FEATURES
Pretrimmed to ⴞ1.0% (AD532K)
No External Components Required
Guaranteed ⴞ1.0% max 4-Quadrant Error (AD532K)
Diff Inputs for (X
– X2) (Y1 – Y2)/10 V Transfer Function
1
Monolithic Construction, Low Cost
APPLICATIONS
Multiplication, Division, Squaring, Square Rooting
Algebraic Computation
Power Measurements
Instrumentation Applications
Available in Chip Form
PRODUCT DESCRIPTION
The AD532 is the first pretrimmed single chip monolithic multiplier/divider. It guarantees a maximum multiplying error of
±1.0% and a ±10 V output voltage without the need for any
external trimming resistors or output op amp. Because the
AD532 is internally trimmed, its simplicity of use provides
design engineers with an attractive alternative to modular multipliers, and its monolithic construction provides significant advantages in size, reliability and economy. Further, the AD532
can be used as a direct replacement for other IC multipliers that
require external trim networks (such as the AD530).
FLEXIBILITY OF OPERATION
The AD532 multiplies in four quadrants with a transfer function of (X
a 10 V Z/(X
– X2)(Y1 – Y2)/10 V, divides in two quadrants with
1
– X2) transfer function, and square roots in one
1
quadrant with a transfer function of ±√10 V Z. In addition to
these basic functions, the differential X and Y inputs provide
significant operating flexibility both for algebraic computation and
transducer instrumentation applications. Transfer functions,
such as XY/10 V, (X
are easily attained and are extremely useful in many modulation
and function generation applications, as well as in trigonometric
calculations for airborne navigation and guidance applications,
where the monolithic construction and small size of the AD532
offer considerable system advantages. In addition, the high
CMRR (75 dB) of the differential inputs makes the AD532
especially well qualified for instrumentation applications, as it
can provide an output signal that is the product of two transducergenerated input signals.
REV. B
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.
2
2
– Y
)/10 V, ±X
2
/10 V and 10 V Z/(X1 – X2),
GUARANTEED PERFORMANCE OVER TEMPERATURE
The AD532J and AD532K are specified for maximum multi-
plying errors of ±2% and ±1% of full scale, respectively at
+25°C, and are rated for operation from 0°C to +70°C. The
AD532S has a maximum multiplying error of ±1% of full scale
at +25°C; it is also 100% tested to guarantee a maximum error
of ±4% at the extended operating temperature limits of –55°C
and +125°C. All devices are available in either the hermetically-
sealed TO-100 metal can, TO-116 ceramic DIP or LCC packages.
J, K and S grade chips are also available.
ADVANTAGES OF ON-THE-CHIP TRIMMING OF THE
MONOLITHIC AD532
1. True ratiometric trim for improved power supply rejection.
2. Reduced power requirements since no networks across supplies are required.
3. More reliable since standard monolithic assembly techniques
can be used rather than more complex hybrid approaches.
4. High impedance X and Y inputs with negligible circuit
loading.
5. Differential X and Y inputs for noise rejection and additional
computational flexibility.
Total Error (–10 V ≤ X, Y ≤ +10 V)±1.5ⴞ2.0±0.7ⴞ1.0±0.5ⴞ1.0%
T
= Min to Max±2.5±1.5ⴞ4.0%
A
Total Error vs. Temperature±0.04±0.03±0.01ⴞ0.04%/°C
(X1– X2)( Y1– Y2)
10V
(X1– X2)( Y1– Y2)
10V
(X1– X2)( Y1– Y2)
10V
Supply Rejection (±15 V ± 10%)±0.05±0.05±0.05%/%
Nonlinearity, X (X = 20 V pk-pk, Y = 10 V)±0.8±0.5±0.5%
Nonlinearity, Y (Y = 20 V pk-pk, X = 10 V)±0.3±0.2±0.2%
Feedthrough, X (Y Nulled,
X = 20 V pk-pk 50 Hz)502003010030100mV
Feedthrough, Y (X Nulled,
Y = 20 V pk-pk 50 Hz)3015025802580mV
Feedthrough vs. Temperature2.01.01.0mV p-p/°C
Feedthrough vs. Power Supply±0.25±0.25±0.25mV/%
DYNAMICS
Small Signal BW (V
1% Amplitude Error757575kHz
Slew Rate (V
Settling Time (to 2%, ∆V
OUT
= 0.1 rms)111MHz
OUT
20 pk-pk)454545V/µs
= 20 V)111µs
OUT
NOISE
Wideband Noise f = 5 Hz to 10 kHz0.60.60.6mV (rms)
Wideband Noise f = 5 Hz to 5 MHz3.03.03.0mV (rms)
OUTPUT
Output Voltage Swing±10±13±10±13±10±13V
Output Impedance (f ≤ 1 kHz)111Ω
Output Offset Voltage±40ⴞ30ⴞ30mV
Output Offset Voltage vs. Temperature0.70.72.0mV/°C
Output Offset Voltage vs. Supply±2.5±2.5±2.5mV/%
INPUT AMPLIFIERS (X, Y and Z)
Signal Voltage Range (Diff. or CM
Operating Diff)±10±10±10V
CMRR405050dB
Input Bias Current
X, Y Inputs31.541.54µA
X, Y Inputs T
Z Input±10±5ⴞ15±5ⴞ15µA
Z Input T
Offset Current±0.3±0.1±0.1µA
MIN
MIN
to T
to T
MAX
MAX
1088µA±30±25±25µA
Differential Resistance101010MΩ
DIVIDER PERFORMANCE
Transfer Function (Xl > X2) 10 V Z/(X1–X2) 10 V Z/(X1–X2) 10 V Z/(X1–X2)
Total Error
(V
= –10 V, –10 V ≤ VZ ≤ +10 V)±2±1±1%
X
(V
= –1 V, –10 V ≤ VZ ≤ +10 V)±4±3±3%
X
SQUARE PERFORMANCE
Transfer Function
Total Error±0.8±0.4±0.4%
(X1– X2)
10V
2
(X1– X2)
10V
2
(X1– X2)
2
10V
SQUARE ROOTER PERFORMANCE
Transfer Function–√10 V Z–√10 V Z–√10 V Z
Total Error (0 V ≤ VZ ≤ 10 V)±1.5±1.0±1.0%
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 are guaranteed, although only those shown
in boldface are tested on all production units.
AD532JD0°C to +70°CSide Brazed DIPD-14
AD532JD/+0°C to +70°CSide Brazed DIPD-14
AD532KD0°C to +70°CSide Brazed DIPD-14
AD532KD/+0°C to +70°CSide Brazed DIPD-14
AD532JH0°C to +70°CHeaderH-10A
AD532KH0°C to +70°CHeaderH-10A
AD532J Chip0°C to +70°CChip
AD532SD–55°C to +125°CSide Brazed DIPD-14
AD532SD/883B–55°C to +125°CSide Brazed DIPD-14
JM38510/13903BCA –55°C to +125°CSide Brazed DIPD-14
AD532SE/883B–55°C to +125°CLCCE-20A
AD532SH–55°C to +125°CHeaderH-10A
AD532SH/883B–55°C to +125°CHeaderH-10A
JM38510/13903BIA–55°C to +125°CHeaderH-10A
AD532S Chip–55°C to +125°CChip
FUNCTIONAL DESCRIPTION
The functional block diagram for the AD532 is shown in Figure
1, and the complete schematic in Figure 2. In the multiplying
and squaring modes, Z is connected to the output to close the
feedback around the output op amp. (In the divide mode, it is
used as an input terminal.)
The X and Y inputs are fed to high impedance differential amplifiers featuring low distortion and good common-mode rejection. The amplifier voltage offsets are actively laser trimmed
to zero during production. The product of the two inputs is
resolved in the multiplier cell using Gilbert’s linearized transconductance technique. The cell is laser trimmed to obtain
= (X1 – X2)(Y1 – Y2)/10 volts. The built-in op amp is used
V
OUT
to obtain low output impedance and make possible self-contained
operation. The residual output voltage offset can be zeroed at
in critical applications . . . otherwise the VOS pin should be
V
OS
grounded.
CHIP DIMENSIONS AND BONDING DIAGRAM
Contact factory for latest dimensions.
Dimensions shown in inches and (mm).
Figure 1. Functional Block Diagram
REV. B
Figure 2. Schematic Diagram
–3–
Page 4
AD532
AD532 PERFORMANCE CHARACTERISTICS
Multiplication accuracy is defined in terms of total error at
+25°C with the rated power supply. The value specified is in
percent of full scale and includes X
and YIN nonlinearities,
IN
feedback and scale factor error. To this must be added such
application-dependent error terms as power supply rejection,
common-mode rejection and temperature coefficients (although
worst case error over temperature is specified for the AD532S).
Total expected error is the rms sum of the individual components since they are uncorrelated.
Accuracy in the divide mode is only a little more complex. To
achieve division, the multiplier cell must be connected in the
feedback of the output op amp as shown in Figure 13. In this
configuration, the multiplier cell varies the closed loop gain of
the op amp in an inverse relationship to the denominator voltage. Thus, as the denominator is reduced, output offset, bandwidth and other multiplier cell errors are adversely affected. The
divide error and drift are then ⑀
× 10 V/X
m
– X2) where ⑀
1
m
represents multiplier full-scale error and drift, and (X1–X2) is
the absolute value of the denominator.
NONLINEARITY
Nonlinearity is easily measured in percent harmonic distortion.
The curves of Figures 3 and 4 characterize output distortion as
a function of input signal level and frequency respectively, with
one input held at plus or minus 10 V dc. In Figure 4 the sine
wave amplitude is 20 V (p-p).
AC FEEDTHROUGH
AC feedthrough is a measure of the multiplier’s zero suppression. With one input at zero, the multiplier output should be
zero regardless of the signal applied to the other input. Feedthrough as a function of frequency for the AD532 is shown in
Figure 5. It is measured for the condition V
(p-p) and V
= 0, VX = 20 V (p-p) over the given frequency
Y
= 0, VY = 20 V
X
range. It consists primarily of the second harmonic and is measured in millivolts peak-to-peak.
Figure 5. Feedthrough vs. Frequency
COMMON-MODE REJECTION
The AD532 features differential X and Y inputs to enhance its
flexibility as a computational multiplier/divider. Common-mode
rejection for both inputs as a function of frequency is shown in
Figure 6. It is measured with X
+10 V dc and Y
= Y2 = 20 V (p-p), (X1 – X2) = +10 V dc.
1
= X2 = 20 V (p-p), (Y1 – Y2) =
1
Figure 3. Percent Distortion vs. Input Signal
Figure 4. Percent Distortion vs. Frequency
–4–
Figure 6. CMRR vs. Frequency
Figure 7. Frequency Response, Multiplying
REV. B
Page 5
AD532
DYNAMIC CHARACTERISTICS
The closed loop frequency response of the AD532 in the multiplier mode typically exhibits a 3 dB bandwidth of 1 MHz and
rolls off at 6 dB/octave thereafter. Response through all inputs is
essentially the same as shown in Figure 7. In the divide mode,
the closed loop frequency response is a function of the absolute
value of the denominator voltage as shown in Figure 8.
Stable operation is maintained with capacitive loads to 1000 pF
in all modes, except the square root for which 50 pF is a safe
upper limit. Higher capacitive loads can be driven if a 100 Ω
resistor is connected in series with the output for isolation.
Figure 8. Frequency Response, Dividing
POWER SUPPLY CONSIDERATIONS
Although the AD532 is tested and specified with ±15 V dc
supplies, it may be operated at any supply voltage from ±10 V
to ±18 V for the J and K versions, and ±10 V to ±22 V for the S
version. The input and output signals must be reduced proportionately to prevent saturation; however, with supply voltages
below ±15 V, as shown in Figure 9. Since power supply sensitiv-
ity is not dependent on external null networks as in the AD530
and other conventionally nulled multipliers, the power supply
rejection ratios are improved from 3 to 40 times in the AD532.
NOISE CHARACTERISTICS
All AD532s are screened on a sampling basis to assure that
output noise will have no appreciable effect on accuracy. Typical spot noise vs. frequency is shown in Figure 10.
Figure 10. Spot Noise vs. Frequency
APPLICATIONS CONSIDERATIONS
The performance and ease of use of the AD532 is achieved
through the laser trimming of thin-film resistors deposited directly on the monolithic chip. This trimming-on-the-chip technique provides a number of significant advantages in terms of
cost, reliability and flexibility over conventional in-package
trimming of off-the-chip resistors mounted or deposited on a
hybrid substrate.
First and foremost, trimming on the chip eliminates the need
for a hybrid substrate and the additional bonding wires that are
required between the resistors and the multiplier chip. By trimming more appropriate resistors on the AD532 chip itself, the
second input terminals that were once committed to external
trimming networks (e.g., AD530) have been freed to allow fully
differential operation at both the X and Y inputs. Further, the
requirement for an input attenuator to adjust the gain at the Y
input has been eliminated, letting the user take full advantage of
the high input impedance properties of the input differential
amplifiers. Thus, the AD532 offers greater flexibility for both
algebraic computation and transducer instrumentation
applications.
Finally, provision for fine trimming the output voltage offset has
been included. This connection is optional, however, as the
AD532 has been factory-trimmed for total performance as
described in the listed specifications.
REV. B
Figure 9. Signal Swing vs. Supply
REPLACING OTHER IC MULTIPLIERS
Existing designs using IC multipliers that require external trimming networks (such as the AD530) can be simplified using the
pin-for-pin replaceability of the AD532 by merely grounding
, Y2 and VOS terminals. (The VOS terminal should always
the X
2
be grounded when unused.)
–5–
Page 6
AD532
Z
OUTAD532
V
OUT
V
OS
20kV
+V
S
–V
S
(OPTIONAL)
V
OUT
=
X
2
– Y
2
10V
X
1
X
2
Y
1
Y
2
–V
S
+V
S
20kV
10kV
AD741KH
20kV
–Y
X
Y
APPLICATIONS
MULTIPLICATION
single-ended positive inputs (0 V to +10 V), connect the input
and the offset null to X1. For optimum performance, gain
to X
2
(S.F.) and offset (X
) adjustments are recommended as shown
0
and explained in Table I.
+V
+V
V
OS
20kV
S
S
X
Y
V
OS
20kV
X
1
2
Y
1
2
–V
+V
+V
Z
S
–V
–V
S
20kV
S
OUTAD532
V
Z
OUTAD532
S
(OPTIONAL)
S
–V
(X0)
–V
OUT
Z
S
S
V
(X
1
=
V
OUT
OUTAD532
OUT
– X2) (Y1 – Y2)
10V
V
OUT
2
V
IN
V
=
OUT
10V
10VZ
=
X
V
OUT
1kV
(SF)
10kV
For practical reasons, the useful range in denominator input is
approximately 500 mV ≤ |(X
adjust (V
), if used, is trimmed with Z at zero and (X1 – X2) at
OS
– X
)| ≤ 10 V. The voltage offset
1
2
full scale.
Table I. Adjust Procedure (Divider or Square Rooter)
DIVIDERSQUARE ROOTER
AdjustAdjust
With:for:With:for:
AdjustXZV
OUT
ZV
OUT
Scale Factor–10 V +10 V–10 V+10 V–10 V
X0 (Offset)–1 V+0.1 V –1 V+0.1 V –1 V
Repeat if required.
SQUARE ROOT
2.2kV
Z
47kV
S
20kV
(X0)
Z
OUTAD532
–V
S
–V
S
X
1
X
2
Y
1
Y
+V
2
+V
S
10VZ
V
=
OUT
V
OUT
1kV
(SF)
10kV
Figure 14. Square Rooter Connection
The connections for square root mode are shown in Figure 14.
Similar to the divide mode, the multiplier cell is connected in
the feedback of the op amp by connecting the output back to
both the X and Y inputs. The diode D
to prevent latch-up as Z
adjustment is made with ZIN = +0.1 V dc, adjusting VOS to
V
OS
approaches 0 volts. In this case, the
IN
obtain –1.0 V dc in the output, V
performance, gain (S.F.) and offset (X
is connected as shown
1
= – √10 V Z. For optimum
OUT
) adjustments are recom-
0
mended as shown and explained in Table I.
DIFFERENCE OF SQUARES
X
1
X
2
Y
1
Y
2
(OPTIONAL)
+V
S
Figure 11. Multiplier Connection
For operation as a multiplier, the AD532 should be connected
as shown in Figure 11. The inputs can be fed differentially to
the X and Y inputs, or single-ended by simply grounding the
unused input. Connect the inputs according to the desired polarity in the output. The Z terminal is tied to the output to close
the feedback loop around the op amp (see Figure 1). The offset
adjust V
is optional and is adjusted when both inputs are zero
OS
volts to obtain zero out, or to buck out other system offsets.
SQUARE
X
1
X
2
Y
1
Y
2
V
IN
Figure 12. Squarer Connection
The squaring circuit in Figure 12 is a simple variation of the
multiplier. The differential input capability of the AD532, however, can be used to obtain a positive or negative output response to the input . . . a useful feature for control applications,
as it might eliminate the need for an additional inverter somewhere
else.
DIVISION
Z
X
2.2kV
47kV
Figure 13. Divider Connection
The AD532 can be configured as a two-quadrant divider by
connecting the multiplier cell in the feedback loop of the op
amp and using the Z terminal as a signal input, as shown in
Figure 13. It should be noted, however, that the output error is
given approximately by 10 V ⑀
/(X1 – X2), where ⑀m is the total
m
error specification for the multiply mode; and bandwidth by
× (X
f
m
Further, to avoid positive feedback, the X input is restricted to
negative values. Thus for single-ended negative inputs (0 V to
–10 V), connect the input to X and the offset null to X
– X2)/10 V, where fm is the bandwidth of the multiplier.
1
; for
2
–6–
Figure 15. Differential of Squares Connection
The differential input capability of the AD532 allows for the
algebraic solution of several interesting functions, such as the
difference of squares, X
– Y2/10 V. As shown in Figure 15, the
2
AD532 is configured in the square mode, with a simple unity
gain inverter connected between one of the signal inputs (Y)
and one of the inverting input terminals (–Y
) of the multiplier.
IN
The inverter should use precision (0.1%) resistors or be otherwise trimmed for unity gain for best accuracy.
REV. B
Page 7
TOP
VIEW
0.358 (9.09)
0.342 (8.69)
SQ
1
20
4
9
8
13
19
BOTTOM
VIEW
14
3
18
0.028 (0.71)
0.022 (0.56)
45° TYP
0.015 (0.38)
MIN
0.055 (1.40)
0.045 (1.14)
0.050 (1.27)
BSC
0.075 (1.91)
REF
0.011 (0.28)
0.007 (0.18)
R TYP
0.095 (2.41)
0.075 (1.90)
0.100 (2.54) BSC
0.200 (5.08)
BSC
0.150 (3.81)
BSC
0.075
(1.91)
REF
0.358
(9.09)
MAX
SQ
0.100 (2.54)
0.064 (1.63)
0.088 (2.24)
0.054 (1.37)
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
Side Brazed DIP
(D-14)
AD532
0.005 (0.13) MIN
0.200 (5.08)
MAX
0.200 (5.08)
0.125 (3.18)
14
1
PIN 1
0.785 (19.94) MAX
0.023 (0.58)
0.014 (0.36)
0.100
(2.54)
BSC
Leadless Chip Carrier
(E-20A)
0.098 (2.49) MAX
8
0.310 (7.87)
0.220 (5.59)
7
0.060 (1.52)
0.015 (0.38)
0.070 (1.78)
0.030 (0.76)
0.150
(3.81)
MAX
SEATING
PLANE
0.320 (8.13)
0.290 (7.37)
0.015 (0.38)
0.008 (0.20)
C136g–0–6/99
REV. B
0.335 (8.51)
0.305 (7.75)
0.370 (9.40)
0.335 (8.51)
0.040 (1.02) MAX
0.185 (4.70)
0.165 (4.19)
0.050
(1.27)
MAX
0.045 (1.14)
0.010 (0.25)
Metal Can
(H-10A)
REFERENCE PLANE
0.750 (19.05)
0.500 (12.70)
0.250 (6.35)
MIN
0.019 (0.48)
0.016 (0.41)
0.021 (0.53)
0.016 (0.41)
BASE & SEATING PLANE
–7–
0.230
(5.84)
BSC
6
57
4
39
2
10
0.115
(2.92)
BSC
1
0.034 (0.86)
0.027 (0.69)
36°
BSC
0.160 (4.06)
0.110 (2.79)
8
0.045 (1.14)
0.027 (0.69)
PRINTED IN U.S.A.
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