7
LTC1051/LTC1053
10513fa
As the ambient temperature rises, the leakage current of
the input protection devices increases, while the charge
injection component of the bias current, for all practical
purposes, stays constant. At elevated temperatures (above
85°C) the leakage current dominates and the bias current
of both inputs assumes the same sign.
The charge injection at the op amp input pins will cause
small output spikes. This phenomenon is often referred to
as “clock feedthrough” and can be easily observed when
the closed-loop gain exceeds 10V/V (Figure 2). The mag-
nitude of the clock feedthrough is temperature indepen-
dent but it increases when the closed-loop gain goes up,
when the source resistance increases and when the gain
setting resistors increase (Figure 2a, 2b). It is important to
note that the output small spikes are centered at 0V level
and do not add to the output offset error budget. For
instance, with R
S
= 1M, the typical output offset voltage
of Figure 2c is:
V
OS(OUT)
10
8
• I
B
+
+ 101V
OS(IN)
A 10pA bias current will yield an output of 1mV ±100µV.
The output clock feedthrough can be attenuated by lower-
ing the value of the gain setting resistors, i.e. R2 = 10k,
R1 = 100, instead of 100k and 1k (Figure 2).
Clock feedthrough can also be attenuated by adding a
capacitor across the feedback resistor to limit the circuit
bandwidth below the internal sampling frequency
(Figure 3).
Input Capacitance
The input capacitance of the LTC1051/LTC1053 op amps
is approximately 12pF. When the LTC1051/LTC1053 op
amps are used with feedback factors approaching unity,
the feedback resistor value should not exceed 7k for
industrial temperature range and 5k for military tempera-
ture range. If a higher feedback resistor value is required,
a feedback capacitor of 20pF should be placed across the
feedback resistor. Note that the most common circuits
with feedback factors approaching unity are unity gain
followers and instrumentation amplifier front ends.
(See Figure 4.)
Figure 2. Clock Feedthrough
Figure 3. Adding a Feedback Capacitor to
Eliminate Clock Feedthrough
+
1/2
LTC1051
R
S
1051/53 F02
(c)
100µs/DIV
(b)
100µs/DIV
(a)
R1
1k
R2
100k
R
S
= 0,
A
V
=11V/V
20mV/DIV
R
S
= 0,
A
V
=101V/V
20mV/DIV
R
S
= 100k,
A
V
=11V/V
20mV/DIV
R
S
= 100k,
A
V
=101V/V
20mV/DIV
Figure 4. Operating the LTC1051
with Feedback Factors Approaching Unity
+
1/2
LTC1051
1051/53 F04
R1
R2 < 7k, IF R1 > >R2
1
2
3
+
1/2
LTC1051
R
S
1051/53 F03
R1
1k
R2
100k
C
1000pF
1
2
3
100µs/DIV
R
S
= 100k
A
V
=101V/V
R
S
= 1M
A
V
=101V/V
20mV/DIV
APPLICATIO S I FOR ATIO
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LTC1051/LTC1053
8
10513fa
LTC1051/LTC1053 as AC Amplifiers
Although initially chopper stabilized op amps were de-
signed to minimize DC offsets and offset drifts, the
LTC1051/LTC1053 family, on top of its outstanding DC
characteristics, presents efficient AC performance. For
instance, at single 5V supply, each op amp typically
consumes 0.5mA and still provides 1.8MHz gain band-
width product and 3V/µs slew rate. This, combined with
almost distortionless swing to the supply rails (Figure 8),
makes the LTC1051/LTC1053 op amps nearly general
purpose. To further expand this idea (the “aliasing” phe-
nomenon) which can occur under AC conditions, should
be described and properly evaluated.
Aliasing
The LTC1051/LTC1053 are equipped with internal cir-
cuitry to minimize aliasing. Aliasing, no matter how small,
occurs when the input signal approaches and exceeds the
internal sampling rate. Aliasing is caused by the sampled
data nature of the chopper op amps. A generalized study
of this phenomenon is beyond the scope of a data sheet;
however, a set of rules of thumb can answer many
questions:
1. Alias signals can be generally defined as output AC
signals at a frequency of nf
CLK
± mf
IN
. The nf
CLK
term is the
internal sampling frequency of the chopper stabilized op
amps and its harmonics; mf
IN
is the frequency of the input
signal and its harmonics, if any.
+
1/2
LTC1051
1051/53 F05a
R1
1k
R2
10k
1
2
3
f
IN
0.8V
P-P
0.1µF
0.1µF
50pF
5V
–5V
V
OUT
B: MAG
RANGE: 9dBV
STATUS: PAUSED
RMS: 25
20dBV
15dB
/DIV
100
START: 100Hz
X: 1825Hz
BW: 47.742Hz
Y: –70.72dBV
STOP: 5 100Hz
f
IN
= 750Hz f
CLK
– f
IN
2f
IN
2f
CLK
– f
IN
80dB
A: MAG
RANGE: 11dBV
STATUS: PAUSED
RMS: 25
20dBV
15dB
/DIV
100
CENTER: 10 000Hz
X: 5550Hz
BW: 95.485Hz
Y: –63.91dBV
SPAN: 10 000Hz
f
IN
= 10kHz
6f
CLK
– f
IN
74dB
Figure 5a. Output Voltage Spectrum of 1/2 LTC1051 Operating as an Inverting Amplifier with Gain of 10,
and Amplifying a 750Hz/800mV, Input AC Signal
Figure 5b. Same as Figure 5a, but the AC Input Signal is 900mV, 10kHz
APPLICATIO S I FOR ATIO
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9
LTC1051/LTC1053
10513fa
2. If we arbitrarily accept that “aliasing” occurs when
output alias signals reach an amplitude of 0.01% or more
of the output signal, then: the approximate minimum
frequency of an AC input signal which will cause aliasing
is equal to the internal clock frequency multiplied by the
square root of the op amp feedback factor. For instance,
with closed-loop gain of –10, the feedback factor is 1/11
and if f
CLK
= 2.6kHz, alias signals can be detected when
the frequency of the input signal exceeds 750Hz to 800Hz
(Figure 5a).
3. The number of alias signals increases when the input
signal frequency increases (Figure 5b).
4. When the frequency, f
IN
, of the input signal is less than
f
CLOCK
, the alias signal(s) amplitude(s) directly scale with
the amplitude of the incoming signal. The output “signal to
alias ratio” cannot be increased by just boosting the input
signal amplitude. However, when the input AC signal
frequency well exceeds the clock frequency, the amplitude
of the alias signals does not directly scale with the input
amplitude. The “signal to alias ratio” increases when the
output swings closely to the rails. (See Figure 5b and
Figure 7.) It is important to note that the LTC1051/
LTC1053 op amps, under light loads (R
L
10k), swing
closely to the supply rails without generating harmonic
distortion (Figure 8).
B: MAG
RANGE: 9dBV
STATUS: PAUSED
RMS: 25
13dBV
15dB
/DIV
107
CENTER: 2 625Hz
X: 2535Hz
BW: 19.097Hz
Y: –74.16dBV
SPAN: 2 000Hz
f
IN
= 2.685kHz
f
CLK
2f
CLK
– f
IN
83.5dB
+
1/2
LTC1051
1051/53 F05a
10k
10k
0.1µF
0.1µF
50pF
5V
–5V
NOTE: THE f
CLK
– f
IN
= 85Hz
ALIAS FREQUENCY IS 95dB
DOWN FROM THE OUTPUT LEVEL
V
IN
= 10kHz
8V
P-P
Figure 6b. Output Voltage Spectrum of 1/2 LTC1051 Operating as a Unity-Gain Inverting Amplifier.
V
S
= ±5V, R
L
= 10k, C
L
= 50pF, V
IN
= 8V
P-P
, 10kHz
Figure 6a. Output Voltage Spectrum of 1/2 LTC1051 Operating as a Unity-Gain Inverting Amplifier.
V
S
= ±5V, R
L
= 10k, C
L
= 50pF, V
IN
= 8V
P-P
, 2.685kHz
B: MAG
RANGE: 9dBV
STATUS: PAUSED
RMS: 50
13dBV
15dB
/DIV
107
CENTER: 10 000Hz
X: 10000Hz
BW: 95.485Hz
Y: 7.98dBV
SPAN: 10 000Hz
f
IN
= 10kHzf
IN
– f
CLK
2 • f
CLK
6f
CLK
– f
IN
80dB
15dB
1kHz
5f
CLK
– f
IN
f
IN
– 2f
CLK
NOTE: ALL ALIAS FREQUENCY
80dB TO 84dB DOWN FROM OUTPUT
APPLICATIO S I FOR ATIO
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LTC1053CSW#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Precision Amplifiers Quad Chopper Stabilized OA
Lifecycle:
New from this manufacturer.
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