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THS4551 Datasheet, PDF (31/70 Pages) Texas Instruments – Low-Noise, Precision, 150-MHz, Fully Differential Amplifier
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THS4551
SBOS778A – APRIL 2016 – REVISED AUGUST 2016
Taking a more complex example by using the THS4551 to attenuate a large bipolar input signal in a dc-coupled
design for an ADC is shown in Figure 71. To remove the peaking for this low-noise gain design, the two CF
elements and an input capacitor are added to shape the noise gain at high frequencies to a capacitive divider, as
described in the Designing Attenuators section. In this example (including the 1.2-pF internal differential capacitor
at the inputs and the 0.6-pF internal feedback capacitors), the high-frequency noise gain is 3 V/V and a flat
frequency response with approximately 45 MHz of –3-dB BW is delivered.
10 k
+
4.096 V
10 k
±
VOCM
1 µF
Gain of 0.2 V/V,
DC-Coupled,
Single-Ended Source to
Differential Output
RG1
4.99 k
VS+
5V +
±
VS-
0V +
±
VS = ±18 V
VOCM
2.6 pF
RG2
4.99 k
3.1 pF
RF1
1k
VS+
THS4551 Wideband,
Fully Differential Amplifier
VOUT = 7.2 VPP
Differential
±
+
FDA
±
+
PD
VS- VS+
RF2
1k
RL
A 1-k load is very
1 k important to include because
of high-frequency resonance;
no load may oscillate.
For Attenuator Design:
NG1 = 1.2
NG2 = 3
GBP = 135 MHz
Zo = 14.3 MHz
3.1 pF
Copyright © 2016, Texas Instruments Incorporated
Figure 71. DC-Coupled, Single-Ended to Differential Attenuator Design
In this example, the output VOCM is 4.096 V / 2, which equals 2.048 V and the source signal VCM is 0 V. These
values set the nominal input pin VICM to 2.048 V × 4.99 kΩ / (4.99 kΩ + 1 kΩ) = 1.71 V. Applying a ±18-V input at
the 4.99-kΩ input resistor produces a 7.2-VPP differential output. That is, a ±1.8-V swing on the lower side around
the 2.048-V common-mode voltage. This 0.248-V to 3.84-V relative-to-ground swing at the output is well within
the 0.2-V output headrooms to the 0-V to 5-V supplies used in the example in Figure 71 (with the same swing
inverted on the other output side). That output swing on the lower side produces an attenuated input common
mode swing of (±1.8 V × (4.99 kΩ / (4.99 kΩ + 1 kΩ)) = ±1.5 V around the midscale input bias of 1.71 V. This
0.2-V to 3.2-V input common-mode swing is well within the available 0-V to 3.8-V input range. This ±18-V bipolar
input signal is delivered to a SAR ADC with a 7.2-VPP differential output with all I/O nodes operating in range
using a single 5-V supply design. The source must sink the 2.048 V / 5.99 kΩ = 0.34-mA common-mode level-
shifting current to take the input 0-V common-mode voltage up to the midscale 1.71-V VICM operating voltage.
Using the single-ended input impedance of Equation 4, the source must also drive an apparent input load of
5.44 kΩ.
Most designs do not run into an input range limit. However, using the approach shown in this section can allow a
quick assessment of the input VICM range under the intended full-scale output condition. The THS4551 TINA-TI™
model can also be used to plot the input voltages under the intended swings and application circuit to verify that
there is no limiting from this effect. Driving the I/O nodes out of range in the TINA-TI™ model results in
convergence problems. Increasing the positive and negative supplies slightly in simulation is an easy way to
discover the simulated swings that might be going out of range.
Copyright © 2016, Texas Instruments Incorporated
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