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THS3217 Datasheet, PDF (34/73 Pages) Texas Instruments – THS3217 DC to 800-MHz, Differential-to-Single-Ended, DAC Output Amplifier
THS3217
SBOS766B – FEBRUARY 2016 – REVISED FEBRUARY 2016
www.ti.com
Feature Description (continued)
The gain from VREF to VO1 is shown in Equation 6:
VREF
R1
§
¨1
R1 R2 ©
RF
·
¸
RG ¹
VO1
(6)
Getting both R1 and (R1 + R2) in terms of RG and the target attenuation, α simplifies, as shown in Equation 7:
R1
R1 R2
RG
1
1
D
D
RG
1
1
D
1D
(7)
Putting Equation 7 back into the gain expression(Equation 6), and expanding out gives:
VREF 1
D
§
¨1
©
RF
·
¸
RG ¹
VO1
(8)
Recall that in order to get differential gain balance, α = –(RF / RG). Putting that into Equation 8 reduces the
expression to VO1 = VREF, a gain of 1 V/V. This gain is very precise as shown in the D2S Electrical
Characteristics table, where the tested dc limits are 0.985 V/V to 1.015 V/V.
The D2S output offset and drift are largely determined by the internal elements. The only external consideration
is the dc source impedance at the two buffer inputs. With low source impedance, the D2S output offset is tested
to be within ±35 mV, that becomes a maximum ±17 mV input differential offset specification. Assuming the dc
source impedances are closely matched, the mismatch in the two input bias currents adds another input offset
term for higher source impedances. The input bias offset current is limited in test to be < ±0.40 µA. This error
term does not rise to add more than ±1 mV input differential offset until the dc source impedance exceeds 2.5
kΩ. A high dc source impedance most commonly occurs in an input ac-coupled, single-supply application, where
dc offsets are less critical.
The absolute input bias currents modifies the common-mode input voltage if the dc source resistance is too
large. That term is tested to a limit of ±4 µA on each input. To move the input common mode voltage by ±100
mV, the dc source impedance must exceed 25 kΩ. This added input common-mode voltage is cancelled by the
D2S at the output (VO1, pin6).
The D2S output noise is largely fixed by the internal elements. The D2S shows a differential input voltage noise
of 9 nV/√Hz, and a current noise of 2 pA/√Hz on each input. Higher termination resistors increase this source
noise, as given by Equation 9, where Rt is the dc termination impedance at each buffer input. The D2S has a 1/f
corner at approximately 30 kHz (see Figure 18).
ei _ diff
9nV 2 2 4kTRt 2 2pA u Rt 2
(9)
The total differential input noise is dominated by the differential voltage noise. For instance, evaluating this
expression for Rt = 200 Ω on each input, increases the total differential input noise to 9.4.nV/√Hz, only slightly
greater than the 9 nV/√Hz for the D2S with 0-Ω source Rt on each input. If higher final output SNR is desired,
consider generating as much input swing as the DAC can support, but increase the termination impedance. It is
possible that a lower tail current with higher Rt will yield improved SNR at the D2S input. This differential input
noise appears at the D2S output times a gain of 2 V/V.
eout _ diff 2 u ei _ diff
(10)
9.3.2 Midscale (DC) Reference Buffer (Pin 1 and Pin 15)
This optional block can be completely unconnected and not used if the design does not require this feature.
Internal 50-kΩ resistors to the power supplies bias the input of the buffer to the midpoint of the supplies used.
The internal resistors set a midsupply operating point when the buffer is not used, as well as a default midsupply
point at the buffer output to be used in other stages for single-supply, ac-coupled applications.
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