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THS4531A_16 Datasheet, PDF (41/59 Pages) Texas Instruments – Ultra Low-Power, Rail-to-Rail Output, Fully Differential Amplifier
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THS4531A
SLOS823C – DECEMBER 2012 – REVISED JANUARY 2016
9.2.6 Single-Ended Input to Differential Output Amplifier
The THS4531A can also be used to amplify and convert single-ended input signals to differential output signals.
A basic block diagram of the circuit is shown in Figure 95 (VOCM and PD inputs not shown). The gain of the
circuit is again set by RF divided by RG.
RG
RF
VIN+
VOUT±
Single-Ended
Input
VS+
Differential
Output
+
THS4531A
±
VS±
RG
RF
VOUT+
Figure 95. Single-Ended Input to Differential Output Amplifier
9.2.6.1 AC-Coupled Signal Path Considerations for Single-Ended Input to Differential Output Conversion
When the signal path can be AC-coupled, the DC biasing for the THS4531A family becomes a relatively simple
task. In all designs, start by defining the output common-mode voltage. The AC-coupling issue can be separated
for the input and output sides of an FDA design. The input can be AC-coupled and the output DC-coupled, or the
output can be ac-coupled and the input dc-coupled, or they can both be AC-coupled.
One situation where the output might be DC-coupled (for an AC-coupled input), is when driving directly into an
ADC where the VOCM control voltage uses the ADC common-mode reference to directly bias the FDA output
common-mode to the required ADC input common-mode. In any case, the design starts by setting the desired
VOCM.
When an AC-coupled path follows the output pins, the best linearity is achieved by operating VOCM at midsupply.
The VOCM voltage must be within the linear range for the common-mode loop, as specified in the headroom
specifications (approximately 0.91 V greater than the negative supply and 1.1 V less than the positive supply). If
the output path is also ac-coupled, simply letting the VOCM control pin float is usually preferred to get a midsupply
default VOCM bias with minimal elements. To limit noise, place a 0.1-µF decoupling capacitor on the VOCM pin to
ground.
After VOCM is defined, check the target output voltage swing to ensure that the VOCM plus the positive and
negative output swing on each side do not clip into the supplies. If the desired output differential swing is defined
as VOPP, divide by 4 to obtain the ±VP swing around VOCM at each of the two output pins (each pin operates 180°
out of phase with the other). Check that VOCM ±VP does not exceed the absolute supply rails for this rail-to-rail
output (RRO) device.
Going to the device input pins side, because both the source and balancing resistor on the nonsignal input side
are DC-blocked (see Figure 96), no common-mode current flows from the output common-mode voltage, thus
setting the input common-mode equal to the output common-mode voltage.
This input headroom also sets a limit for higher VOCM voltages. Because the input VICM is the output VOCM for ac-
coupled sources, the 1.2-V minimum headroom for the input pins to the positive supply overrides the 1.1-V
headroom limit for the output VOCM. Also, the input signal moves this input VICM around the dc bias point, as
described in the section Resistor Design Equations for the Single-Ended to Differential Configuration of the FDA.
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