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PDF LTC1563-2 Data sheet ( Hoja de datos )

Número de pieza LTC1563-2
Descripción Active RC/ 4th Order Lowpass Filter Family
Fabricantes Linear Technology 
Logotipo Linear Technology Logotipo



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LTC1563-2/LTC1563-3
Active RC, 4th Order
Lowpass Filter Family
FEATURES
Extremely Easy to Use—A Single Resistor Value
Sets the Cutoff Frequency (256Hz < fC < 256kHz)
Extremely Flexible—Different Resistor Values
Allow Arbitrary Transfer Functions with or without
Gain (256Hz < fC < 256kHz)
Supports Cutoff Frequencies Up to 360kHz Using
FilterCADTM
LTC1563-2: Unity-Gain Butterworth Response Uses a
Single Resistor Value, Different Resistor Values
Allow Other Responses with or without Gain
LTC1563-3: Unity-Gain Bessel Response Uses a
Single Resistor Value, Different Resistor Values
Allow Other Responses with or without Gain
Rail-to-Rail Input and Output Voltages
Operates from a Single 3V (2.7V Min) to ±5V Supply
Low Noise: 36µVRMS for fC = 25.6kHz, 60µVRMS for
fC = 256kHz
fC Accuracy < ±2% (Typ)
DC Offset < 1mV
Cascadable to Form 8th Order Lowpass Filters
Available in NarroUw SSOP-16 Package
APPLICATIO S
Discrete RC Active Filter Replacement
Antialiasing Filters
Smoothing or Reconstruction Filters
Linear Phase Filtering for Data Communication
Phase Locked Loops
DESCRIPTIO
The LTC®1563-2/LTC1563-3 are a family of extremely
easy-to-use, active RC lowpass filters with rail-to-rail
inputs and outputs and low DC offset suitable for systems
with a resolution of up to 16 bits. The LTC1563-2, with a
single resistor value, gives a unity-gain Butterworth
response. The LTC1563-3, with a single resistor value,
gives a unity-gain Bessel response. The proprietary
architecture of these parts allows for a simple resistor
calculation:
R = 10k (256kHz/fC); fC = Cutoff Frequency
where fC is the desired cutoff frequency. For many appli-
cations, this formula is all that is needed to design a filter.
By simply utilizing different valued resistors, gain and
other responses are achieved.
The LTC1563-X features a low power mode, for the lower
frequency applications, where the supply current is re-
duced by an order of magnitude and a near zero power
shutdown mode.
The LTC1563-Xs are available in the narrow SSOP-16
package (Same footprint as an SO-8 package).
, LTC and LT are registered trademarks of Linear Technology Corporation.
FilterCAD is trademark of Linear Technology Corporation.
All other trademarks are the property of their respective owners.
TYPICAL APPLICATIO
Single 3.3V, 256Hz to 256kHz Butterworth Lowpass Filter
3.3V
0.1µF
R
R
R
VIN
0.1µF
LTC1563-2
1
LP
2
SA
V+ 16
15
LPB
3
NC
4
INVA
5
NC
14
NC
13
INVB
12
NC
6
LPA
7
AGND
8 V
11
SB
10
NC
9
EN
( )fC = 256kHz
10k
R
VOUT
R
R
R
1563 TA01
Frequency Response
10
0
–10
–20
–30
–40
–50
–60
–70
–80
100
R = 10k
fC = 256kHz
R = 10M
fC = 256Hz
1k 10k 100k
FREQUENCY (Hz)
1M
1563 TA02
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LTC1563-2 pdf
LTC1563-2/LTC1563-3
TYPICAL PERFOR A CE CHARACTERISTICS
Output Voltage Swing High vs
Load Resistance
3.4
VS = SINGLE 3.3V
3.2
3.0
2.8
HS MODE
2.6
LP MODE
2.4
2.2
2.0
100
1k
10k 100k
LOAD RESISTANCE—LOAD TO GROUND ()
1563 G01
Output Voltage Swing Low vs
Load Resistance
0.025
VS = SINGLE 3.3V
0.020
HS MODE
0.015
LP MODE
Output Voltage Swing High vs
Load Resistance
5.5
VS = SINGLE 5V
5.0
4.5
HS MODE
4.0
LP MODE
3.5
3.0
2.5
100
1k
10k 100k
LOAD RESISTANCE—LOAD TO GROUND ()
1563 G02
Output Voltage Swing Low vs
Load Resistance
0.025
0.020
VS = SINGLE 5V
HS MODE
0.015
LP MODE
0.010
0.010
0.005
0.005
0
100
1k
10k 100k
LOAD RESISTANCE—LOAD TO GROUND ()
1563 G04
THD + Noise vs Input Voltage
–40
3.3V SUPPLY
–50
5V SUPPLY
–60
±5V SUPPLY
–70
–80
fC = 25.6kHz
–90 LOW POWER MODE
fIN = 5kHz
–100
0.1
1
INPUT VOLTAGE (VP-P)
10
1563 G07
0
100
1k
10k 100k
LOAD RESISTANCE—LOAD TO GROUND ()
1563 G05
THD + Noise vs Input Voltage
–40
3.3V SUPPLY
–50
5V SUPPLY
–60
±5V SUPPLY
–70
–80
fC = 25.6kHz
–90 HIGH SPEED MODE
fIN = 5kHz
–100
0.1
1
INPUT VOLTAGE (VP-P)
10
1563 G08
Output Voltage Swing High vs
Load Resistance
5.5
VS = ±5V
5.0
4.5
HS MODE
4.0
LP MODE
3.5
3.0
2.5
100
1k
10k 100k
LOAD RESISTANCE—LOAD TO GROUND ()
1563 G03
Output Voltage Swing Low vs
Load Resistance
–4.3
VS = ± 5V
–4.4
–4.5
–4.6
–4.7
HS MODE
–4.8
–4.9
LP MODE
–5.0
100
1k
10k 100k
LOAD RESISTANCE—LOAD TO GROUND ()
1563 G06
THD + Noise vs Input Voltage
–40
3.3V SUPPLY
–50
5V SUPPLY
–60
±5V SUPPLY
–70
–80
fC = 256kHz
–90 HIGH SPEED MODE
fIN = 50kHz
–100
0.1
1
INPUT VOLTAGE (VP-P)
10
1563 G09
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LTC1563-2 arduino
LTC1563-2/LTC1563-3
APPLICATIONS INFORMATION
Output Loading: Resistive and Capacitive
The op amps of the LTC1563-X have a rail-to-rail output
stage. To obtain maximum performance, the output load-
ing effects must be considered. Output loading issues can
be divided into resistive effects and capacitive effects.
Resistive loading affects the maximum output signal swing
and signal distortion. If the output load is excessive, the
output swing is reduced and distortion is increased. All of
the output voltage swing testing on the LTC1563-X is done
with R22 = 100k and a 10k load resistor. For best undistorted
output swing, the output load resistance should be greater
than 10k.
Capacitive loading on the output reduces the stability of
the op amp. If the capacitive loading is sufficiently high,
the stability margin is decreased to the point of oscillation
at the output. Capacitive loading should be kept below
30pF. Good, tight layout techniques should be maintained
at all times. These parts should not drive long traces and
must never drive a long coaxial cable. When probing the
LTC1563-X, always use a 10x probe. Never use a 1x probe.
A standard 10x probe has a capacitance of 10pF to 15pF
while a 1x probe’s capacitance can be as high as 150pF.
The use of a 1x probe will probably cause oscillation.
For larger capacitive loads, a series isolation resistor can
be used between the part and the capacitive load. If the
load is too great, a buffer must be used.
Layout Precautions
The LTC1563-X is an active RC filter. The response of the
filter is determined by the on-chip capacitors and the
external resistors. Any external, stray capacitance in par-
allel with an on-chip capacitor, or to an AC ground, can
alter the transfer function.
Capacitance to an AC ground is the most likely problem.
Capacitance on the LPA or LPB pins does not affect the
transfer function but does affect the stability of the op
amps. Capacitance on the INVA and INVB pins will affect
the transfer function somewhat and will also affect the
stability of the op amps. Capacitance on the SA and SB
pins alters the transfer function of the filter. These pins are
the most sensitive to stray capacitance. Stray capacitance
on these pins results in peaking of the frequency response
near the cutoff frequency. Poor layout can give 0.5dB to
1dB of excess peaking.
To minimize the effects of parasitic layout capacitance, all
of the resistors for section A should be placed as close as
possible to the SA pin. Place the R31 resistor first so that
it is as close as possible to the SA pin on one end and as
close as possible to the INVA pin on the other end. Use the
same strategy for the layout of section B, keeping all of the
resistors as close as possible to the SB node and first
placing R32 between the SB and INVB pins. It is also best
if the signal routing and resistors are on the same layer as
the part without any vias in the signal path.
Figure 1 illustrates a good layout using the LTC1563-X
with surface mount 0805 size resistors. An even tighter
layout is possible with smaller resistors.
R11
VIN
LTC1563-X
VOUT
R12
1653 F01
Figure 1. PC Board Layout
Single Pole Sections and Odd Order Filters
The LTC1563 is configured to naturally form even ordered
filters (2nd, 4th, 6th and 8th). With a little bit of work,
single pole sections and odd order filters are easily achieved.
To form a single pole section you simply use the op amp,
the on-chip C1 capacitor and two external resistors as
shown in Figure 2. This gives an inverting section with the
gain set by the R2-R1 ratio and the pole set by the R2-C1
time constant. You can use this pole with a 2nd order
section to form a noninverting gain 3rd order filter or as a
stand alone inverting gain single pole filter.
Figure 3 illustrates another way of making odd order
filters. The R1 input resistor is split into two parts with an
additional capacitor connected to ground in between the
resistors. This “TEE” network forms a single real pole. RB1
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