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THS4541 Datasheet(PDF) 28 Page - Texas Instruments

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Part # THS4541
Description  THS4541-Q1 Negative Rail Input, Rail-to-Rail Output, Precision, 850-MHz Fully Differential Amplifier
PDF  64 Pages
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Manufacturer  TI1 [Texas Instruments]
Direct Link  http://www.ti.com
Logo TI1 - Texas Instruments

THS4541 Datasheet(HTML) 28 Page - Texas Instruments

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‡
(
)
(
)
2
Vod
G
4
Vocm
1
G
1
T
T
Vocm G1
G2
Vicm G1
G2
Vod
G1
G2
1
2
28
THS4541-Q1
SLOS930B – NOVEMBER 2015 – REVISED NOVEMBER 2019
www.ti.com
Product Folder Links: THS4541-Q1
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Copyright © 2015–2019, Texas Instruments Incorporated
8.4 Output DC Error and Drift Calculations and the Effect of Resistor Imbalances
The THS4541-Q1 offers a trimmed input offset voltage and extremely low offset drift over the full –40°C to
+125°C operating range. This offset voltage combines with several other error contribution terms to produce an
initial 25°C differential offset error band, and then a drift over temperature. For each error term, a gain must be
assigned to that term. For this analysis, only DC-coupled signal paths are considered. One new source of output
error (versus typical op amp analysis) arises from the effect that mismatched resistor values and ratios can have
on the two sides of the FDA. Any common-mode voltage or drift creates a differential output error through the
slight mismatches arising from the external feedback and gain-setting resistor tolerances, and the approximation
(or snap) to standard value.
The error terms (25°C and drift), along with the gain to the output differential voltage, include:
•
Input offset voltage—this voltage has a gain equal to the noise gain or 1 + Rf / Rg, where Rg is the total DC
impedance from the input pins back to the source, or a DC reference (typically ground).
•
Input offset current—this current has a gain to the differential output through the average feedback resistor
value.
The remaining terms arise from an assumed range on both the absolute feedback resistor mismatch and the
mismatch in the divider ratio on each side of the FDA. The first of these resistor mismatch terms is the input bias
current creating a differential output offset because of Rf mismatch. For simplicity, the upper Rf and Rg values
are called Rf1 and Rg1 with a ratio of Rf1 / Rg1
≡ G1. The lower elements are defined as Rf2 and Rg2 with a
ratio of Rf2 / Rg2
≡ G2. To compute worst-case contributions, a maximum variation in the design resistor
tolerance is used in the absolute and ratio mismatches. For instance, ±1% tolerance resistors are assumed,
giving a worst-case G1 that is 2% higher than nominal and a G2 that is 2% lower than nominal, with a worst-case
Rf value mismatch of 2% as well. For matched impedance designs with Rt and Rg1 on a single-ended to
differential stage, the standard value snap imposes a fixed mismatch in the initial feedback ratios with the resistor
tolerance adding a mismatch to this initial ratio mismatch. Define the selected external resistor tolerance as ±T
(so for 1% tolerance resistors, T = 0.01).
•
Total gain for bias current error is ±2 × T × Rfnom
Anything that generates an output common-mode level or shift over temperature also generates an output
differential error term if the two feedback ratios, G1 and G2, are not equal. An error trying to produce a shift in
the output common-mode is overridden by the common-mode control loop, where any feedback ratio mismatch
creates a balanced, differential error around the Vocm output.
The terms that create a differential error from a common-mode term and feedback ratio mismatch include the
desired Vocm voltage, any source common-mode voltage, any drift on the reference bias to the Vocm control
pin, and any internal offset and drift in the Vocm control path.
Considering just the output common-mode control and the source common-mode voltage (Vicm), the conversion
to output differential offsets is done by using Equation 4:
(4)
Neglecting any G1 and G2 mismatch because of standard values snap, the conversion gain for these two terms
can be recast in terms of the nominal Rf / Rg
≡ G, and tolerance T, as shown in Equation 5. As G increases, this
conversion gain approaches 4T, as a worst-case gain for these terms to output differential offset.
(5)



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