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ADA4938-2ACPZ-R2 数据表(PDF) 19 Page - Analog Devices

部件名 ADA4938-2ACPZ-R2
功能描述  Ultralow Distortion Differential ADC Driver
PDF  26 Pages
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制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

ADA4938-2ACPZ-R2 数据表(HTML) 19 Page - Analog Devices

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Data Sheet
ADA4938-1/ADA4938-2
Rev. B | Page 19 of 26
THEORY OF OPERATION
The ADA4938-1/ADA4938-2 differ from conventional op amps
in that they have two outputs whose voltages move in opposite
directions. Like an op amp, it relies on open-loop gain and
negative feedback to force these outputs to the desired voltages.
The ADA4938-1/ADA4938-2 behave much like a standard
voltage feedback op amp and makes it easier to perform single-
ended-to-differential conversions, common-mode level shifting,
and amplifications of differential signals. Also like an op amp,
the ADA4938-1/ADA4938-2 have high input impedance and
low output impedance.
Two feedback loops are employed to control the differential and
common-mode output voltages. The differential feedback, set
with external resistors, controls only the differential output
voltage. The common-mode feedback controls only the common-
mode output voltage. This architecture makes it easy to set the
output common-mode level to any arbitrary value. It is forced,
by internal common-mode feedback, to be equal to the voltage
applied to the VOCM input, without affecting the differential
output voltage.
The ADA4938-1/ADA4938-2 architecture results in outputs
that are highly balanced over a wide frequency range without
requiring tightly matched external components. The common-
mode feedback loop forces the signal component of the output
common-mode voltage to zero, which results in nearly perfectly
balanced differential outputs that are identical in amplitude and
are exactly 180° apart in phase.
ANALYZING AN APPLICATION CIRCUIT
The ADA4938-1/ADA4938-2 use open-loop gain and negative
feedback to force its differential and common-mode output
voltages in such a way as to minimize the differential and
common-mode error voltages. The differential error voltage is
defined as the voltage between the differential inputs labeled
+IN and −IN (see Figure 57). For most purposes, this voltage
can be assumed to be zero. Similarly, the difference between the
actual output common-mode voltage and the voltage applied to
VOCM can also be assumed to be zero. Starting from these two
assumptions, any application circuit can be analyzed.
SETTING THE CLOSED-LOOP GAIN
The differential-mode gain of the circuit in Figure 57 can be
determined by
G
F
dm
IN
dm
OUT
R
R
V
V
=
,
,
This assumes the input resistors (RG) and feedback resistors (RF)
on each side are equal.
ESTIMATING THE OUTPUT NOISE VOLTAGE
The differential output noise of the ADA4938-1/ADA4938-2
can be estimated using the noise model in Figure 58. The input-
referred noise voltage density, vnIN, is modeled as a differential
input, and the noise currents, inIN− and inIN+, appear between
each input and ground. The noise currents are assumed to be
equal and produce a voltage across the parallel combination of
the gain and feedback resistances. vn,cm is the noise voltage
density at the VOCM pin. Each of the four resistors contributes
(4kTR)1/2. Table 9 summarizes the input noise sources, the
multiplication factors, and the output-referred noise density terms.
ADA4938
+
RF2
VnOD
VnCM
VOCM
VnIN
RF1
RG2
RG1
VnRF1
VnRF2
VnRG1
VnRG2
inIN+
inIN–
Figure 58. ADA4938-1/ADA4938-2 Noise Model
Table 9. Output Noise Voltage Density Calculations
Input Noise Contribution
Input Noise Term
Input Noise
Voltage Density
Output
Multiplication Factor
Output Noise
Voltage Density Term
Differential Input
vnIN
vnIN
GN
vnO1 = GN(vnIN)
Inverting Input
inIN−
inIN− × (RG2||RF2)
GN
vnO2 = GN[inIN− × (RG2||RF2)]
Noninverting Input
inIN+
inIN+ × (RG1||RF1)
GN
vnO3 = GN[inIN+ × (RG1||RF1)]
VOCM Input
vn, cm
vn, cm
GN(β1 − β2)
vnO4 = GN(β1 − β2)(vnCM)
Gain Resistor, RG1
vnRG1
(4kTRG1)1/2
GN(1 − β1)
vnO5 = GN(1 − β1)(4kTRG1)1/2
Gain Resistor, RG2
vnRG2
(4kTRG2)1/2
GN(1 − β2)
vnO6 = GN(1 − β2)(4kTRG2)1/2
Feedback Resistor, RF1
vnRF1
(4kTRF1)1/2
1
vnO7 = (4kTRF1)1/2
Feedback Resistor, RF2
vnRF2
(4kTRF2)1/2
1
vnO8 = (4kTRF2)1/2



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