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THS4502 Datasheet, PDF (26/49 Pages) Texas Instruments – WIDEBAND, LOW-DISTORTION FULLY DIFFERENTIAL AMPLIFIERS
THS4502
THS4503
SLOS352E – APRIL 2002 – REVISED OCTOBER 2011
RS
CG Rg
Rf
VS
RT
15 V
Riso CS
VOCM
+-
THS4500/2
VDD
RL
0.1 µF
-+
Riso CS
Rf
Rg
CG
VOD = 26 VPP
Fully Differential Line Driver With High Output Swing
Figure 99.
Filtering With Fully Differential Amplifiers
Similar to their single-ended counterparts, fully
differential amplifiers have the ability to couple
filtering functionality with voltage gain. Numerous filter
topologies can be based on fully differential
amplifiers. Several of these are outlined in A
Differential Circuit Collection, (literature number
SLOA064) referenced at the end of this data sheet.
The circuit below depicts a simple two-pole low-pass
filter applicable to many different types of systems.
The first pole is set by the resistors and capacitors in
the feedback paths, and the second pole is set by the
isolation resistors and the capacitor across the
outputs of the isolation resistors.
CF1
RS
Rg1
Rf1
VS
RT
+
Riso
-
C VO
-+
Rg2
Riso
Rf2
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SETTING THE OUTPUT COMMON-MODE
VOLTAGE WITH THE VOCM INPUT
The output common-mode voltage pin provides a
critical function to the fully differential amplifier; it
accepts an input voltage and reproduces that input
voltage as the output common-mode voltage. In other
words, the VOCM input provides the ability to level-shift
the outputs to any voltage inside the output voltage
swing of the amplifier.
A description of the input circuitry of the VOCM pin is
shown below to facilitate an easier understanding of
the VOCM interface requirements. The VOCM pin has
two 50-kΩ resistors between the power supply rails to
set the default output common-mode voltage to
midrail. A voltage applied to the VOCM pin alters the
output common-mode voltage as long as the source
has the ability to provide enough current to overdrive
the two 50-kΩ resistors. This phenomenon is
depicted in the VOCM equivalent circuit diagram. The
table contains some representative examples to aid in
determining the current drive requirement for the
VOCM voltage source. This parameter is especially
important when using the reference voltage of an
analog-to-digital converter to drive VOCM. Output
current drive capabilities differ from part to part, so a
voltage buffer may be necessary in some
applications.
VS+
VOCM
IIN
R = 50 kΩ
IIN =
2 VOCM - VS+ - VS-
R
R = 50 kΩ
VS-
Equivalent Input Circuit for VOCM
Figure 101.
CF2
A Two-Pole, Low-Pass Filter Design Using a Fully
Differential Amplifier With Poles Located at:
P1 = (2πRfCF)-1 in Hz and P2 = (4πRisoC)-1 in Hz
Figure 100.
Often times, filters like these are used to eliminate
broadband noise and out-of-band distortion products
in signal acquisition systems. It should be noted that
the increased load placed on the output of the
amplifier by the second low-pass filter has a
detrimental effect on the distortion performance. The
preferred method of filtering is using the feedback
network, as the typically smaller capacitances
required at these points in the circuit do not load the
amplifier nearly as heavily in the pass-band.
By design, the input signal applied to the VOCM pin
propagates to the outputs as a common-mode signal.
As shown in the equivalent circuit diagram, the VOCM
input has a high impedance associated with it,
dictated by the two 50-kΩ resistors. While the high
impedance allows for relaxed drive requirements, it
also allows the pin and any associated printed-circuit
board traces to act as an antenna. For this reason, a
decoupling capacitor is recommended on this node
for the sole purpose of filtering any high frequency
noise that could couple into the signal path through
the VOCM circuitry. A 0.1-µF or 1-µF capacitance is a
reasonable value for eliminating a great deal of
broadband interference, but additional, tuned
decoupling capacitors should be considered if a
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