FEATURES
Two Channels with Independent Gain Control
“Linear in dB” Gain Response
Two Gain Ranges:
AD600: 0 dB to +40 dB
AD602: –10 dB to +30 dB
Accurate Absolute Gain: 60.3 dB
Low Input Noise: 1.4 nV/√
Low Distortion: –60 dBc THD at 61 V Output
High Bandwidth: DC to 35 MHz (–3 dB)
Stable Group Delay: 62 ns
Low Power: 125 mW (max) per Amplifier
Signal Gating Function for Each Amplifier
Drives High Speed A/D Converters
MIL-STD-883 Compliant and DESC Versions Available
APPLICATIONS
Ultrasound and Sonar Time-Gain Control
High Performance Audio and RF AGC Systems
Signal Measurement
PRODUCT DESCRIPTION
The AD600 and AD602 dual channel, low noise variable gain
amplifiers are optimized for use in ultrasound imaging systems,
but are applicable to any application requiring very precise gain,
low noise and distortion, and wide bandwidth. Each independent channel provides a gain of 0 dB to +40 dB in the AD600
and –10 dB to +30 dB in the AD602. The lower gain of the
AD602 results in an improved signal-to-noise ratio at the output. However, both products have the same 1.4 nV/√
noise spectral density. The decibel gain is directly proportional
to the control voltage, is accurately calibrated, and is supplyand temperature-stable.
To achieve the difficult performance objectives, a proprietary
circuit form—the X-AMP®—has been developed. Each channel
of the X-AMP comprises a variable attenuator of 0 dB to
–42.14 dB followed by a high speed fixed gain amplifier. In this
way, the amplifier never has to cope with large inputs, and can
benefit from the use of negative feedback to precisely define the
gain and dynamics. The attenuator is realized as a seven-stage
R-2R ladder network having an input resistance of 100 Ω, lasertrimmed to ±2%. The attenuation between tap points is 6.02 dB;
the gain-control circuit provides continuous interpolation between these taps. The resulting control function is linear in dB.
X-AMP is a registered trademark of Analog Devices, Inc.
*Patented.
REV. A
Information furnished by Analog Devices is believed to be accurate and
reliable. However, no responsibility is assumed by Analog Devices for its
use, nor for any infringements of patents or other rights of third parties
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.
Hz
Hz input
Variable Gain Amplifiers
AD600/AD602*
FUNCTIONAL BLOCK DIAGRAM
The gain-control interfaces are fully differential, providing an
input resistance of ~15 MΩ and a scale factor of 32 dB/V (that
is, 31.25 mV/dB) defined by an internal voltage reference. The
response time of this interface is less than 1 µs. Each channel
also has an independent gating facility that optionally blocks signal transmission and sets the dc output level to within a few millivolts of the output ground. The gating control input is TTL
and CMOS compatible.
The maximum gain of the AD600 is 41.07 dB, and that of the
AD602 is 31.07 dB; the –3 dB bandwidth of both models is
nominally 35 MHz, essentially independent of the gain. The
signal-to-noise ratio (SNR) for a 1 V rms output and a 1 MHz
noise bandwidth is typically 76 dB for the AD600 and 86 dB for
the AD602. The amplitude response is flat within ±0.5 dB from
100 kHz to 10 MHz; over this frequency range the group delay
varies by less than ±2 ns at all gain settings.
Each amplifier channel can drive 100 Ω load impedances with
low distortion. For example, the peak specified output is ±2.5 V
minimum into a 500 Ω load, or ± 1 V into a 100 Ω load. For a
200 Ω load in shunt with 5 pF, the total harmonic distortion for
a ±1 V sinusoidal output at 10 MHz is typically –60 dBc.
The AD600J and AD602J are specified for operation from 0°C
to +70°C, and are available in both 16-pin plastic DIP (N) and
16-pin SOIC (R). The AD600A and AD602A are specified for
operation from –40°C to +85°C and are available in both 16-pin
cerdip (Q) and 16-pin SOIC (R).
The AD600S and AD602S are specified for operation from
–55°C to +125°C and are available in a 16-pin cerdip (Q) package and are MIL-STD-883 compliant. The AD600S and
AD602S are also available under DESC SMD 5962-94572.
One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A.
Tel: 617/329-4700Fax: 617/326-8703
AD600/AD602–SPECIFICATIONS
(Each amplifier section, at TA = +258C, VS = 65 V, –625 mV ≤ VG ≤
+625 mV, RL = 500 V, and CL = 5 pF, unless otherwise noted. Specifications for AD600 and AD602 are identical unless otherwise noted.)
ParameterConditionsMinTypMaxMinTypMaxUnits
AD600J/AD602JAD600A/AD602A
INPUT CHARACTERISTICS
Input ResistancePins 2 to 3; Pins 6 to 79810010295100105Ω
Input Capacitance22pF
Input Noise Spectral Density
1
1.41.4nV/√Hz
Noise FigureRS = 50 Ω, Maximum Gain5.35.3dB
RS = 200 Ω, Maximum Gain22dB
Common-Mode Rejection Ratiof = 100 kHz3030dB
OUTPUT CHARACTERISTICS
–3 dB BandwidthV
Slew Rate275275V/µs
Peak Output
2
= 100 mV rms3535MHz
OUT
RL ≥ 500 Ω±2.5±3±2.5±3V
Output Impedancef ≤ 10 MHz22Ω
Output Short-Circuit Current5050mA
Group Delay Change vs. Gainf = 3 MHz; Full Gain Range±2±2ns
Group Delay Change vs. FrequencyVG = 0 V, f = 1 MHz to 10 MHz±2±2ns
Total Harmonic DistortionRL= 200 Ω, V
= ±1 V Peak, Rpd = 1 kΩ–60–60dBc
OUT
ACCURACY
AD600
Gain Error0 dB to 3 dB Gain0+0.5+1–0.5+0.5+0.5dB
3 dB to 37 dB Gain–0.5±0.2+0.5–0.1±0.2+1.0dB
37 dB to 40 dB Gain–1–0.50–1.5–0.5+0.5dB
Maximum Output Offset Voltage3VG = –625 mV to +625 mV10501065mV
Output Offset VariationVG = –625 mV to +625 mV10501065mV
AD602
Gain Error–10 dB to –7 dB Gain0+0.5+1–0.5+0.5+1.5dB
–7 dB to 27 dB Gain–0.5±0.2+0.5–0.1±0.2+1.0dB
27 dB to 30 dB Gain–1–0.50–1.5–0.5+0.5dB
Maximum Output Offset Voltage3VG = –625 mV to +625 mV5301045mV
Output Offset VariationVG = –625 mV to +625 mV5301045mV
GAIN CONTROL INTERFACE
Gain Scaling Factor3 dB to 37 dB (AD600); –7 dB to 27 dB (AD602)31.73232.330.53233.5dB/V
Common-Mode Range–0.752.5–0.752.5V
Input Bias Current0.3510.351µA
Input Offset Current10501050nA
Differential Input ResistancePins I to 16; Pins 8 to 9151550MΩ
Response RateFull 40 dB Gain Change4040dB/µs
SIGNAL GATING INTERFACE
Logic Input “LO” (Output ON)0.80.8V
Logic Input “HI” (Output OFF)2.42.4V
Response TimeON to OFF, OFF to ON0.30.3µs
Input ResistancePins 4 to 3 Pins 5 to 63030kΩ
Output Gated OFF
Typical open or short-circuited input; noise is lower when system is set to maximum gain and input is short-circuited. This figure includes the effects of both voltage
and current noise sources.
2
Using resistive loads of 500 Ω or greater, or with the addition of a 1 kΩ pull-down resistor when driving lower loads
3
The dc gain of the main amplifier in the AD600 is X113; thus an input offset of only 100 µV becomes an 11.3 mV output offset. In the AD602, the amplifier’s gain is
X35.7; thus, an input offset of 100 µV becomes a 3.57 mV output offset.
Specifications shown in boldface are tested on all production units at final electrical test Results from those tests are used to calculate outgoing quality levels. All min
and max specifications guaranteed, although only those shown in boldface are tested on all production units.
Specifications subject to change without notice.
Operating Temperature Range (J) . . . . . . . . . . . 0°C to +70°C
Operating Temperature Range (A) . . . . . . . . .–40°C to +85°C
Operating Temperature Range (S) . . . . . . . . .–55°C to +125°C
Storage Temperature Range . . . . . . . . . . . . .–65°C to +150°C
Lead Temperature Range (Soldering 60 sec) . . . . . . . . +300°C
NOTES
1
Stresses above those listed under “Absolute Maximum Ratings” may cause
permanent damage to the device. This is a stress rating only and functional
operation of the device at these or any other conditions above those indicated in the
operational section of this specification is not implied. Exposure to absolute
maximum rating conditions for extended periods may affect device reliability.
AD600AQ0 dB to +40 dB–40°C to +85°C Q-16
AD600AR0 dB to +40 dB–40° C to +85°C R-16
AD602AQ–10 dB to +30 dB–40°C to +85°C Q-16
AD602AR–10 dB to +30 dB–40°C to +85°C R-16
AD600JN0 dB to +40 dB0°C to +70°CN-16
AD600JR0 dB to +40 dB0°C to +70°CR-16
AD602JN–10 dB to +30 dB0°C to +70°CN-16
AD602JR–10 dB to +30 dB0°C to +70°CR-16
AD600SQ/883B
2
0 dB to +40 dB–55°C to +150°C Q-16
AD602SQ/883B3–10 dB to +30 dB–55°C to +150°C Q-16
NOTES
1
N = Plastic DIP; Q= Cerdip; R= Small Outline IC (SOIC).
2
Refer to AD600/AD602 Military data sheet. Also available as 5962-9457201MPA.
3
Refer to AD600/AD602 Military data sheet. Also available as 5962-9457202MPA.
PIN DESCRIPTION
PinFunction Description
Pin 1C1LOCH1 Gain-Control Input “LO” (Positive
Voltage Reduces CH1 Gain).
Pin 2A1HICH1 Signal Input “HI” (Positive Voltage
Increases CH1 Output).
Pin 3A1LOCH1 Signal Input “LO” (Usually Taken to
CH1 Input Ground)
Pin 4GAT1CH1 Gating Input (A Logic “HI” Shuts Off
CH1 Signal Path).
Pin 5GAT2CH2 Gating Input (A Logic “HI” Shuts Off
CH2 Signal Path).
Pin 6A2LOCH2 Signal Input “LO” (Usually Taken to
CH2 Input Ground).
Pin 7A2HICH2 Signal Input “HI” (Positive Voltage
Increases CH2 Output).
Pin 8C2LOCH2 Gain-Control Input “LO” (Positive
Voltage Reduces CH2 Gain).
Pin 9C2HICH2 Gain-Control Input “HI” (Positive
Voltage Increases CH2 Gain).
Pin 10 A2CMCH2 Common (Usually Taken to CH2
Output Ground).
Pin 11 A2OPCH2 Output.
Pin 12 VNEGNegative Supply for Both Amplifiers.
Pin 13 VPOSPositive Supply for Both Amplifiers.
Pin 14 A1OPCH1 Output.
Pin 15 A1CMCH1 Common (Usually Taken to CH1
ESD (electrostatic discharge) sensitive device. Permanent damage may occur on unconnected
devices subject to high energy electrostatic fields. Unused devices must be stored in conductive
foam or shunts. The protective foam should be discharged to the destination socket before
devices are removed.
REV. A
AD600/AD602
THEORY OF OPERATION
The AD600 and AD602 have the same general design and features. They comprise two fixed gain amplifiers, each preceded
by a voltage-controlled attenuator of 0 dB to 42.14 dB with independent control interfaces, each having a scaling factor of
32 dB per volt. The gain of each amplifier in the AD600 is laser
trimmed to 41.07 dB (X113), thus providing a control range of
–1.07 dB to 41.07 dB (0 dB to 40 dB with overlap), while the
AD602 amplifiers have a gain of 31.07 dB (X35.8) and provide
an overall gain of –11.07 dB to 31.07 dB (–10 dB to 30 dB with
overlap).
The advantage of this topology is that the amplifier can use
negative feedback to increase the accuracy of its gain; also, since
the amplifier never has to handle large signals at its input, the
distortion can be very low. A further feature of this approach is
that the small-signal gain and phase response, and thus the
pulse response, are essentially independent of gain.
The following discussion describes the AD600. Figure 1 is a
simplified schematic of one channel. The input attenuator is a
seven-section R-2R ladder network, using untrimmed resistors
of nominally R = 62.5 Ω, which results in a characteristic resistance of 125 Ω± 20%. A shunt resistor is included at the input
and laser trimmed to establish a more exact input resistance of
100 Ω± 2%, which ensures accurate operation (gain and HP
corner frequency) when used in conjunction with external resistors or capacitors.
Figure 1. Simplified Block Diagram of Single Channel of
the AD600 and AD602
The nominal maximum signal at input A1HI is 1 V rms (±1.4 V
peak) when using the recommended ± 5 V supplies, although
operation to ±2 V peak is permissible with some increase in HF
distortion and feedthrough. Each attenuator is provided with a
separate signal “LO” connection, for use in rejecting commonmode, the voltage between input and output grounds. Circuitry
is included to provide rejection of up to ±100 mV.
The signal applied at the input of the ladder network is attenuated by 6.02 dB by each section; thus, the attenuation to each of
the taps is progressively 0, 6.02, 12.04, 18.06, 24.08, 30.1, 36.12
and 42.14 dB. A unique circuit technique is employed to interpolate between these tap points, indicated by the “slider” in Figure 1, providing continuous attenuation from 0 dB to 42.14 dB.
It will help, in understanding the AD600, to think in terms of a
mechanical means for moving this slider from left to right; in
fact, it is voltage controlled. The details of the control interface
are discussed later. Note that the gain is at all times exactly determined, and a linear decibel relationship is automatically guaranteed between the gain and the control parameter which
determines the position of the slider. In practice, the gain deviates from the ideal law, by about ±0.2 dB peak (see, for example, Figure 6).
Note that the signal inputs are not fully differential: A1LO and
A1CM (for CH1) and A2LO and A2CM (for CH2) provide
separate access to the input and output grounds. This recognizes the practical fact that even when using a ground plane,
small differences will arise in the voltages at these nodes. It is
important that A1LO and A2LO be connected directly to the
input ground(s); significant impedance in these connections will
reduce the gain accuracy. A1CM and A2CM should be connected to the load ground(s).
Noise Performance
An important reason for using this approach is the superior
noise performance that can be achieved. The nominal resistance
seen at the inner tap points of the attenuator is 41.7 Ω (one
third of 125 Ω), which exhibits a Johnson noise spectral density
(NSD) of 0.84 nV/√
Hz (that is, √4kTR) at 27°C, which is a
large fraction of the total input noise. The first stage of the amplifier contributes a further 1.12 nV/√
of 1.4 nV/√
Hz.
Hz, for a total input noise
The noise at the 0 dB tap depends on whether the input is
short-circuited or open-circuited: when shorted, the minimum
NSD of 1.12 nV/√
100 Ω at the first tap generates 1.29 nV/√
creases to a total of 1.71 nV/√
Hz is achieved; when open, the resistance of
Hz, so the noise in-
Hz. (This last calculation would
be important if the AD600 were preceded, for example, by a
900 Ω resistor to allow operation from inputs up to ± 10 V rms.
However, in most cases the low impedance of the source will
limit the maximum noise resistance.)
It will be apparent from the foregoing that it is essential to use a
low resistance in the design of the ladder network to achieve low
noise. In some applications this may be inconvenient, requiring
the use of an external buffer or preamplifier. However, very few
amplifiers combine the needed low noise with low distortion at
maximum input levels, and the power consumption needed to
achieve this performance is fundamentally required to be quite
high (due to the need to maintain very low resistance values
while also coping with large inputs). On the other hand, there is
little value in providing a buffer with high input impedance,
since the usual reason for this—the minimization of loading of a
high resistance source—is not compatible with low noise.
Apart from the small variations just discussed, the signal-tonoise (S/ N) ratio at the output is essentially independent of the
attenuator setting, since the maximum undistorted output is 1 V
rms and the NSD at the output of the AD600 is fixed at 113
times 1.4 nV/√
Hz, or 158 nV/√Hz. Thus, in a 1 MHz band-
width, the output S/N ratio would be 76 dB. The input NSD of
the AD600 and AD602 are the same, but because of the 10 dB
lower gain in the AD602’s fixed amplifier, its output S/N ratio is
10 dB better, or 86 dB in a 1 MHz bandwidth.
–4–
REV. A
AD600/AD602
The Gain-Control Interface
The attenuation is controlled through a differential, high impedance (15 MΩ) input, with a scaling factor which is laser
trimmed to 32 dB per volt, that is, 31.25 mV/dB. Each of the
two amplifiers has its own control interface. An internal bandgap reference ensures stability of the scaling with respect to
supply and temperature variations, and is the only circuitry
common to both channels.
When the differential input voltage V
= 0 V, the attenuator
G
“slider” is centered, providing an attenuation of 21.07 dB, thus
resulting in an overall gain of 20 dB (= –21.07 dB + 41.07 dB).
When the control input is –625 mV, the gain is lowered by
20 dB (= 0.625 × 32), to 0 dB; when set to +625 mV, the gain
is increased by 20 dB, to 40 dB. When this interface is overdriven in either direction, the gain approaches either –1.07 dB
(= –42.14 dB + 41.07 dB) or 41.07 dB (= 0 + 41.07 dB),
respectively.
The gain of the AD600 can thus be calculated using the following simple expression:
Gain (dB) = 32 V
where V
is in volts. For the AD602, the expression is:
G
Gain (dB) = 32 V
Operation is specified for V
+ 20 (1)
G
+ 10 (2)
G
in the range from –625 mV dc to
G
+625 mV dc. The high impedance gain-control input ensures
minimal loading when driving many amplifiers in multiplechannel applications. The differential input configuration provides flexibility in choosing the appropriate signal levels and
polarities for various control schemes.
For example, the gain-control input can be fed differentially to
the inputs, or single-ended by simply grounding the unused input. In another example, if the gain is to be controlled by a
DAC providing a positive only ground referenced output, the
“Gain Control LO” pin (either C1LO or C2LO) should be biased to a fixed offset of +625 mV, to set the gain to 0 dB when
“Gain Control HI” (C1HI or C2HI) is at zero, and to 40 dB
when at +1.25 V.
It is a simple matter to include a voltage divider to achieve other
scaling factors. When using an 8-bit DAC having a FS output of
+2.55 V (10 mV/bit) a divider ratio of 1.6 (generating 6.25 mV/
bit) would result in a gain setting resolution of 0.2 dB/ bit.
Later, we will discuss how the two sections of an AD600 or
AD602 may be cascaded, when various options exist for gain
control.
Signal-Gating Inputs
Each amplifier section of the AD600 and AD602 is equipped
with a signal gating function, controlled by a TTL or CMOS
logic input (GAT1 or GAT2). The ground references for these
inputs are the signal input grounds A1LO and A2LO, respectively. Operation of the channel is unaffected when this input is
LO or left open-circuited. Signal transmission is blocked when
this input is HI. The dc output level of the channel is set to
within a few millivolts of the output ground (A1CM or A2CM),
and simultaneously the noise level drops significantly. The
reduction in noise and spurious signal feedthrough is useful in
ultrasound beam-forming applications, where many amplifier
outputs are summed.
Common-Mode Rejection
A special circuit technique is used to provide rejection of voltages appearing between input grounds (A1LO and A2LO) and
output grounds (A1CM and A2CM). This is necessary because
of the “op amp” form of the amplifier, as shown in Figure 1.
The feedback voltage is developed across the resistor RF1
(which, to achieve low noise, has a value of only 20 Ω). The
voltage developed across this resistor is referenced to the input
common, so the output voltage is also referred to that node.
To provide rejection of this common voltage, an auxiliary amplifier (not shown) is included, which senses the voltage difference
between input and output commons and cancels this error
component. Thus, for zero differential signal input between
A1HI and A1LO, the output A1OP simply follows the voltage at
A1CM. Note that the range of voltage differences which can exist between A1LO and A1CM (or A2LO and A2CM) is limited
to about ±100 mV. Figure 50 (one of the typical performance
curves at the end of this data sheet) shows typical commonmode rejection ratio versus frequency.
ACHIEVING 80 dB GAIN RANGE
The two amplifier sections of the X-AMP can be connected in
series to achieve higher gain. In this mode, the output of A1
(A1OP and A1CM) drives the input of A2 via a high-pass
network (usually just a capacitor) that rejects the dc offset. The
nominal gain range is now –2 dB to +82 dB for the AD600 or
–22 dB to +62 dB for the AD602.
There are several options in connecting the gain-control inputs.
The choice depends on the desired signal-to-noise ratio (SNR)
and gain error (output ripple). The following examples feature
the AD600; the arguments generally apply to the AD602, with
appropriate changes to the gain values.
Sequential Mode (Maximum S/N Ratio)
In the sequential mode of operation, the SNR is maintained at
its highest level for as much of the gain control range possible,
as shown in Figure 2. Note here that the gain range is 0 dB to
80 dB. Figure 3 shows the general connections to accomplish
this. Both gain-control inputs, C1HI and C2HI, are driven in
parallel by a positive only, ground referenced source with a
range of 0 V to +2.5 V.
85
80
75
70
65
60
55
50
S/N RATIO – dB
45
40
35
30
–0.5
0.0
V
G
3.0
2.52.01.51.00.5
Figure 2. S/N Ratio vs. Control Voltage Sequential Control
(1 MHz Bandwidth)
REV. A
–5–
AD600/AD602
A1A2
–40.00dB
–41.07dB
INPUT
0dB
V = 0V
C
INPUT
0dB
V = 1.25V
C
INPUT
0dB
V = 25V
C
–40.00dB
C1HIC1LO
V
G1
V = 0.592V
O1
–0.51dB
C1HIC1LO
V
G1
V = 0.592V
O1
0dB
C1HIC1LO
V
G1
V = 0.592V
O1
41.07dB
41.07dB
41.07dB
1.07dB
(a)
40.56dB
(b)
41.07dB
(c)
Figure 3. AD600 Gain Control Input Calculations for Sequential Control Operation
The gains are offset (Figure 4) such that A2’s gain is increased
only after A1’s gain has reached its maximum value. Note that
for a differential input of –700 mV or less, the gain of a single
amplifier (A1 or A2) will be at its minimum value of –1.07 dB;
for a differential input of +700 mV or more, the gain will be at
its maximum value of 41.07 dB. Control inputs beyond these
limits will not affect the gain and can be tolerated without damage or foldover in the response. See the Specifications Section of
this data sheet for more details on the allowable voltage range.
The gain is now
where V
Gain (dB) = 32 V
is the applied control voltage.
C
+41.07dB
A1A2
20dB
C
40.56dB+38.93dB
*
(3)
*
+1.07dB
GAIN
(dB)
00.6251.251.875
020406080–2.1482.14
Figure 4. Explanation of Offset Calibration for Sequential
Control
–0.56dB
0.5921.908
*GAIN OFFSET OF 1.07dB, OR 33.44mV
2.5
V (V)
C
–1.07dB
–42.14dB
C1HIC1LO
V
G2
V = 1.908V
O2
–1.07dB–0.51dB
–41.63dB
C1HIC1LO
V
G2
V = 1.908V
O2
38.93dB0dB
–2.14dB
C1HIC1LO
V
G2
V = 1.908V
O2
41.07dB
41.07dB
41.07dB
OUTPUT
0dB
OUTPUT
40dB
OUTPUT
80dB
When VC is set to zero, VG1 = –0.592 V and the gain of A1 is
+1.07 dB (recall that the gain of each amplifier section is 0 dB
for V
= 625 mV); meanwhile, VG2 = –1.908 V so the gain of
G
A2 is –1.07 dB. The overall gain is thus 0 dB (see Figure 3a).
When V
sets the gain of A1 to 40.56 dB, while V
= +1.25 V, VG1 = 1.25 V– 0.592 V = +0.658 V, which
C
= 1.25 V – 1.908 V =
G2
–0.658 V, which sets A2’s gain at –0.56 dB. The overall gain is
now 40 dB (see Figure 3b). When V
= +2.5 V, the gain of A1
C
is 41.07 dB and that of A2 is 38.93 dB, resulting in an overall
gain of 80 dB (see Figure 3c). This mode of operation is further
clarified by Figure 5, which is a plot of the separate gains of A1
and A2 and the overall gain versus the control voltage. Figure 6
is a plot of the gain error of the cascaded amplifiers versus the
control voltage.
Parallel Mode (Simplest Gain-Control Interface)
In this mode, the gain-control voltage is applied to both inputs
in parallel—C1HI and C2HI are connected to the control voltage, and C1LO and C2LO are optionally connected to an offset
voltage of +0.625 V. The gain scaling is then doubled to 64 dB/
V, requiring only 1.25 V for an 80 dB change of gain. The amplitude of the gain ripple in this case is also doubled, as shown
in Figure 7, and the instantaneous signal-to-noise ratio at the
output of A2 decreases linearly as the gain is increased (Figure 8).
Low Ripple Mode (Minimum Gain Error)
As can be seen in Figures 6 and 7, the output ripple is periodic.
By offsetting the gains of Al and A2 by half the period of the
ripple, or 3 dB, the residual gain errors of the two amplifiers
can be made to cancel. Figure 9 shows the much lower gain rip
ple when configured in this manner. Figure 10 plots the S/N
ratio as a function of gain; it is very similar to that in the “Parallel Mode.”
–6–
REV. A
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