Low Cost, Low Power, True RMS-to-DC Converter AD736

Transcription

1 Low Cost, Low Power, True RMS-to-Donverter FEATURES Computes True rms value Average rectified value Absolute value Provides 00 mv full-scale input range (larger inputs with input attenuator) High input impedance: 0 Ω Low input bias current: pa maximum High accuracy: ±0.3 mv ± 0.3% of reading RMS conversion with signal crest factors up to Wide power supply range:. V, 3. V to ±. V Low power: 00 ma maximum supply current Buffered voltage output No external trims needed for specified accuracy AD737 an unbuffered voltage output version with chip power-down also available GENERAL DESCRIPTION The is a low power, precision, monolithic true rms-todc converter. It is laser trimmed to provide a maximum error of ±0.3 mv ± 0.3% of reading with sine wave inputs. Furthermore, it maintains high accuracy while measuring a wide range of input waveforms, including variable duty-cycle pulses and triac (phase)-controlled sine waves. The low cost and small size of this converter make it suitable for upgrading the performance of non-rms precision rectifiers in many applications. Compared to these circuits, the offers higher accuracy at an equal or lower cost. The can compute the rms value of both ac and dc input voltages. It can also be operated as an ac-coupled device by adding one external capacitor. In this mode, the can resolve input signal levels of 00 μv rms or less, despite variations in temperature or supply voltage. High accuracy is also maintained for input waveforms with crest factors of to 3. In addition, crest factors as high as can be measured (introducing only.% additional error) at the 00 mv full-scale input level. The has its own output buffer amplifier, thereby providing a great deal of design flexibility. Requiring only 00 μa of power supply current, the is optimized for use in portable multimeters and other battery-powered applications. 3 FUNCTIONAL BLOCK DIAGRAM FULL WAVE RECTIFIER INPUT BIAS SECTION rms CORE Figure. COM 7 V S The allows the choice of two signal input terminals: a high impedance FET input (0 Ω) that directly interfaces with High-Z input attenuators and a low impedance input ( kω) that allows the measurement of 300 mv input levels while operating from the minimum power supply voltage of. V, 3. V. The two inputs can be used either single ended or differentially. The has a % reading error bandwidth that exceeds 0 khz for the input amplitudes from 0 mv rms to 00 mv rms while consuming only mw. The is available in four performance grades. The J and K grades are rated over the 0 C to 70 C and 0 C to C commercial temperature ranges. The A and B grades are rated over the 0 C to C industrial temperature range. The is available in three low cost, -lead packages: PDIP, SOIC, and CERDIP. PRODUCT HIGHLIGHTS. The is capable of computing the average rectified value, absolute value, or true rms value of various input signals.. Only one external component, an averaging capacitor, is required for the to perform true rms measurement. 3. The low power consumption of mw makes the suitable for many battery-powered applications.. A high input impedance of 0 Ω eliminates the need for an external buffer when interfacing with input attenuators.. A low impedance input is available for those applications that require an input signal up to 300 mv rms operating from low power supply voltages Rev. H 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 that may result from its use. Specifications subject to change without notice. No license is granted by implication or otherwise under any patent or patent rights of Analog Devices. Trademarks and registered trademarks are the property of their respective owners. One Technology Way, P.O. Box 90, Norwood, MA 00-90, U.S.A. Tel: Fax: Analog Devices, Inc. All rights reserved.

2 TABLE OF CONTENTS Features... General Description... Functional Block Diagram... Product Highlights... Revision History... Specifications... 3 Absolute Maximum Ratings... ESD Caution... Pin Configuration and Function Descriptions... Typical Performance Characteristics... 7 Theory of Operation... 0 Types of AC Measurement... 0 Calculating Settling Time Using Figure... RMS Measurement Choosing the Optimum Value for CAV... Rapid Settling Times via the Average Responding Connection... DC Error, Output Ripple, and Averaging Error... AC Measurement Accuracy and Crest Factor... Applications... 3 Connecting the Input... 3 Selecting Practical Values for Input Coupling (CC), Averaging (CAV), and Filtering (CF) Capacitors... Evaluation Board... Outline Dimensions... Ordering Guide... 9 REVISION HISTORY /07 Rev. G to Rev. H Updated Layout...9 to Added Applications Section... 3 Inserted Figure to Figure ; Renumbered Sequentially... 3 Deleted Figure... Added Evaluation Board Section... Inserted Figure 9 to Figure 3; Renumbered Sequentially... Inserted Figure 3; Renumbered Sequentially... 7 Added Table... 7 /0 Rev. F to Rev. G Updated Format...Universal Changes to Features... Added Table 3... Changes to Figure and Figure... Changes to Figure 3, Figure, and Figure... Updated Outline Dimensions... Changes to Ordering Guide... 7 /03 Rev. D to Rev. E Changes to General Description... Changes to Specifications...3 Changes to Absolute Maximum Ratings... Changes to Ordering Guide... /0 Rev. C to Rev. D Changes to Functional Block Diagram... Changes to Pin Configuration...3 Figure Replaced... Changes to Figure... Changes to Application Circuits Figures to... Outline Dimensions Updated... /0 Rev. E to Rev. F Changes to Specifications... Replaced Figure... 0 Updated Outline Dimensions... Changes to Ordering Guide... Rev. H Page of 0

3 SPECIFICATIONS At C ± V supplies, ac-coupled with khz sine wave input applied, unless otherwise noted. Specifications in bold are tested on all production units at final electrical test. Results from those tests are used to calculate outgoing quality levels. Table. J/A K/B Parameter Conditions Min Typ Max Min Typ Max Unit TRANSFER FUNCTION VOUT = Avg (VIN ) CONVERSION ACCURACY khz sine wave Total Error, Internal Trim Using CC All Grades 0 mv rms to 00 mv rms 0.3/0.3 0./0. 0./0. 0.3/0.3 ±mv/±% of reading 00 mv to V rms. ±.0. ±.0 % of reading TMIN to TMAX A and B 00 mv rms 0.7/0.7 0./0. ±mv/±% of reading J and K 00 mv rms ±% of reading/ C vs. Supply 00 mv rms Input VS = ± V to ±. V %/V VS = ± V to ±3 V %/V DC Reversal Error, 00 mv dc % of reading Nonlinearity, 0 mv to mv rms % of reading Total Error, External Trim 0 mv rms to 00 mv rms 0./0. 0./0.3 ±mv/±% of reading ERROR VS. CREST FACTOR 3 Crest Factor = to 3 CAV, CF = 00 μf % additional error Crest Factor = CAV, CF = 00 μf.. % additional error INPUT CHARACTERISTICS High Impedance Input Signal Range (Pin ) Continuous RMS Level VS =. V, 3. V mv rms VS = ± V to ±. V V rms Peak Transient Input VS =. V, 3. V ±0.9 ±0.9 V VS = ± V ±.7 ±.7 V VS = ±. V ±.0 ±.0 V Input Resistance 0 0 Ω Input Bias Current VS = ±3 V to ±. V pa Low Impedance Input Signal Range (Pin ) Continuous RMS Level VS =. V, 3. V mv rms VS = ± V to ±. V V rms Peak Transient Input VS =. V, 3. V ±.7 ±.7 V VS = ± V ±3. ±3. V VS = ±. V ± ± V Input Resistance kω Maximum Continuous All supply voltages ± ± V p-p Nondestructive Input Input Offset Voltage J and K Grades ±3 ±3 mv A and B Grades ±3 ±3 mv vs. Temperature μv/ C vs. Supply VS = ± V to ±. V μv/v VS = ± V to ±3 V 0 0 μv/v Rev. H Page 3 of 0

4 J/A K/B Parameter Conditions Min Typ Max Min Typ Max Unit CHARACTERISTICS Output Offset Voltage J and K Grades ±0. ±0. ±0. ±0.3 mv A and B Grades ±0. ±0.3 mv vs. Temperature 0 0 μv/ C vs. Supply VS = ± V to ±. V μv/v VS = ± V to ±3 V 0 0 μv/v Output Voltage Swing kω Load VS =. V, 3. V 0 to.7 0 to.7 V.. VS = ± V 0 to 3. 0 to 3. V VS = ±. V 0 to 0 to V No Load VS = ±. V 0 to 0 to V Output Current ma Short-Circuit Current 3 3 ma Output dc Ω FREQUENCY RESPONSE High Impedance Input (Pin ) Sine wave input for % Additional Error VIN = mv rms khz VIN = 0 mv rms khz VIN = 00 mv rms khz VIN = 00 mv rms khz ±3 db Bandwidth Sine wave input VIN = mv rms khz VIN = 0 mv rms khz VIN = 00 mv rms khz VIN = 00 mv rms khz Low Impedance Input (Pin ) Sine wave input for % Additional Error VIN = mv rms khz VIN = 0 mv rms khz VIN = 00 mv rms khz VIN = 00 mv rms khz ±3 db Bandwidth Sine wave input VIN = mv rms khz VIN = 0 mv rms khz VIN = 00 mv rms khz VIN = 00 mv rms 0 0 khz POWER SUPPLY Operating Voltage Range., 3. ± ±.., 3. ± ±. V Quiescent Current Zero signal μa 00 mv rms, No Load Sine wave input μa TEMPERATURE RANGE Operating, Rated Performance Commercial 0 C to 70 C JN, JR KN, KR Industrial 0 C to C AQ, AR BQ, BR Accuracy is specified with the connected as shown in Figure with Capacitor CC. Nonlinearity is defined as the maximum deviation (in percent error) from a straight line connecting the readings at 0 mv rms and 00 mv rms. Output offset voltage is adjusted to zero. 3 Error vs. crest factor is specified as additional error for a 00 mv rms signal. Crest factor = VPEAK/V rms. DC offset does not limit ac resolution. Rev. H Page of 0

5 ABSOLUTE MAXIMUM RATINGS Table. Parameter Rating Supply Voltage ±. V Internal Power Dissipation 00 mw Input Voltage ±VS Output Short-Circuit Duration Indefinite Differential Input Voltage VS and VS Storage Temperature Range (Q) C to 0 C Storage Temperature Range (N, R) C to C Lead Temperature (Soldering, 0 sec) 300 C ESD Rating 00 V Stresses above those listed under Absolute Maximum Ratings may cause permanent damage to the device. This is a stress rating only; 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. ESD CAUTION -Lead PDIP: θja = C/W, -Lead CERDIP: θja = 0 C/W, and -Lead SOIC: θja = C/W. Rev. H Page of 0

6 PIN CONFIGURATION AND FUNCTION DESCRIPTIONS 3 TOP VIEW (Not to Scale) 7 COM V S Figure. Pin Configuration Table 3. Pin Function Descriptions Pin No. Mnemonic Description Coupling Capacitor. If dc coupling is desired at Pin, connect a coupling capacitor to this pin. If the coupling at Pin is ac, connect this pin to ground. Note that this pin is also an input, with an input impedance of kω. Such an input is useful for applications with high input voltages and low supply voltages. VIN High Input Impedance Pin. 3 CF Connect an Auxiliary Low-Pass Filter Capacitor from the Output. VS Negative Supply Voltage if Dual Supplies Are Used, or Ground if Connected to a Single-Supply Source. CAV Connect the Averaging Capacitor Here. DC Output Voltage. 7 VS Positive Supply Voltage. COM Common. Rev. H Page of 0

7 TYPICAL PERFORMANCE CHARACTERISTICS ADDITIONAL ERROR (% of Reading) = 00mV rms khz SINE WAVE = 00µF = µf INPUT LEVEL (rms) 0V V 00mV 0mV mv SINE WAVE INPUT, V S =±V, = µf, =.7µF, = µf % ERROR 3dB 0% ERROR SUPPLY VOLTAGE (±V) Figure 3. Additional Error vs. Supply Voltage µV dB FREQUENCY (khz) Figure. Frequency Response Driving Pin PEAK INPUT BEFORE CLIPPING (V) 0 DC-COUPLED PIN PIN INPUT LEVEL (rms) 0V V 00mV 0mV mv SINE WAVE INPUT, V S =±V, = µf, =.7µF, = µf % ERROR 3dB 0% ERROR SUPPLY VOLTAGE (±V) Figure. Maximum Input Level vs. Supply Voltage µV dB FREQUENCY (khz) Figure 7. Frequency Response Driving Pin PEAK BUFFER (V) 0 khz SINE WAVE INPUT ADDITIONAL ERROR (% of Reading) 3 3ms BURST OF khz = 3 CYCLES 00mV rms SIGNAL V S = ±V = µf = 00µF = 0µF = 33µF = 0µF = 00µF SUPPLY VOLTAGE (±V) Figure. Peak Buffer Output vs. Supply Voltage CREST FACTOR (V PEAK /V rms) Figure. Additional Error vs. Crest Factor with Various Values of CAV Rev. H Page 7 of 0

8 ADDITIONAL ERROR (% of Reading) = 00mV rms khz SINE WAVE = 00mF = mf V S = ±V TEMPERATURE ( C) Figure 9. Additional Error vs. Temperature ERROR (% of Reading) = SINE khz = µf, = 7µF, =.7µF, V S = ±V. 0mV 00mV V V INPUT LEVEL (rms) Figure. Error vs. RMS Input Voltage (Pin ), Output Buffer Offset Is Adjusted to Zero DC SUPPLY CURRENT (µa) = 00mV rms khz SINE WAVE = 00µF = µf V S = ±V (µf) 00 0 % 0.% = 00mV rms = 7µF = 7µF V S = ±V rms INPUT LEVEL (V) Figure 0. DC Supply Current vs. rms Input Level k FREQUENCY (Hz) Figure 3. CAV vs. Frequency for Specified Averaging Error mV = khz SINE WAVE INPUT AC-COUPLED V S = ±V V % 0.% INPUT LEVEL (rms) mv 00µV INPUT LEVEL (rms) 00mV 0mV 0µV 00 k 0k 00k 3dB FREQUENCY (Hz) Figure. RMS Input Level (Pin ) vs. 3 db Frequency SINE WAVE AC-COUPLED = 0µF, = 7µF, = 7µF, V S = ±V mv 0 00 k FREQUENCY (Hz) Figure. RMS Input Level vs. Frequency for Specified Averaging Error Rev. H Page of 0

9 .0 0nA INPUT BIAS CURRENT (pa) INPUT BIAS CURRENT na 00pA 0pA pa SUPPLY VOLTAGE (±V) Figure. Pin Input Bias Current vs. Supply Voltage fA 3 0 TEMPERATURE ( C) Figure 7. Pin Input Bias Current vs. Temperature V V S = V = µf = 0µF 00mV INPUT LEVEL (rms) 0mV = 0µF = 33µF = 00µF mv 00µV ms 0ms 00ms s 0s 00s SETTLING TIME Figure. RMS Input Level for Various Values of CAV vs. Settling Time Rev. H Page 9 of 0

10 THEORY OF OPERATION AC = 0µF DC OPTIONAL RETURN PATH FWR CURRENT MODE ABSOLUTE VALUE COM 7 0.µF V S INPUT I B <0pA 3 BIAS SECTION rms rms TRANSLINEAR CORE 0.µF TO COM PIN C A 33µF As shown by Figure, the has five functional subsections: the input amplifier, full-wave rectifier (FWR), rms core, output amplifier, and bias section. The FET input amplifier allows both a high impedance, buffered input (Pin ) and a low impedance, wide dynamic range input (Pin ). The high impedance input, with its low input bias current, is well suited for use with high impedance input attenuators. The output of the input amplifier drives a full-wave precision rectifier that, in turn, drives the rms core. The essential rms operations of squaring, averaging, and square rooting are performed in the core using an external averaging capacitor, CAV. Without CAV, the rectified input signal travels through the core unprocessed, as is done with the average responding connection (see Figure 9). A final subsection, an output amplifier, buffers the output from the core and allows optional low-pass filtering to be performed via the external capacitor, CF, which is connected across the feedback path of the amplifier. In the average responding connection, this is where all of the averaging is carried out. In the rms circuit, this additional filtering stage helps reduce any output ripple that was not removed by the averaging capacitor, CAV. 0µF (OPTIONAL) Figure. True RMS Circuit TYPES OF AC MEASUREMENT The is capable of measuring ac signals by operating as either an average responding converter or a true rms-to-dc converter. As its name implies, an average responding converter computes the average absolute value of an ac (or ac and dc) voltage or current by full-wave rectifying and low-pass filtering the input signal; this approximates the average. The resulting output, a dc average level, is scaled by adding (or reducing) gain; this scale factor converts the dc average reading to an rms equivalent value for the waveform being measured. For example, the average absolute value of a sine wave voltage is 0.3 times VPEAK; the corresponding rms value is VPEAK. Therefore, for sine wave voltages, the required scale factor is. (0.707/0.3). In contrast to measuring the average value, true rms measurement is a universal language among waveforms, allowing the magnitudes of all types of voltage (or current) waveforms to be compared to one another and to dc. RMS is a direct measure of the power or heating value of an ac voltage compared to that of a dc voltage; an ac signal of V rms produces the same amount of heat in a resistor as a V dc signal. Rev. H Page 0 of 0

11 Mathematically, the rms value of a voltage is defined (using a simplified equation) as V rms = Avg ( V ) This involves squaring the signal, taking the average, and then obtaining the square root. True rms converters are smart rectifiers; they provide an accurate rms reading regardless of the type of waveform being measured. However, average responding converters can exhibit very high errors when their input signals deviate from their precalibrated waveform; the magnitude of the error depends on the type of waveform being measured. For example, if an average responding converter is calibrated to measure the rms value of sine wave voltages and then is used to measure either symmetrical square waves or dc voltages, the converter has a computational error % (of reading) higher than the true rms value (see Table ). CALCULATING SETTLING TIME USING FIGURE Figure can be used to closely approximate the time required for the to settle when its input level is reduced in amplitude. The net time required for the rms converter to settle is the difference between two times extracted from the graph (the initial time minus the final settling time). As an example, consider the following conditions: a 33 μf averaging capacitor, a 00 mv initial rms input level, and a final (reduced) mv input level. From Figure, the initial settling time (where the 00 mv line intersects the 33 μf line) is approximately 0 ms. The settling time corresponding to the new or final input level of mv is approximately seconds. Therefore, the net time for the circuit to settle to its new value is seconds minus 0 ms, which is 7.9 seconds. Note that because of the smooth decay characteristic inherent with a capacitor/diode combination, this is the total settling time to the final value (that is, not the settling time to %, 0.%, and so on, of the final value). In addition, this graph provides the worst-case settling time because the settles very quickly with increasing input levels. RMS MEASUREMENT CHOOSING THE OPTIMUM VALUE FOR Because the external averaging capacitor, CAV, holds the rectified input signal during rms computation, its value directly affects the accuracy of the rms measurement, especially at low frequencies. Furthermore, because the averaging capacitor appears across a diode in the rms core, the averaging time constant increases exponentially as the input signal is reduced. This means that as the input level decreases, errors due to nonideal averaging decrease, and the time required for the circuit to settle to the new rms level increases. Therefore, lower input levels allow the circuit to perform better (due to increased averaging) but increase the waiting time between measurements. Obviously, when selecting CAV, a trade-off between computational accuracy and settling time is required. Table. Error Introduced by an Average Responding Circuit when Measuring Common Waveforms Waveform Type V Peak Amplitude Crest Factor (VPEAK/V rms) True RMS Value (V) Average Responding Circuit Calibrated to Read RMS Value of Sine Waves (V) Undistorted Sine Wave Symmetrical Square Wave Undistorted Triangle Wave Gaussian Noise (9% of Peaks < V) Rectangular Pulse Train SCR Waveforms 0% Duty Cycle % Duty Cycle % of Reading Error Using Average Responding Circuit Rev. H Page of 0

12 RAPID SETTLING TIMES VIA THE AVERAGE RESPONDING CONNECTION Because the average responding connection shown in Figure 9 does not use the CAV averaging capacitor, its settling time does not vary with the input signal level. It is determined solely by the RC time constant of CF and the internal kω resistor in the output amplifier s feedback path. INPUT POSITIVE SUPPLY COMMON NEGATIVE SUPPLY 0µF (OPTIONAL) FULL WAVE RECTIFIER 33µF 0.µF 0.µF V S V S 7 COM V S 3 BIAS SECTION rms CAV CORE Figure 9. Average Responding Circuit V OUT DC ERROR, RIPPLE, AND AVERAGING ERROR Figure 0 shows the typical output waveform of the with a sine wave input applied. As with all real-world devices, the ideal output of VOUT = VIN is never achieved exactly. Instead, the output contains both a dc and an ac error component. As shown in Figure 0, the dc error is the difference between the average of the output signal (when all the ripple in the output is removed by external filtering) and the ideal dc output. The dc error component is therefore set solely by the value of the averaging capacitor used. No amount of post filtering (that is, using a very large CF) allows the output voltage to equal its ideal value. The ac error component, an output ripple, can be easily removed by using a large enough post filtering capacitor, CF In most cases, the combined magnitudes of both the dc and ac error components need to be considered when selecting appropriate values for Capacitor CAV and Capacitor CF. This combined error, representing the maximum uncertainty of the measurement, is termed the averaging error and is equal to the peak value of the output ripple plus the dc error. E O IDEAL E O DC ERROR = E O E O (IDEAL) AVERAGE E O = E O DOUBLE-FREQUENCY RIPPLE TIME Figure 0. Output Waveform for Sine Wave Input Voltage As the input frequency increases, both error components decrease rapidly; if the input frequency doubles, the dc error and ripple reduce to one quarter and one half of their original values, respectively, and rapidly become insignificant. AC MEASUREMENT ACCURACY AND CREST FACTOR The crest factor of the input waveform is often overlooked when determining the accuracy of an ac measurement. Crest factor is defined as the ratio of the peak signal amplitude to the rms amplitude (crest factor = VPEAK/V rms). Many common waveforms, such as sine and triangle waves, have relatively low crest factors ( ). Other waveforms, such as low duty-cycle pulse trains and SCR waveforms, have high crest factors. These types of waveforms require a long averaging time constant (to average out the long periods between pulses). Figure shows the additional error vs. the crest factor of the for various values of CAV Rev. H Page of 0

13 APPLICATIONS CONNECTING THE INPUT The inputs of the resemble an op amp, with noninverting and inverting inputs. The input stages are JFETs accessible at Pin and Pin. Designated as the high impedance input, Pin is connected directly to a JFET gate. Pin is the low impedance input because of the scaling resistor connected to the gate of the second JFET. This gate-resistor junction is not externally accessible and is servo-ed to the voltage level of the gate of the first JFET, as in a classic feedback circuit. This action results in the typical kω input impedance referred to ground or reference level. This input structure provides four input configurations as shown in Figure, Figure, Figure 3, and Figure. Figure and Figure show the high impedance configurations, and Figure 3 and Figure show the low impedance connections used to extend the input voltage range. 3 COM V 7 S VS VOUT DC Figure 3. Low-Z AC-Coupled Input Connection 3 COM V 7 S VS VOUT DC MΩ 3 COM V 7 S V S VOUT DC Figure. Low-Z DC-Coupled Input Connection Figure. High-Z AC-Coupled Input Connection (Default) COM V 7 S VS 3 VOUT DC Figure. High-Z DC-Coupled Input Connection Rev. H Page 3 of 0

14 SELECTING PRACTICAL VALUES FOR INPUT COUPLING ( ), AVERAGING ( ), AND FILTERING ( ) CAPACITORS Table provides practical values of CAV and CF for several common applications. The input coupling capacitor, CC, in conjunction with the kω internal input scaling resistor, determine the 3 db low frequency roll-off. This frequency, FL, is equal to F = L π (000)( Value of C in Farads) C Note that at FL, the amplitude error is approximately 30% ( 3 db) of the reading. To reduce this error to 0.% of the reading, choose a value of CC that sets FL at one-tenth of the lowest frequency to be measured. In addition, if the input voltage has more than 00 mv of dc offset, then the ac-coupling network shown in Figure 7 should be used in addition to CC. Table. Capacitor Selection Chart Application RMS Input Level Low Frequency Cutoff ( 3 db) Max Crest Factor CAV (μf) CF (μf) Settling Time to % General-Purpose RMS Computation 0 V to V 0 Hz ms 00 Hz 3 ms 0 mv to 00 mv 0 Hz ms 00 Hz ms General Purpose 0 V to V 0 Hz None 33. sec Average 00 Hz None ms Responding 0 mv to 00 mv 0 Hz None 33. sec 00 Hz None ms SCR Waveform Measurement 0 mv to 00 mv 0 Hz sec 0 Hz 7.0 sec 0 mv to 00 mv 0 Hz sec 0 Hz sec Audio Applications Speech 0 mv to 00 mv 300 Hz ms Music 0 mv to 00 mv 0 Hz sec Settling time is specified over the stated rms input level with the input signal increasing from zero. Settling times are greater for decreasing amplitude input signals. OPTIONAL AOUPLING CAPACITOR 0.0µF 9MΩ 900kΩ 90kΩ 0kΩ kv 00mV V 0V 00V 7kΩ W V S N N 3 0µF (OPTIONAL) FULL WAVE RECTIFIER INPUT BIAS SECTION rms CORE COM V S 7 V S µf µf 33µF 0µF (OPTIONAL) Figure. with a High Impedance Input Attenuator Rev. H Page of 0

15 IN IN AD7 3 0µF INPUT IMPEDANCE: 0 Ω 0pF FULL WAVE RECTIFIER INPUT V S 7 COM 3 BIAS SECTION rms CORE V S µf µf 33µF 0µF (OPTIONAL) Figure. Differential Input Connection DC-COUPLED 0.µF AC-COUPLED MΩ 3 0µF (OPTIONAL) FULL WAVE RECTIFIER INPUT BIAS SECTION V S rms CORE COM V S 7 V S µf MΩ 39MΩ V OS ADJUST µf 33µF 0µF (OPTIONAL) Figure 7. External Output VOS Adjustment µF 0.µF MΩ V S 3 INPUT BIAS SECTION FULL WAVE RECTIFIER COM V S rms CORE 7 33µF 00kΩ V S 00kΩ.7µF.7µF 9V 0µF (OPTIONAL) Figure. Battery-Powered Option Rev. H Page of 0

16 EVALUATION BOARD An evaluation board, -EVALZ, is available for experimentation or becoming familiar with rms-to-dc converters. Figure 9 is a photograph of the board, and Figure 30 is the top silkscreen showing the component locations. Figure 3, Figure 3, Figure 33, and Figure 3 show the layers of copper, and Figure 3 shows the schematic of the board configured as shipped. The board is designed for multipurpose applications and can be used for the AD737 as well. Figure 3. Evaluation Board Component-Side Copper Figure 9. Evaluation Board Figure 30. Evaluation Board Component-Side Silkscreen As shipped, the board is configured for dual supplies and high impedance input. Optional jumper locations enable low impedance and dc input connections. Using the low impedance input (Pin ) often enables higher input signals than otherwise possible. A dc connection enables an ac plus dc measurement, but care must be taken so that the opposite polarity input is not dc-coupled to ground. Figure 3 shows the board schematic with all movable jumpers. The jumper positions in black are default connections; the dottedoutline jumpers are optional connections. The board is tested prior to shipment and only requires a power supply connection and a precision meter to perform measurements. Table is the bill of materials for the evaluation board Figure 3. Evaluation Board Secondary-Side Copper Figure 33. Evaluation Board Internal Power Plane Figure 3. Evaluation Board Internal Ground Plane Rev. H Page of 0

17 V S GND GND GND3 GND C 0µF V V S C 0µF V W DC COUP W LO-Z IN LO-Z W3 AOUP R3 0Ω J VIN CIN 0.µF GND NORM PD P HI-Z SEL IN R MΩ SEL J3 W HI-Z C 0.µF 3 CAV 33µF V R 0Ω COM C 7 0.µF V S V S OUT CAV VOUT CF J V S FILT CF Figure 3. Evaluation Board Schematic Table. Evaluation Board Bill of Materials Qty Name Description Reference Designator Manufacturer Mfg. Part Number Test loop Red VS Components Corp. TP Test loop Green VS Components Corp. TP Capacitors Tantalum 0 μf, V C, C Nichicon Corp. F93E0MCC 3 Capacitors 0. μf, V, 003, X7R C, C, CIN KEMET Corp. C003C0KRACTU Capacitor Tantalum 33 μf, V, 0%, 03 CAV Nichicon Corp. F93C33MCC Test loops Purple CAV, HI Z, LO Z, VIN, VOUT Components Corp. TP Integrated circuit RMS-to-dc converter DUT Analog Devices, Inc. JRZ Test loops Black GND, GND, GND3, GND Components Corp. TP Connectors BNC, right angle J, J AMP 7- Header -pin, 3 J3 3M Header 3-pin P Molex, Inc Resistor MΩ, /0 W, %, 003 R Panasonic Corp. ERJ3EKF00V Resistors 0 Ω, %, 003 R3, R Panasonic Corp. ERJ3GEY0R00V Headers -pin, 0." center W, W, W3, W Molex, Inc Rev. H Page 7 of 0

18 OUTLINE DIMENSIONS 0.00 (0.) 0.3 (9.7) 0.3 (9.0) 0.0 (.33) MAX 0.0 (3.) 0.30 (3.30) 0. (.9) 0.0 (0.) 0.0 (0.) 0.0 (0.3) 0.00 (.) BSC 0.0 (7.) 0.0 (.3) 0.0 (.0) 0.0 (0.3) MIN SEATING PLANE 0.00 (0.3) MIN 0.00 (.) MAX 0.0 (0.3) GAUGE PLANE 0.3 (.) 0.30 (7.7) (7.) 0.30 (0.9) MAX 0.9 (.9) 0.30 (3.30) 0. (.9) 0.0 (0.3) 0.00 (0.) 0.00 (0.0) (.7) 0.00 (.) 0.0 (.) COMPLIANT TO JEDEC STANDARDS MS-00 CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS (IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN. CORNER LEADS MAY BE CONFIGURED AS WHOLE OR HALF LEADS. Figure 3. -Lead Plastic Dual In-Line Package [PDIP] Narrow Body (N-) Dimensions shown in inches and (millimeters) 0700-A 0.00 (0.3) MIN 0.0 (.0) MAX 0.00 (.0) MAX 0.00 (.) BSC 0.0 (0.9) MAX 0.00 (.0) 0. (3.) 0.03 (0.) 0.0 (0.3) (.7) (0.7) 0.30 (7.7) 0.0 (.9) 0.00 (.) 0.0 (0.3) 0.0 (3.) MIN SEATING PLANE CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS (IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FOR REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN (.3) 0.90 (7.37) Figure 37. -Lead Ceramic Dual In-Line Package [CERDIP] (Q-) Dimensions shown in inches and (millimeters) 0.0 (0.3) 0.00 (0.0).00 (0.7) 3.0 (0.97) 0. (0.009) 0.0 (0.000) COPLANARITY 0.0 SEATING PLANE.00 (0.9).0 (0.90).7 (0.000) BSC.0 (0.).0 (0.).7 (0.0).3 (0.03) 0. (0.00) 0.3 (0.0) 0. (0.009) 0.7 (0.007) 0.0 (0.09) 0. (0.0099).7 (0.000) 0.0 (0.07) COMPLIANT TO JEDEC STANDARDS MS-0-AA CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS (IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR REFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN. Figure 3. -Lead Standard Small Outline Package [SOIC_N] Narrow Body (R-) Dimensions shown in millimeters and (inches) A Rev. H Page of 0

19 ORDERING GUIDE Model Temperature Range Package Description Package Option AQ 0 C to C -Lead CERDIP Q- BQ 0 C to C -Lead CERDIP Q- AR 0 C to C -Lead SOIC_N R- AR-REEL 0 C to C -Lead SOIC_N R- AR-REEL7 0 C to C -Lead SOIC_N R- ARZ 0 C to C -Lead SOIC_N R- ARZ-R7 0 C to C -Lead SOIC_N R- ARZ-RL 0 C to C -Lead SOIC_N R- BR 0 C to C -Lead SOIC_N R- BR-REEL 0 C to C -Lead SOIC_N R- BR-REEL7 0 C to C -Lead SOIC_N R- BRZ 0 C to C -Lead SOIC_N R- BRZ-R7 0 C to C -Lead SOIC_N R- BRZ-RL 0 C to C -Lead SOIC_N R- JN 0 C to 70 C -Lead PDIP N- JNZ 0 C to 70 C -Lead PDIP N- KN 0 C to 70 C -Lead PDIP N- KNZ 0 C to 70 C -Lead PDIP N- JR 0 C to 70 C -Lead SOIC_N R- JR-REEL 0 C to 70 C -Lead SOIC_N R- JR-REEL7 0 C to 70 C -Lead SOIC_N R- JRZ 0 C to 70 C -Lead SOIC_N R- JRZ-RL 0 C to 70 C -Lead SOIC_N R- JRZ-R7 0 C to 70 C -Lead SOIC_N R- KR 0 C to 70 C -Lead SOIC_N R- KR-REEL 0 C to 70 C -Lead SOIC_N R- KR-REEL7 0 C to 70 C -Lead SOIC_N R- KRZ 0 C to 70 C -Lead SOIC_N R- KRZ-RL 0 C to 70 C -Lead SOIC_N R- KRZ-R7 0 C to 70 C -Lead SOIC_N R- -EVALZ Evaluation Board Z = RoHS compliant part. Rev. H Page 9 of 0

20 NOTES 007 Analog Devices, Inc. All rights reserved. Trademarks and registered trademarks are the property of their respective owners. C003-0-/07(H) Rev. H Page 0 of 0