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THS4532_16 Datasheet, PDF (44/58 Pages) Texas Instruments – Ultra Low Power, Rail-to-Rail Output, Fully-Differential Amplifier
THS4532
SLOS829A – FEBRUARY 2013 – REVISED JULY 2015
www.ti.com
Systems Examples (continued)
9.3.3.1 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 THS5432 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 98), 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.
50-Input Match,
Gain of 2 V/V from Rt,
Single-Ended Source to
Differential Output
Wideband,
Fully-Differential Amplifier
Rf1
1.02 kΩ
50-Ω
Source
C1
Rg1
100 nF 499 Ω
Rt
52.3 Ω
Vocm
Rg2
523 Ω
Vcc
–
+
FDA –
+
PD
Vcc
Rload
500 Ω
Output
Measurement
Point
C2
100 nF
Rf2
1.02 kΩ
Figure 98. AC-Coupled, Single-Ended Source to a Differential Gain of 2 V/V Test Circuit
44
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