16
50
VS = ±15V
T
= 25°C
A
40
≥ 10k
R
L
= 100mV
V
O
AV = +10, RF = 10k, CF = 20pF
30
20
OVERSHOOT (%)
10
0
0.1
2µs/DIV
P-P
A
= 1
V
A
= 10
V
1
10
CAPACITIVE LOAD (pF)
100
1000
1113 G14
10000
1113 G17
SUPPLY CURRENT PER AMPLIFIER (mA)
4
0
±5
±10
SUPPLY VOLTAGE (V)
Slew Rate and Gain-Bandwidth
Product vs Temperature
±15
±20
1113 G15
7
Page 8
LT1113
LPER
UW
R
F
O
ATYPICA
CCHARA TERIST
E
C
ICS
Distribution of Offset Voltage Drift
with Temperature (J8)
40
30
20
PERCENT OF UNITS
10
0
–10 –8–2
–12
OFFSET VOLTAGE DRIFT WITH TEMPERATURE (µV/°C)
–4
VS = ±15V
75 J8
150 OP AMPS
0
2–6
4
THD and Noise vs Frequency for
Noninverting Gain
1
ZL = 2k15pF
= 20V
V
P-P
O
AV = +1, +10, +100
MEASUREMENT BANDWIDTH
0.1
= 10Hz TO 80kHz
AV = 100
0.01
0.001
TOTAL HARMONIC DISTORTION + NOISE (%)
0.0001
201k10k 20k
AV = 10
100
FREQUENCY (Hz)
AV = 1
NOISE FLOOR
6
1113 G19
1113 • G22
Distribution of Offset Voltage Drift
with Temperature (N8, S8)
40
30
20
PERCENT OF UNITS
10
8
0
–20 –150
–25
OFFSET VOLTAGE DRIFT WITH TEMPERATURE (µV/°C)
–5
THD and Noise vs Frequency for
Inverting Gain
1
ZL = 2k15pF
= 20V
V
P-P
O
AV = –1, –10, –100
MEASUREMENT BANDWIDTH
0.1
= 10Hz TO 80kHz
0.01
AV = –10
0.001
TOTAL HARMONIC DISTORTION + NOISE (%)
0.0001
201k10k 20k
100
FREQUENCY (Hz)
VS = ±15V
78 S8
100 N8
356 OP AMPS
5
10–10
AV = –100
NOISE FLOOR
152025
1113 G20
AV = –1
1113 G23
Warm-Up Drift
500
VS = ±15V
= 25°C
T
A
400
300
200
100
CHANGE IN OFFSET VOLTAGE (µV)
0
123 5
0
TIME AFTER POWER ON (MINUTES)
IN STILL AIR (S8 PACKAGE
SOLDERED ONTO BOARD)
4
Channel Separation vs Frequency
160
140
120
100
80
60
VS = ±15V
40
CHANNEL SEPARATION (dB)
R
L
V
O
20
TA = 25°C
0
10
LIMITED BY
THERMAL INTERACTION
LIMITED BY
= 1k
= 10V
P-P
10010k 100k10M
1k1M
FREQUENCY (Hz)
PIN-TO-PIN
CAPACITANCE
S8 PACKAGE
N8 PACKAGE
J8 PACKAGE
6
1113 G21
1113 G24
THD and Noise vs Output
Amplitude for Noninverting Gain
1
ZL = 2k15pF, fO = 1kHz
= +1, +10, +100
A
V
MEASUREMENT BANDWIDTH
= 10Hz TO 22kHz
0.1
0.01
0.001
TOTAL HARMONIC DISTORTION + NOISE (%)
0.0001
0.31030
AV = 100
AV = 10
AV = 1
1
OUTPUT SWING (V
8
NOISE FLOOR
)
P-P
1113 • G25
THD and Noise vs Output
Amplitude for Inverting Gain
1
ZL = 2k15pF, fO = 1kHz
= –1, –10, –100
A
V
MEASUREMENT BANDWIDTH
= 10Hz TO 22kHz
0.1
0.01
0.001
TOTAL HARMONIC DISTORTION + NOISE (%)
0.0001
AV = –100
AV = –10
AV = –1
NOISE FLOOR
0.31030
1
OUTPUT SWING (V
P-P
)
1113 • G26
CCIF IMD Test (Equal Amplitude
Tones at 13kHz, 14kHz)*
0.1
VS = ±15V
= 2k
R
L
= 25°C
T
A
0.01
AV = ±10
0.001
INTERMODULATION DISTORTION (AT 1kHz)(%)
0.0001
20m130
0.1
OUTPUT SWING (V
* See LT1115 data sheet for definition of CCIF testing.
P-P
)
10
1113 • G27
Page 9
LT1113
PPLICATI
A
U
O
IFORATIO
S
WU
U
The LT1113 dual in the plastic and ceramic DIP packages
are pin compatible with and directly replace such JFET op
amps as the OPA2111 and OPA2604 with improved noise
performance. Being the lowest noise dual JFET op amp
available to date, the LT1113 can replace many bipolar op
amps that are used in amplifying low level signals from
high impedance transducers. The best bipolar op amps
will eventually loose out to the LT1113 when transducer
impedance increases due to higher current noise. The low
voltage noise of the LT1113 allows it to surpass every dual
and most single JFET op amps available. For the best
performance versus area available anywhere, the LT1113
is offered in the narrow SO-8 surface mount package with
standard pinout and no degradation in performance.
The low voltage and current noise offered by the LT1113
makes it useful in a wide range of applications, especially
where high impedance, capacitive transducers are used
such as hydrophones, precision accelerometers and photo
diodes. The total output noise in such a system is the gain
times the RMS sum of the op amp input referred voltage
noise, the thermal noise of the transducer, and the op amp
bias current noise times the transducer impedance.
Figure 1 shows total input voltage noise versus source
resistance. In a low source resistance (<5k) application
the op amp voltage noise will dominate the total noise.
This means the LT1113 will beat out any dual JFET op amp,
only the lowest noise bipolar op amps have the edge
(at low source resistances). As the source resistance
increases from 5k to 50k, the LT1113 will match the best
bipolar op amps for noise performance, since the thermal
noise of the transducer (4kTR) begins to dominate the
total noise. A further increase in source resistance, above
50k, is where the op amp’s current noise component (2qI
R
) will eventually dominate the total noise. At these
TRANS
B
high source resistances, the LT1113 will out perform
the lowest noise bipolar op amp due to the inherently low
current noise of FET input op amps. Clearly, the LT1113
will extend the range of high impedance transducers
that can be used for high signal to noise ratios. This
makes the LT1113 the best choice for high impedance,
capacitive transducers.
The high input impedance JFET front end makes the
LT1113 suitable in applications where very high charge
sensitivity is required. Figure 2 illustrates the LT1113 in its
inverting and noninverting modes of operation. A charge
amplifier is shown in the inverting mode example; here the
gain depends on the principal of charge conservation at
the input of the LT1113. The charge across the transducer
capacitance, CS, is transferred to the feedback capacitor
CF, resulting in a change in voltage, dV, equal to dQ/CF.
1k
C
S
R
S
–
100
+
C
R
S
10
INPUT NOISE VOLTAGE (nV/√Hz)
1
Figure 1. Comparison of LT1113 and LT1124 Total Output 1kHz Voltage Noise Versus Source Resistance
LT1124
RESISTOR NOISE ONLY
100
1k100M
LT1124*
LT1113*
V
O
S
†
LT1113
LT1113
SOURCE RESISTANCE (Ω)
100k
LT1124
†
10M10k1M
SOURCE RESISTANCE = 2RS = R
* PLUS RESISTOR
†
PLUS RESISTOR 1000pF CAPACITOR
Vn = AV √V
n2(OP AMP)
+ 4kTR + 2q IB • R
1113 • F01
2
9
Page 10
LT1113
PPLICATI
A
U
O
IFORATIO
S
R2
C
B
R
B
R1
CSR
S
TRANSDUCER
Figure 2. Noninverting and Inverting Gain Configurations
WU
–
+
CB ≅ C
S
RB = R
S
RS > R1 OR R2
U
OUTPUT
The gain therefore is 1 + CF/CS. For unity gain, CF should
equal the transducer capacitance plus the input capacitance of the LT1113 and RF should equal RS. In the
noninverting mode example, the transducer current is
converted to a change in voltage by the transducer capacitance; this voltage is then buffered by the LT1113 with a
gain of 1 + R1/R2. A DC path is provided by RS, which is
either the transducer impedance or an external resistor.
Since RS is usually several orders of magnitude greater
than the parallel combination of R1 and R2, RB is added to
balance the DC offset caused by the noninverting input
bias current and RS. The input bias currents, although
small at room temperature, can create significant errors
over increasing temperature, especially with transducer
resistances of up to 100M or more. The optimum value for
RB is determined by equating the thermal noise (4kTRS) to
the current noise (2qIB) times R
in RB = RS = 2VT/I
kT
V
==°
T
q
B
mV atC
2625.
2
. Solving for RS results
S
A parallel capacitor, CB, is used to cancel the phase shift
caused by the op amp input capacitance and RB.
R
F
C
F
–
CSR
TRANSDUCER
S
C
B
+
R
B
Q = CV;
OUTPUT
CB = CFC
RB = RFR
S
S
dQ
= I = C
dt
dt
1113 • F02
dV
Reduced Power Supply Operation
The LT1113 can be operated from ±5V supplies for lower
power dissipation resulting in lower IB and noise at the
expense of reduced dynamic range. To illustrate this
benefit, let’s look at the following example:
An LT1113CS8 operates at an ambient temperature of
25°C with ±15V supplies, dissipating 318mW of power
(typical supply current = 10.6mA for the dual). The SO-8
package has a θJA of 190°C/W, which results in a die
temperature increase of 60.4°C or a room temperature die
operating temperature of 85.4°C. At ±5V supplies, the die
temperature increases by only one third of the previous
amount or 20.1°C resulting in a typical die operating
temperature of only 45.1°C. A 40 degree reduction of die
temperature is achieved at the expense of a 20V reduction
in dynamic range. If no DC correction resistor is used at
the input, the input referred offset will be the input bias
current at the operating die temperature times the transducer resistance (refer to Input Bias and Offset Currents vs
Chip Temperature graph in Typical Performance Characteristics section). A 100mV input VOS is the result of a 1nA
IB (at 85°C) dropped across a 100M transducer resistance; at ±5V supplies, the input offset is only 28mV (IB at
45°C is 280pA). Careful selection of a DC correction
10
Page 11
LT1113
U
O
PPLICATI
A
INPUT: ±5.2V Sine WaveLT1113 OutputOPA2111 Output
resistor (RB) will reduce the IR errors due to IB by an order
of magnitude. A further reduction of IR errors can be
achieved by using a DC servo circuit shown in the applications section of this data sheet. The DC servo has the
advantage of reducing a wide range of IR errors to the
millivolt level over a wide temperature variation. The
preservation of dynamic range is especially important
when reduced supplies are used, since input bias currents
can exceed the nanoamp level for die temperatures
over 85°C.
To take full advantage of a wide input common mode
range, the LT1113 was designed to eliminate phase reversal. Referring to the photographs shown in Figure 3, the
LT1113 is shown operating in the follower mode (AV = +1)
at ±5V supplies with the input swinging ±5.2V. The output
of the LT1113 clips cleanly and recovers with no phase
reversal, unlike the competition as shown by the last
photograph. This has the benefit of preventing lock-up in
servo systems and minimizing distortion components.
The effect of input and output overdrive on one amplifier
has no effect on the other, as each amplifier is biased
independently.
IFORATIO
S
Figure 3. Voltage Follower with Input Exceeding the Common-Mode Range ( VS = ±5V)
WU
U
Advantages of Matched Dual Op Amps
In many applications the performance of a system
depends on the matching between two operational amplifiers rather than the individual characteristics of the two op
amps. Two or three op amp instrumentation amplifiers,
tracking voltage references and low drift active filters
are some of the circuits requiring matching between two
op amps.
The well-known triple op amp configuration in Figure 4
illustrates these concepts. Output offset is a function of the
difference between the two halves of the LT1113. This
error cancellation principle holds for a considerable
number of input referred parameters in addition to
offset voltage and bias current. Input bias current will
be the average of the two noninverting input currents
(IB+). The difference between these two currents (∆IB+)
is the offset current of the instrumentation amplifier.
Common mode and power supply rejections will be
dependent only on the match between the two amplifiers
(assuming perfect resistor matching).
11
Page 12
LT1113
O
PPLICATI
A
15V
3
–
IN
2
6
5
+
IN
WIDEBAND NOISE DC TO 400kHz =
8
+
1/2
LT1113
IC1
–
1
4
–15V
–
1/2
LT1113
IC1
+
INPUT REFERRED NOISE =
7
GAIN =
BANDWIDTH =
C
U
IFORATIO
S
R4
1k
R1
1k
R2
200Ω
R3
1k
R5
1k
100
400kHz
6.6nV/√Hz AT 1kHz
6.6 µV
≤
0.01µF
L
2
3
R7
10k
RMS
WU
R6
10k
C1
50pF
–
1/2
LT1113
IC2
+
U
1
OUTPUT
C
L
1113 • F04
Figure 4. Three Op Amp Instrumentation Amplifier
The concepts of common mode and power supply
rejection ratio match (∆CMRR and ∆PSRR) are best
demonstrated with a numerical example:
Typical performance of the instrumentation amplifier:
Input offset voltage = 0.8mV
Input bias current = 320pA
Input offset current = 10pA
Input resistance = 1011Ω
Input noise = 3.4µV
P-P
High Speed Operation
The low noise performance of the LT1113 was achieved by
making the input JFET differential pair large to maximize
the first stage gain. Increasing the JFET geometry also
increases the parasitic gate capacitance, which if left
unchecked, can result in increased overshoot and ringing.
When the feedback around the op amp is resistive (RF),
a pole will be created with RF, the source resistance and
capacitance (RS,CS), and the amplifier input capacitance
(CIN = 27pF). In closed loop gain configurations and
with RS and RF in the kilohm range (Figure 5), this pole
can create excess phase shift and even oscillation.
A small capacitor (CF) in parallel with RF eliminates this
problem. With RS(CS + CIN) = RFCF, the effect of the
feedback pole is completely removed.
Assume CMRRA = +50µV/V or 86dB,
and CMRRB = + 39µV/V or 88dB,
then ∆CMRR = 11µV/V or 99dB;
if CMRRB = -39µV/V which is still 88dB,
then ∆CMRR = 89µV/V or 81dB
Clearly the LT1113, by specifying and guaranteeing all of
these matching parameters, can significantly improve the
performance of matching-dependent circuits.
C
F
R
F
–
C
IN
R
C
S
S
+
OUTPUT
1113 • F05
Figure 5.
12
Page 13
LT1113
1. ASSUME VOLTAGE NOISE OF LT1113 AND 51Ω SOURCE RESISTOR = 4.6nV/√Hz
2. GAIN WITH n LT1113s IN PARALLEL = n • 200
3. OUTPUT NOISE = √n • 200 • 4.6nV/√Hz
4. INPUT REFERRED NOISE =
OUTPUT NOISE = 4.6
nV/√Hz
n • 200 √n
5. NOISE CURRENT AT INPUT INCREASES √n TIMES
6. IF n = 5, GAIN = 1000, BANDWIDTH = 1MHz, RMS NOISE, DC TO 1MHz =
10Hz Fourth Order Chebyshev Lowpass Filter (0.01dB Ripple)
R2
237k
C1
33nF
R1
237k
V
IN
TYPICAL OFFSET ≈ 0.8mV
1% TOLERANCES
FOR V
= 10V
IN
= –6dB AT f = 16.3Hz
LOWER RESISTOR VALUES WILL RESULT IN LOWER THERMAL NOISE AND LARGER CAPACITORS
R3
249k
C2
100nF
, V
= –121dB AT f > 330Hz
P-P
OUT
–
2
1/2 LT1113
+
3
15V
–15V
8
1
4
R4
154k
R6
249k
C4
330nF
R5
154k
–
6
1/2 LT1113
+
5
C3
10nF
7
1113 • TA06
V
OUT
14
Page 15
PACKAGEDESCRIPTI
0.300 BSC
(0.762 BSC)
0.008 – 0.018
(0.203 – 0.457)
NOTE: LEAD DIMENSIONS APPLY TO SOLDER DIP/PLATE
OR TIN PLATE LEADS
(1.143 – 1.727)
0° – 15°
O
0.045 – 0.068
FULL LEAD
OPTION
0.045 – 0.065
(1.143 – 1.651)
0.014 – 0.026
(0.360 – 0.660)
U
Dimensions in inches (millimeters) unless otherwise noted.
J8 Package
8-Lead CERDIP (Narrow 0.300, Hermetic)
(LTC DWG # 05-08-1110)
CORNER LEADS OPTION
(4 PLCS)
0.023 – 0.045
(0.584 – 1.143)
HALF LEAD
OPTION
0.015 – 0.060
(0.381 – 1.524)
0.100
(2.54)
BSC
0.200
(5.080)
MAX
0.125
3.175
MIN
0.005
(0.127)
MIN
0.025
(0.635)
RAD TYP
0.405
(10.287)
MAX
87
12
65
3
4
0.220 – 0.310
(5.588 – 7.874)
J8 1298
LT1113
0.300 – 0.325
(7.620 – 8.255)
0.065
(1.651)
0.009 – 0.015
(0.229 – 0.381)
+0.035
0.325
–0.015
+0.889
8.255
()
–0.381
*THESE DIMENSIONS DO NOT INCLUDE MOLD FLASH OR PROTRUSIONS.
MOLD FLASH OR PROTRUSIONS SHALL NOT EXCEED 0.010 INCH (0.254mm)
TYP
8-Lead Plastic Small Outline (Narrow 0.150)
0.010 – 0.020
(0.254 – 0.508)
0.008 – 0.010
(0.203 – 0.254)
*
DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE
**
DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD
FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE
× 45°
0.016 – 0.050
(0.406 – 1.270)
0°– 8° TYP
N8 Package
8-Lead PDIP (Narrow 0.300)
(LTC DWG # 05-08-1510)
0.045 – 0.065
(1.143 – 1.651)
0.100
(2.54)
BSC
0.018 ± 0.003
(0.457 ± 0.076)
S8 Package
(LTC DWG # 05-08-1610)
0.053 – 0.069
(1.346 – 1.752)
0.014 – 0.019
(0.355 – 0.483)
TYP
0.130 ± 0.005
(3.302 ± 0.127)
0.125
(3.175)
MIN
0.004 – 0.010
(0.101 – 0.254)
0.050
(1.270)
BSC
0.020
(0.508)
MIN
0.255 ± 0.015*
(6.477 ± 0.381)
0.228 – 0.244
(5.791 – 6.197)
(10.160)
876
1234
0.189 – 0.197*
(4.801 – 5.004)
7
8
1
2
0.400*
MAX
6
3
5
N8 1098
5
0.150 – 0.157**
(3.810 – 3.988)
4
SO8 1298
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.
However, no responsibility is assumed for its use. Linear Technology Corporation makes no representation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
15
Page 16
LT1113
U
O
PPLICATITYPICAL
SA
Light Balance Detection Circuit
R1
1M
I
1
PD
1
I
2
PD
2
C1
2pF TO 8pF
–
1/2 LT1113
+
V
= 1M • (I1 – I2)
OUT
PD
= HAMAMATSU S1336-5BK
1,PD2
WHEN EQUAL LIGHT ENTERS PHOTODIODES, V
V
OUT
1113 • TA07
OUT
< 3mV.
Unity Gain Buffer with Extended Load Capacitance Drive Capability
R2
1k
C1
–
1/2 LT1113
+
V
IN
R1
33Ω
V
C
L
C1 = CL ≤ 0.1µF
OUTPUT SHORT-CIRCUIT CURRENT
(∼30mA) WILL LIMIT THE RATE AT WHICH THE
VOLTAGE CAN CHANGE ACROSS LARGE CAPACITORS
OUT
(I = CdV)
dt
1113 • TA08
RELATED PARTS
PART NUMBERDESCRIPTIONCOMMENTS
LT1028Single Low Noise Precision Op AmpV
LT1124Dual Low Noise Precision Op AmpV
LT1169Dual Low Noise Precision JFET Op Amp10pA I
LT1462Dual Picoamp IB C-LoadTM Op AmpIB = 2pA Max, 10000pF C-Load, IS = 45µA
LT1464Dual Picoamp IB C-Load Op AmpIB = 2pA Max, 10000pF C-Load, IS = 200µA
LT1792Single Low Noise Precision Op AmpSingle LT1113
LT1793Single Low Noise Precision Op AmpSingle LT1169
C-Load is a trademark of Linear Technology Corporation.
Linear Technology Corporation
16
1630 McCarthy Blvd., Milpitas, CA 95035-7417
(408) 432-1900 ● FAX: (408) 434-0507
●
www.linear-tech.com
= 1.1nV/√Hz Max
NOISE
= 4.2nV/√Hz Max
NOISE
B
1113fa LT/TP 0100 2K REV A • PRINTED IN USA
LINEAR TECHNOLOGY CORPORATION 1993
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