AD650 Freq to Voltage

7/31/2019 AD650 Freq to Voltage

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Voltage-to-Frequency andFrequency-to-Voltage Converter

AD650

Rev. DInformation furnished by Analog Devices is believed to be accurate and reliable. However, noresponsibility is assumed by Analog Devices for its use, nor for any infringements of patents or otherrights of third parties that may result from its use. Specifications subject to change without notice. Nolicense 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 9106, Norwood, MA 02062-9106, U.S.A.Tel: 781.329.4700 www.analog.comFax: 781.461.3113 2006 Analog Devices, Inc. All rights reserved.

FEATURESV/F conversion to 1 MHzReliable monolithic constructionVery low nonlinearity

0.002% typ at 10 kHz0.005% typ at 100 kHz0.07% typ at 1 MHz

Input offset trimmable to zeroCMOS- or TTL-compatibleUnipolar, bipolar, or differential V/FV/F or F/V conversionAvailable in surface mountMIL-STD-883 compliant versions available

FUNCTIONAL BLOCK DIAGRAM

0 0 7 9 7

- 0 0 1

OPAMP

COMP

INFREQ

OUT

OUTONE

SHOT

8 FOUTPUT

9COMPARATORINPUT

10DIGITALGND

11ANALOGGND

12 +VS

13OFFSETNULL

7NC

6ONE

SHOTCAPACITOR

5 VS

4BIPOLAR

OFFSETCURRENT

3 IN

2+IN

1VOUT 14OFFSETNULLINPUT

OFFSETTRIM

0.6V

AD650

VS

VS

1mA

S1

NC = NO CONNECT Figure 1.

PRODUCT DESCRIPTION

The AD650 V/F/V (voltage-to-frequency or frequency-to-voltageconverter) provides a combination of high frequency operationand low nonlinearity previously unavailable in monolithic form.The inherent monotonicity of the V/F transfer function makesthe AD650 useful as a high-resolution analog-to-digital converter.A flexible input configuration allows a wide variety of input voltage and current formats to be used, and an open-collectoroutput with separate digital ground allows simple interfacing toeither standard logic families or opto-couplers.

The linearity error of the AD650 is typically 20 ppm (0.002% of full scale) and 50 ppm (0.005%) maximum at 10 kHz full scale.This corresponds to approximately 14-bit linearity in an analog-to-digital converter circuit. Higher full-scale frequencies orlonger count intervals can be used for higher resolutionconversions. The AD650 has a useful dynamic range of sixdecades allowing extremely high resolution measurements.Even at 1 MHz full scale, linearity is guaranteed less than1000 ppm (0.1%) on the AD650KN, BD, and SD grades.

In addition to analog-to-digital conversion, the AD650 can beused in isolated analog signal transmission applications,

phased-locked loop circuits, and precision stepper motor speedcontrollers. In the F/V mode, the AD650 can be used inprecision tachometer and FM demodulator circuits.

The input signal range and full-scale output frequency are user-programmable with two external capacitors and one resistor.Input offset voltage can be trimmed to zero with an externalpotentiometer.

The AD650JN and AD650KN are offered in plastic 14-lead DIPpackages. The AD650JP is available in a 20-lead plastic leadedchip carrier (PLCC). Both plastic packaged versions of theAD650 are specified for the commercial temperature range(0C to 70C). For industrial temperature range (25C to+85C) applications, the AD650AD and AD650BD are offeredin ceramic packages. The AD650SD is specified for the full55C to +125C extended temperature range.

PRODUCT HIGHLIGHTS1. Can operate at full-scale output frequencies up to 1 MHz

(in addition to having very high linearity).

2. Can be configured to accommodate bipolar, unipolar, ordifferential input voltages, or unipolar input currents.

3. TTL or CMOS compatibility is achieved by using an opencollector frequency output. The pull-up resistor can beconnected to voltages up to 30 V.

4. The same components used for V/F conversion can also beused for F/V conversion by adding a simple logic biasing

network and reconfiguring the AD650.5. Separate analog and digital grounds prevent ground loops

in real-world applications.

6. Available in versions compliant with MIL-STD-883.


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AD650

Rev. D | Page 2 of 20

TABLE OF CONTENTSFeatures.............................................................................................. 1

Functional Block Diagram .............................................................. 1

Product Description......................................................................... 1

Product Highlights ........................................................................... 1

Revision History ............................................................................... 2

Specifications..................................................................................... 3

Absolute Maximum Ratings............................................................ 5

ESD Caution.................................................................................. 5

Pin Configurations and Function Descriptions........................... 6

Circuit Operation ............................................................................. 7

Unipolar Configuration............................................................... 7 Component Selection................................................................... 8

Bipolar V/F .................................................................................. 10

Unipolar V/F, Negative Input Voltage ..................................... 10

F/V Conversion .......................................................................... 10

High Frequency Operation....................................................... 10

Decoupling and Grounding...................................................... 12

Temperature Coefficients.......................................................... 12

Nonlinearity Specification ........................................................ 13

PSRR............................................................................................. 1

Other Circuit Considerations................................................... 14

Applications..................................................................................... 16

Differential Voltage-to-Frequency Conversion...................... 16

Autozero Circuit......................................................................... 16

Phase-Locked Loop F/V Conversion ...................................... 17 Outline Dimensions....................................................................... 19

Ordering Guide .......................................................................... 20

REVISION HISTORY

3/06Rev. C to Rev. D Updated Format..................................................................UniversalChanges to Product Highlights....................................................... 1Changes to Table 1............................................................................ 3Added Pin Function Descriptions Table ...................................... 6Updated Outline Dimensions....................................................... 18Changes to Ordering Guide.......................................................... 19


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SPECIFICATIONST = 25C, VS = 15 V, unless otherwise noted.

Table 1.AD650J/AD650A AD650K/AD650B AD650S

Model Min Typ Max Min Typ Max Min Typ Max UnitsDYNAMIC PERFORMANCEFull-Scale Freque ncy Range 1 1 1 MHzNonlinearity 1

f MAX= 10 kHz 0.002 0.005 0.002 0.005 0.002 0.005 %f MAX= 100 kHz 0.005 0.02 0.005 0.02 0.005 0.02 %f MAX= 500 kHz 0.02 0.05 0.02 0.05 0.02 0.05 %f MAX= 1 MHz 0.1 0.05 0.1 0.05 0.1 %

Full-Scale Calibration Error2 100 kHz 5 5 5 %1 MHz 10 10 10 %

vs. Supply3 0.015 +0.015 0.015 +0.015 0.015 +0.015% of FSR/V

vs. Temperature

A, B, and S Gradesat 10 kHz 75 75 75 ppm/at 100 kHz 150 150 200 ppm/

J and K Gradesat 10 kHz 75 75 ppm/at 100 kHz 150 150 ppm/

BIPOLAR OFFSET CURRENTActivated by 1.24 k Between

Pin 4 and Pin 5 0.45 0.5 0.55 0.45 0.5 0.55 0.45 0.5 0.55 mADYNAMIC RESPONSE

Maximum Settling Time forFull-Scale Step Input 1 pulse of new frequency plus 1 s 1 pulse of new frequency plus 1 s 1 pulse of new frequency plus 1 s

Overload Recovery TimeStep Input 1 pulse of new frequency plus 1 s 1 pulse of new frequency plus 1 s 1 pulse of new frequency plus 1 s

ANALOG INPUT AMPLIFIER(V/F CONVERSION)Current Input Range ( Figure 4) 0 +0.6 0 +0.6 0 +0.6 mAVoltage Input Range ( Figure 12) 10 0 10 0 10 0 VDifferential Impedance 2 M||10 pF 2 M||10 pF 2 M||10 pFCommon-Mode Impedance 1000 M||10 pF 1000 M||10 pF 1000 M||10 pFInput Bias Current

Noninverting Input 40 100 40 100 40 100 nAInverting Input 8 20 8 20 8 20 nA

Input Offset Voltage(Trimmable to Zero) 4 4 4 mVvs. Temperature (TMINto TMAX) 30 30 30 V/C

Safe Input Voltage VS VS VS VCOMPARATOR (F/V CONVERSION)

Logic 0 Level VS 1 VS 1 VS 1 VLogic 1 Level 0 +VS 0 +VS 0 +VS VPulse Width Range 4 0.1 (0.3 tOS) 0.1 (0.3 tOS) 0.1 (0.3 tOS) sInput Impedance 250 250 250 k

OPEN COLLECTOR OUTPUT(V/F CONVERSION)Output Voltage in Logic 0

ISINK 8 mA, TMINto TMAX 0.4 0.4 0.4 VOutput Leakage Current in Logic 1 100 100 100 nAVoltage Rang e 5 0 36 0 36 0 36 V


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AD650


AD650J/AD650A AD650K/AD650B AD650SModel Min Typ Max Min Typ Max Min Typ Max UnitsAMPLIFIER OUTPUT (F/V CONVERSION)

Voltage Range(1500 Min Load Resistance) 0 10 0 10 0 10 V

Source Current(750 Max Load Resistance) 10 10 10 mA

Capacitive Load(Without Oscillation) 100 100 100 pF

POWER SUPPLYVoltage, Rated Performance 9 18 9 18 9 18 VQuiescent Current 8 8 8 mA

TEMPERATURE RANGERated Performance

N Package 0 +70 0 +70 CD Package 25 +85 25 +85 55 +125 C

1 Nonlinearity is defined as deviation from a straight line from zero to full scale, expressed as a fraction of full scale.2 Full-scale calibration error adjustable to zero.3 Measured at full-scale output frequency of 100 kHz.4 Refer to F/V conversion section of the text.5 Referred to digital ground.

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 minand max specifications are guaranteed, although only those shown in boldface are tested on all production units.


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AD65


ABSOLUTE MAXIMUM RATINGSParameter Rating Total Supply Voltage 36 VStorage Temperature Range 55C to +150CDifferential Input Voltage 10 VMaximum Input Voltage VS Open Collector Output Voltage

Above Digital GND36 V

Current 50 mAAmplifier Short Circuit to Ground IndefiniteComparator Input Voltage V S

Stresses above those listed under Absolute Maximum Ratingsmay cause permanent damage to the device. This is a stressrating only; functional operation of the device at these or any other conditions above those indicated in the operationalsection of this specification is not implied. Exposure to absolutemaximum rating conditions for extended periods may affectdevice reliability.

ESD CAUTIONESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily accumulate onthe human body and test equipment and can discharge without detection. Although this product featuresproprietary ESD protection circuitry, permanent damage may occur on devices subjected to high energyelectrostatic discharges. Therefore, proper ESD precautions are recommended to avoid performance

degradation or loss of functionality.


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AD650


PIN CONFIGURATIONS AND FUNCTION DESCRIPTIONSVOUT 1

+IN 2

IN 3BIBOLAR OFFSET

CURRENT4

OFFSET NULL14

OFFSET NULL13

+VS12

ANALOG GND11

VS 5 DIGITAL GND10ONE SHOT

CAPACITOR6 COMPARATORINPUT9

NC 7 FOUTPUT8

NC = NO CONNECT

AD650TOP VIEW

(Not to Scale)

0 0 7 9 7

- 0 1 0

Figure 2. D-14, N-14 Pin Configurations

1 20 1923

4

5

6

7

8

18

17

16

15

14

9 10 11 12 13

NC = NO CONNECT

INNC

BIPOLAR OFFSETCURRENT

NC

VS

+VS

NC

ANALOG GND

NC

DIGITAL GND

+ I N

V O U T

N C

O F F S E T

N U L L

O F F S E T

N U L L

O N E S H O T

C A P A C I T O R

N C

N C

F O U T P U T

C O M P A R A T O R

I N P U T

PIN 1INDENTFIER

AD650TOP VIEW

(Not to scale)

0 0 7 9 7

- 0 1 1

Figure 3. P-20A Pin Configuration

Table 2. Pin Function Descriptions

Pin No.D-14, N-14 P-20A Mnemonic Description1 2 VOUT Output of Operational Amplifier. The operational amplifier, along with C INT,

is used in the integrate stage of the V to F conversion.2 3 +IN Positive Analog Input.3 4 IN Negative Analog Input.4 6 BIPOLAR OFFSET

CURRENTOn-Chip Current Source. This can be used in conjunction with an externalresistor to remove the operational amplifiers offset.

5 8 VS Negative Power Supply Input.6 9 ONE-SHOT

CAPACITOR The Capacitor, COS, is Connected to This Pin. COS determines the time periodfor the one shot.

7 1, 5, 7, 10, 11, 15, 17 NC No Connect.8 12 FOUTPUT Frequency Output from AD650.9 13 COMPARATOR INPUT Input to Comparator. When the input voltage reaches 0.6 V, the one shot is

triggered.10 14 DIGITAL GND Digital Ground.11 16 ANALOG GND Analog Ground.12 18 +VS Positive Power Supply Input.13, 14 19, 20 OFFSET NULL Offset Null Pins. Using an external potentiometer, the offset of the

operational amplifier can be removed.


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AD650


The positive input voltage develops a current (I IN = VIN/R IN) thatcharges the integrator capacitor C INT. As charge builds up onCINT, the output voltage of the integrator ramps downwardtowards ground. When the integrator output voltage (Pin 1)crosses the comparator threshold (0.6 V) the comparatortriggers the one shot, whose time period, t OS is determined by the one-shot capacitor C OS.

Specifically, the one-shot time period is

sec100.3F/sec108.6 73 += OSOS C t (1)

The reset period is initiated as soon as the integrator output voltage crosses the comparator threshold, and the integratorramps upward by an amount

( IN INT

OSOS I C

)t dt dV t V == mA1 (2)

After the reset period has ended, the device starts anotherintegration period, as shown in Figure 8, and starts rampingdownward again. The amount of time required to reach thecomparator threshold is given as

( )

=

== 1mA1

mA11

IN OS

INT

N

IN INT

OS

I t

C I

I C t

dt dV

V T (3)

The output frequency is now given as

F C RV AF

t I

T t f

OS

IN IN

OS

IN

OSOUT

11

1

104.4 /Hz15.0

mA11

+

=

=+

=(4)

Note that C INT, the integration capacitor, has no effect on thetransfer relation, but merely determines the amplitude of thesawtooth signal out of the integrator.

One-Shot Timing

A key part of the preceding analysis is the one-shot time periodgiven in Equation 1. This time period can be broken down intoapproximately 300 ns of propagation delay and a second timesegment dependent linearly on timing capacitor C OS. When theone shot is triggered, a voltage switch that holds Pin 6 at analog

ground is opened, allowing that voltage to change. An internal0.5 mA current source connected to Pin 6 then draws itscurrent out of C OS, causing the voltage at Pin 6 to decreaselinearly. At approximately 3.4 V, the one shot resets itself,thereby ending the timed period and starting the V/Fconversion cycle over again. The total one-shot time period canbe written mathematically as

DELAY GATEDISCHARGE

OSOS T I

C V t +

= (5)

substituting actual values quoted in Equation 5,

sec10300A105.0

V4.3 93

+

= OSOS

C t (6)

This simplifies into the timed period equation (see Equation 1).

COMPONENT SELECTION

Only four component values must be selected by the user. Theseare input resistance R IN, timing capacitor C OS, logic resistor R2,and integration capacitor C INT. The first two determine theinput voltage and full-scale frequency, while the last two aredetermined by other circuit considerations.

Of the four components to be selected, R2 is the easiest todefine. As a pull-up resistor, it should be chosen to limit thecurrent through the output transistor to 8 mA if a TTLmaximum V OL of 0.4 V is desired. For example, if a 5 V logicsupply is used, R2 should be no smaller than 5 V/8 mA or625 . A larger value can be used if desired.

R IN and COS are the only two parameters available to set the full-scale frequency to accommodate the given signal range. The swing variable that is affected by the choice of R IN and COS is nonlinearity.The selection guides of Figure 9 and Figure 10 show this quitegraphically. In general, larger values of COS and lower full-scaleinput currents (higher values of R IN) provide better linearity. InFigure 10, the implications of four different choices of R IN areshown. Although the selection guide is set up for a unipolarconfiguration with a 0 V to 10 V input signal range, the resultscan be extended to other configurations and input signal ranges.For a full-scale frequency of 100 kHz (corresponding to 10 Vinput), among the available choices R IN = 20 k and C OS = 620 pFgives the lowest nonlinearity, 0.0038%. In addition, the highestfrequency that gives the 20 ppm minimum nonlinearity isapproximately 33 kHz (40.2 k and 1000 pF).

For input signal spans other than 10 V, the input resistancemust be scaled proportionately. For example, if 100 k is calledout for a 0 V to 10 V span, 10 k would be used with a 0 V to 1 Vspan, or 200 k with a 10 V bipolar connection.

The last component to be selected is the integration capacitorCINT. In almost all cases, the best value for CINT can be calculatedusing the equation

( minimumpF1000sec/104

) MAX

INT

f

F C

= (7)

When the proper value for C INT is used, the charge balancearchitecture of the AD650 provides continuous integrationof the input signal, therefore, large amounts of noise andinterference can be rejected. If the output frequency ismeasured by counting pulses during a constant gate period,the integration provides infinite normal-mode rejection forfrequencies corresponding to the gate period and its harmonics.However, if the integrator stage becomes saturated by anexcessively large noise pulse, then the continuous integration of the signal is interrupted, allowing the noise to appear at the output.


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AD65


If the approximate amount of noise that appears on C INT is known(VNOISE), then the value of CINT can be checked using the followinginequality:

NOISES

OSINT V V

At C +

>

V3101 3

(8)

For example, consider an application calling for a maximumfrequency of 75 kHz, a 0 V to 1 V signal range, and supply voltages of only 9 V. The component selection guide of Figure 9 is used to select 2.0 k for R IN and 1000 pF for COS. This resultsin a one-shot time period of approximately 7 s. Substituting75 kHz into Equation 7 yields a value of 1300 pF for CINT. Whenthe input signal is near zero, 1 mA flows through the integrationcapacitor to the switched current sink during the reset phase,causing the voltage across CINT to increase by approximately 5.5 V.Because the integrator output stage requires approximately 3 Vheadroom for proper operation, only 0.5 V margin remains forintegrating extraneous noise on the signal line. A negative noisepulse at this time could saturate the integrator, causing an errorin signal integration. Increasing C INT to 1500 pF or 2000 pFprovides much more noise margin, thereby eliminating thispotential trouble spot.

1MHz

100kHz

10kHz

50 100 1000

F R E Q U E N C Y F U

L L - S

C A L E

C OS (pF)

0 0 7 9 7

- 0 0 8

INPUTRESISTOR

16.9k20k

40.2k

100k

Figure 9. Full-Scale Frequency vs. C OS

100

20

50 100 1000

T Y P I C A L N O N L I N E A R I T Y ( p p m

)

ONE SHOT CAPACITORCOS (pF)

1000

INPUTRESISTOR

16.9k

40.2k

100k

20k

0 0 7 9 7

- 0 0 9

Figure 10. Typical Nonlinearity vs. C OS


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AD650


BIPOLAR V/FFigure 11 shows how the internal bipolar current sink is used toprovide a half-scale offset for a 5 V signal range, while providinga 100 kHz maximum output frequency. The nominally 0.5 mA(10%) offset current sink is enabled when a 1.24 k resistor is

connected between Pin 4 and Pin 5. Thus, with the grounded10 k nominal resistance shown, a 5 V offset is developed atPin 2. Because Pin 3 must also be at 5 V, the current through R IN is 10 V/40 k = +0.25 mA at VIN = +5 V, and 0 mA at V IN = 5 V.

Components are selected using the same guidelines outlined forthe unipolar configuration with one alteration. The voltageacross the total signal range must be equated to the maximuminput voltage in the unipolar configuration. In other words, the value of the input resistor R IN is determined by the input voltagespan, not the maximum input voltage. A diode from Pin 1 toground is also recommended. This is further discussed in theOther Circuit Considerations section.

As in the unipolar circuit, R IN and COS must have low temperaturecoefficients to minimize the overall gain drift. The 1.24 kresistor used to activate the 0.5 mA offset current should alsohave a low temperature coefficient. The bipolar offset currenthas a temperature coefficient of approximately 200 ppm/C.

UNIPOLAR V/F, NEGATIVE INPUT VOLTAGEFigure 12 shows the connection diagram for V/F conversion of negative input voltages. In this configuration, full-scale outputfrequency occurs at negative full-scale input, and zero outputfrequency corresponds with zero input voltage.

A very high impedance signal source can be used because it only drives the noninverting integrator input. Typical input impedanceat this terminal is 1 G or higher. For V/F conversion of positiveinput signals using the connection diagram of Figure 4, thesignal generator must be able to source the integration currentto drive the AD650. For the negative V/F conversion circuit of Figure 12, the integration current is drawn from groundthrough R1 and R3, and the active input is high impedance.

Circuit operation for negative input voltages is very similar topositive input unipolar conversion described in the UnipolarConfiguration section. For best operating results use Equation 7and Equation 8 in the Component Selection section.

F/V CONVERSIONThe AD650 also makes a very linear frequency-to-voltageconverter. Figure 13 shows the connection diagram for F/Vconversion with TTL input logic levels. Each time the inputsignal crosses the comparator threshold going negative, the oneshot is activated and switches 1 mA into the integrator input fora measured time period (determined by C OS). As the frequency increases, the amount of charge injected into the integrationcapacitor increases proportionately. The voltage across theintegration capacitor is stabilized when the leakage currentthrough R1 and R3 equals the average current being switchedinto the integrator. The net result of these two effects is anaverage output voltage that is proportional to the input

frequency. Optimum performance can be obtained by selectingcomponents using the same guidelines and equations listed inthe Bipolar V/F section.

For a more complete description of this application, refer toAnalog Devices Application Note AN-279.

HIGH FREQUENCY OPERATIONProper RF techniques must be observed when operating theAD650 at or near its maximum frequency of 1 MHz. Leadlengths must be kept as short as possible, especially on the oneshot and integration capacitors, and at the integrator summing junction. In addition, at maximum output frequencies above

500 kHz, a 3.6 k pull-down resistor from Pin 1 to VS isrequired (see Figure 14). The additional current drawn throughthe pulldown resistor reduces the op amps output impedanceand improves its transient response.

0 0 7 9 7

- 0 1 2

OP

AMP

COMP

INFREQ

OUT

OUTONE

SHOT

8

9

10

11

13

12

7

6

5

4

3

2

1 14INPUT

OFFSETTRIM

0.6V

AD650

VS

VS

1mA

S1

COS330pF

15V0.1F

VIN5V

1.24k

R337.4k

10k R15k

C INT1000pF

20k

250k

0.1F

1F

1k

+15V

+5V

DIGITALGND

ANALOGGND

FOUT

Figure 11. Connections for 5 V Bipolar V/F with 0 kHz to 100 kHz TTL Output


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AD650


DECOUPLING AND GROUNDINGIt is effective engineering practice to use bypass capacitors onthe supply-voltage pins and to insert small-valued resistors(10 to 100 ) in the supply lines to provide a measure of decoupling between the various circuits in a system. Ceramic

capacitors of 0.1 F to 1.0 F should be applied between thesupply-voltage pins and analog signal ground for properbypassing on the AD650.

In addition, a larger board level decoupling capacitor of 1 F to10 F should be located relatively close to the AD650 on eachpower supply line. Such precautions are imperative in highresolution, data acquisition applications where users expect toexploit the full linearity and dynamic range of the AD650.Although some types of circuits can operate satisfactorily withpower supply decoupling at only one location on each circuitboard, such practice is strongly discouraged in high accuracy analog design.

Separate digital and analog grounds are provided on theAD650. The emitter of the open collector frequency outputtransistor is the only node returned to the digital ground. Allother signals are referred to analog ground. The purpose of thetwo separate grounds is to allow isolation between the highprecision analog signals and the digital section of the circuitry.As much as several hundred millivolts of noise can be toleratedon the digital ground without affecting the accuracy of theVFC. Such ground noise is inevitable when switching the largecurrents associated with the frequency output signal.

At 1 MHz full scale, it is necessary to use a pull-up resistor of

about 500 in order to get the rise time fast enough to providewell defined output pulses. This means that from a 5 V logicsupply, for example, the open collector output draws 10 mA.

This much current being switched causes ringing on longground runs due to the self-inductance of the wires. Forinstance, 20 gauge wire has an inductance of about 20 nH perinch; a current of 10 mA being switched in 50 ns at the end of 12 inches of 20 gauge wire produces a voltage spike of 50 mV.The separate digital ground of the AD650 easily handles thesetypes of switching transients.

A problem remains from interference caused by radiation of electromagnetic energy from these fast transients. Typically, a voltage spike is produced by inductive switching transients;these spikes can capacitively couple into other sections of thecircuit. Another problem is ringing of ground lines and powersupply lines due to the distributed capacitance and inductanceof the wires. Such ringing can also couple interference intosensitive analog circuits. The best solution to these problems isproper bypassing of the logic supply at the AD650 package. A1 F to 10 F tantalum capacitor should be connected directly

to the supply side of the pull-up resistor and to the digitalground (Pin 10). The pull-up resistor should be connecteddirectly to the frequency output (Pin 8). The lead lengths on thebypass capacitor and the pull-up resistor should be as short aspossible. The capacitor supplies (or absorbs) the currenttransients, and large ac signals flows in a physically small loopthrough the capacitor, pull-up resistor, and frequency outputtransistor. It is important that the loop be physically small fortwo reasons: first, there is less self-inductance if the wires areshort, and second, the loop does not radiate RFI efficiently.

The digital ground (Pin 10) should be separately connected tothe power supply ground. Note that the leads to the digitalpower supply are only carrying dc current and cannot radiateRFI. There can also be a dc ground drop due to the difference incurrents returned on the analog and digital grounds. This doesnot cause any problem. In fact, the AD650 tolerates as much as0.25 V dc potential difference between the analog and digitalgrounds. These features greatly ease power distribution andground management in large systems. Proper technique forgrounding requires separate digital and analog ground returnsto the power supply. Also, the signal ground must be referreddirectly to analog ground (Pin 11) at the package. All of thesignal grounds should be tied directly to Pin 11, especially theone-shot capacitor. More information on proper grounding andreduction of interference can be found in Noise ReductionTechniques in Electronic Systems, 2nd edition by Henry W. Ott,(John Wiley & Sons, Inc., 1988).

TEMPERATURE COEFFICIENTSThe drift specifications of the AD650 do not include

temperature effects of any of the supporting resistors orcapacitors. The drift of the input resistors R1 and R3 and thetiming capacitor C OS directly affect the overall temperaturestability. In the application of Figure 5, a 10 ppm/C inputresistor used with a 100 ppm/C capacitor can result in amaximum overall circuit gain drift of:

150 ppm/C (AD650A) + 100 ppm/C (COS)+ 10 ppm/C (R IN) = 260 ppm/C

In bipolar configuration, the drift of the 1.24 k resistor used toactivate the internal bipolar offset current source directly affectsthe value of this current. This resistor should be matched to theresistor connected to the op amp noninverting input, Pin 2 (seeFigure 11). That is, the temperature coefficients of these tworesistors should be equal. If this is the case, then the effects of thetemperature coefficients of the resistors cancel each other, and thedrift of the offset voltage developed at the op amp noninvertinginput is solely determined by the AD650. Under these conditions,the TC of the bipolar offset voltage is typically 200 ppm/C andis a maximum of 300 ppm/C. The offset voltage alwaysdecreases in magnitude as temperature is increased.


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AD65


Other circuit components do not directly influence the accuracy of the VFC over temperature changes as long as their actual values are not as different from the nominal value as to precludeoperation. This includes the integration capacitor C INT. A changein the capacitance value of CINT simply results in a different rate of voltage change across the capacitor. During the integration phase(see Figure 8), the rate of voltage change across CINT has theopposite effect that it does during the reset phase. The result isthat the conversion accuracy is unchanged by either drift ortolerance of CINT. The net effect of a change in the integratorcapacitor is simply to change the peak-to-peak amplitude of thesawtooth waveform at the output of the integrator.

The gain temperature coefficient of the AD650 is not a constant value. Rather, the gain TC is a function of both the full-scalefrequency and the ambient temperature. At a low full-scalefrequency, the gain TC is determined primarily by the stability of the internal reference (a buried Zener reference). This low speedgain TC can be quite effective; at 10 kHz full scale, the gain TC near25C is typically 0 50 ppm/C. Although the gain TC changeswith ambient temperature (tending to be more positive at highertemperatures), the drift remains within a 75 ppm/C window overthe entire military temperature range. At full-scale frequencieshigher than 10 kHz, dynamic errors become much more importantthan the static drift of the dc reference. At a full-scale frequency of 100 kHz and above, these timing errors dominate the gainTC. For example, at 100 kHz full-scale frequency (R IN = 40 k andCOS = 330 pF) the gain TC near room temperature is typically 80 50 ppm/C, but at an ambient temperature near 125C, thegain TC tends to be more positive and is typically 15 50 ppm/C.This information is presented in a graphical form in Figure 15.

The gain TC always tends to become more positive at highertemperatures. Therefore, it is possible to adjust the gain TC of the AD650 by using a one-shot capacitor with an appropriateTC to cancel the drift of the circuit. For example, consider the100 kHz full-scale frequency. An average drift of 100 ppm/Cmeans that as temperature is increased, the circuit produces alower frequency in response to a given input voltage. This meansthat the one-shot capacitor must decrease in value as temperatureincreases in order to compensate the gain TC of the AD650; thatis, the capacitor must have a TC of 100 ppm/C. Now considerthe 1 MHz full-scale frequency.

100

50

10kHz

100kHz

1MHz

25 0 25 50 75

100 1250

100

200

300

400

TEMPERATURE (C)

G A I N T C ( p p m

/ C )

0 0 7 9 7

- 0 1 6

Figure 15. Gain TC vs. Temperature

It is not possible to achieve much improvement in performanceunless the expected ambient temperature range is known. Forexample, in a constant low temperature application such asgathering data in an Arctic climate (approximately 20C), aCOS with a drift of 310 ppm/C is called for in order to compensatethe gain drift of the AD650. However, if that circuit should seean ambient temperature of 75C, then the C OS capacitor wouldchange the gain TC from approximately 0 ppm to 310 ppm/C.

The temperature effects of these components are the same whenthe AD650 is configured for negative or bipolar input voltages,and for F/V conversion as well.

NONLINEARITY SPECIFICATIONThe linearity error of the AD650 is specified by the endpointmethod. That is, the error is expressed in terms of the deviationfrom the ideal voltage to frequency transfer relation aftercalibrating the converter at full scale and zero. The nonlinearity varies with the choice of one-shot capacitor and input resistor(see Figure 10). Verification of the linearity specificationrequires the availability of a switchable voltage source (or aDAC) having a linearity error below 20 ppm, and the use of very long measurement intervals to minimize countuncertainties. Every AD650 is automatically tested for linearity,and it is not usually necessary to perform this verification,which is both tedious and time consuming. If it is required toperform a nonlinearity test either as part of an incoming quality screening or as a final product evaluation, an automated bench-top tester proves useful. Such a system based on AnalogDevices LTS-2010 is described in V-F Converters DemandAccurate Linearity Testing, by L. DeVito, (Electronic Design,

March 4, 1982).The voltage-to-frequency transfer relation is shown in Figure 16and Figure 17 with the nonlinearity exaggerated for clarity. Thefirst step in determining nonlinearity is to connect the endpoints of the operating range (typically at 10 mV and 10 V) with a straightline. This straight line is then the ideal relationship that is desiredfrom the circuit. The second step is to find the difference betweenthis line and the actual response of the circuit at a few pointsbetween the endpointstypically ten intermediate pointssuffices. The difference between the actual and the idealresponse is a frequency error measured in hertz. Finally, thesefrequency errors are normalized to the full-scale frequency and

expressed either as parts per million of full scale (ppm) or partsper hundred of full scale (%). For example, on a 100 kHz fullscale, if the maximum frequency error is 5 Hz, the nonlinearity is specified as 50 ppm or 0.005%. Typically on the 100 kHzscale, the nonlinearity is positive and the maximum valueoccurs at about midscale (Figure 16). At higher full-scalefrequencies, (500 kHz to 1 MHz), the nonlinearity becomes Sshaped and the maximum value can be either positive or negative.Typically, on the 1 MHz scale (R IN = 16.9 k, COS = 51 pF) thenonlinearity is positive below about 2/3 scale and is negativeabove this point. This is shown graphically in Figure 17.


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AD650


100k

100

10mV

ACTUAL

IDEAL50ppm

10VINPUT VOLTAGE

O U T P U T F R E Q

U E N C Y ( H z )

0 0 7 9 7

- 0 1 7

Figure 16. Exaggerated Nonlinearity at 100 kHz Full Scale

1M

1k

10mV

ACTUALVOLTAGE TO FREQUENCY

TRANSFER RELATION

IDEAL RELATION600ppm

10VINPUT VOLTAGE

O U T P U T F R E Q U E N C Y ( H z

)

600ppm

0 0 7 9 7

- 0 1 8

Figure 17. Exaggerated Nonlinearity at 1 MHz Full Scale

1k

10

FULL SCALE FREQUENCY (Hz)

P S R R ( p p m

/ % )

100

10k 100k 1M 0 0 7 9 7

- 0 1 9

Figure 18. PSRR vs. Full-Scale Frequency

PSRRThe power supply rejection ratio is a specification of the changein gain of the AD650 as the power supply voltage is changed.The PSRR is expressed in units of parts-per-million change of the gain per percent change of the power supply (ppm/%). For

example, consider a VFC with a 10 V input applied and anoutput frequency of exactly 100 kHz when the power supply potential is 15 V. Changing the power supply to 12.5 V is a5 V change out of 30 V, or 16.7%. If the output frequency changesto 99.9 kHz, then the gain has changed 0.1% or 1000 ppm. ThePSRR is 1000 ppm divided by 16.7%, which equals 60 ppm/%.

The PSRR of the AD650 is a function of the full-scale operatingfrequency. At low full-scale frequencies the PSRR is determinedby the stability of the reference circuits in the device and can be very effective. At higher frequencies, there are dynamic errorsthat become more important than the static reference signals,and consequently the PSRR is not quite as effective. The values

of PSRR are typically 0 20 ppm/% at 10 kHz full-scale frequency (R IN = 40 k, COS = 3300 pF). At 100 kHz (R IN = 40 k, COS =330 pF) the PSRR is typically +80 40 ppm/%, and at 1 MHz(R IN = 16.9 k, COS = 51 pF) the PSRR is +350 50 ppm/%.This information is summarized graphically in Figure 18.

OTHER CIRCUIT CONSIDERATIONSThe input amplifier connected to Pin 1, Pin 2, and Pin 3 is not astandard operational amplifier. Rather, the design has beenoptimized for simplicity and high speed. The single largestdifference between this amplifier and a normal op amp is the lack of an integrator (or level shift) stage. Consequently, the voltage onthe output (Pin 1) must always be more positive than 2 V below theinputs (Pin 2 and Pin 3). For example, in the F-to-V conversionmode (Figure 13) the noninverting input of the op amp (Pin 2)is grounded, which means that the output (Pin 1) is not able togo below 2 V. Normal operation of the circuit shown in Figure 13 never calls for a negative voltage at the output, but users canimagine an arrangement calling for a bipolar output voltage (forexample, 10 V) by connecting an extra resistor from Pin 3 to apositive voltage. However, this does not work.

Care should be taken under conditions where a high positiveinput voltage exists at or before power up. These situations cancause a latch up at the integrator output (Pin 1). This is anondestructive latch and, as such, normal operation can berestored by cycling the power supply. Latch up can be preventedby connecting two diodes (for example, 1N914 or 1N4148) asshown in Figure 11, thereby preventing Pin 1 from swingingbelow Pin 2.


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AD65


A second major difference is that the output only sinks 1 mA tothe negative supply. There is no pulldown stage at the outputother than the 1 mA current source used for the V-to-Fconversion. The op amp sources a great deal of current from thepositive supply, and it is internally protected by current limiting.The output of the op amp can be driven to within 3 V of thepositive supply when it is not sourcing external current. Whensourcing 10 mA the output voltage can be driven to within 6 Vof the positive supply.

A third difference between this op amp and a normal device isthat the inverting input, Pin 3, is bias current compensated andthe noninverting input is not bias-current compensated. Thebias current at the inverting input is nominally zero, but can beas much as 20 nA in either direction. The noninverting inputtypically has a bias current of 40 nA that always flows into thenode (an npn input transistor). Therefore, it is not possible tomatch input voltage drops due to bias currents by matchinginput resistors.

The op amp has provisions for trimming the input offset voltage. A potentiometer of 20 k is connected from Pin 13 toPin 14 and the wiper is connected to the positive supply through a 250 k resistor. A potential of about 0.6 V isestablished across the 250 k resistor, and the 3 A current isinjected into the null pins. It is also possible to null the op ampoffset voltage by using only one of the null pins and by using abipolar current either into or out of the null pin. The amount of current required is very smalltypically less than 3 A. Thistechnique is shown in the Applications section of this datasheet; the autozero circuit uses this technique.

The bipolar offset current is activated by connecting a 1.24 kresistor between Pin 4 and the negative supply. The resultingcurrent delivered to the op amp noninverting input is nominally 0.5 mA and has a tolerance of 10%. This current is then usedto provide an offset voltage when Pin 2 is tied to ground througha resistor. The 0.5 mA that appears at Pin 2 is also flowingthrough the 1.24 k resistor. An external resistor is used toactivate the bipolar offset current source to provide the lowesttolerance and temperature drift of the resulting offset voltage.It is possible to use other values of resistance between Pin 4 andVS to obtain a bipolar offset current different from 0.5 mA.Figure 19 shows the relationship between the bipolar offsetcurrent and the value of the resistor used to activate the source.

A

200

500 4000EXTERNAL RESISTOR

B I P O L A R O F F S E T C U R R E N T

400

600

800

1000

1000 1500 2000 2500 3000 3500 0 0 7 9 7

- 0 2 0

Figure 19. Bipolar Offset Current vs. External Resistor


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AD650


APPLICATIONSDIFFERENTIAL VOLTAGE-TO-FREQUENCYCONVERSIONThe circuit in Figure 20 accepts a true floating differential input

signal. The common-mode input, V CM, can be in the range+15 V to 5 V with respect to analog ground. The signal input,VIN, can be 5 V with respect to the common-mode input. Bothinputs are low impedance; the source that drives the common-mode input must supply the 0.5 mA drawn by the bipolar offsetcurrent source, and the source that drives the signal input mustsupply the integration current.

If less common-mode voltage range is required, then a lower voltage Zener can be used. For example, if a 5 V Zener is used,the VCM input can be in the range +10 V to 5 V. If the Zener isnot used at all, the common-mode range is 5 V with respect toanalog ground. If no Zener is used, the 10 k pulldown resistor

is not needed and the integrator output (Pin 1) is connecteddirectly to the comparator input (Pin 9).

AUTOZERO CIRCUITIn order to exploit the full dynamic range of the AD650 VFC, very small input voltages need to be converted. For example, asix decade dynamic range based on a full scale of 10 V requiresaccurate measurement of signals down to 10 V. In thesesituations, a well-controlled input offset voltage is imperative. Aconstant offset voltage does not affect dynamic range but simply shifts all of the frequency readings by a few hertz. However, if the offset should change, it is not possible to distinguishbetween a small change in a small input voltage and a drift of the offset voltage. Therefore, the usable dynamic range is less.The circuit shown in Figure 21 provides automatic adjustmentof the op amp offset voltage. The circuit uses an AD582 sample-

and-hold amplifier to control the offset, and the input voltage tothe VFC is switched between ground and the signal to bemeasured via an AD7512DI analog switch. The offset of theAD650 is adjusted by injecting a current intoor drawing a

current out ofPin 13. Note that only one of the offset null pinsis used. During the VFC norm mode, the SHA is in the holdmode and the hold capacitor is very large, 0.1 F, which holdsthe AD650 offset constant for a long period of time.

When the circuit is in the autozero mode, the SHA is in samplemode and behaves like an op amp. The circuit is a variation of the classical two amplifier servo loop, where the output of thedevice under test (DUT)here the DUT is the AD650 opampis forced to ground by the feedback action of the controlamplifierthe SHA. Because the input of the VFC circuit isconnected to ground during the autozero mode, the inputcurrent that can flow is determined by the offset voltage of theAD650 op amp. Because the output of the integrator stage isforced to ground, it is known that the voltage is not changing (itis equal to ground potential). Therefore, if the output of theintegrator is constant, its input current must be zero, so theoffset voltage has been forced to be zero. Note that the output of the DUT could have been forced to any convenient voltageother than ground. All that is required is that the output voltagebe known to be constant. Note also that the effect of the biascurrent at the inverting input of the AD650 op amp is alsomulled in this circuit. The 1000 pF capacitor shunting the200 k resistor is compensation for the two amplifier servoloop. Two integrators in a loop require a single zero forcompensation. The 3.6 k resistor from Pin 1 of the AD650 tothe negative supply is not part of the autozero circuit, but rather,it is required for VFC operation at 1 MHz.

0 0 7 9 7

- 0 2 1

OPAMP

COMP

INFREQ

OUT

OUTONE

SHOT

8

9

10

11

13

12

7

6

5

4

3

2

1 14INPUT

OFFSETTRIM

10V ZENER 1N5240

NOTES1. V CM IS THE COMMON MODE INPUT +15V TO 5V WITH RESPECT TO ANALOG GROUND.2. V IN IS THE SIGNAL INPUT 5V WITH RESPECT TO V CM.

0.6V

AD650

VS

VIN

VCM

INPUT

V S

1mA

S1

20k

250k

0.1F

1F

+15V

GND

GND

FREQUENCYOUTPUT

0kHz TO 100kHz

15V

+5V

+

+

0.1F

+

1k

10k

COS330pF

C I1000pF

1.24k

40k

10k

Figure 20. Differential Input
http://www.analog.com/en/prod/0,2877,AD7512,00.htmlhttp://www.analog.com/en/prod/0,2877,AD7512,00.html


17/20


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AD650


In signal recovery applications of a PLL, the desired outputsignal is the voltage applied to the oscillator. In these situations,a linear relationship between the input frequency and theoutput voltage is desired; the AD650 makes a superb oscillatorfor FM demodulation. The wide dynamic range and

outstanding linearity of the AD650 VFC allow simpleembodiment of high performance analog signal isolation ortelemetry systems. The circuit shown in Figure 22 uses a digitalphase detector that also provides proper feedback in the eventof unequal frequencies. Such phase-frequency detectors (PFDs)are available in integrated form. For a full discussion of phase-lock loop circuits see Phase Lock Techniques, 3rd Edition, by F.M. Gardner, (John Wiley & Sons, Inc., 1979).

An analysis of this circuit must begin at the 7474 Dual D f lipflop. When the input carrier matches the output carrier in bothphase and frequency, the Q outputs of the flip flops rise atexactly the same time. With two zeros, and then two ones on

the inputs of the exclusive or (XOR) gate, the output remainslow keeping the DMOS FET switched off. Also, the NAND gategoes low resetting the flip-flops to zero. Throughout this entirecycle, the DMOS integrator gate remains off, allowing the voltage at the integrator output to remain unchanged from theprevious cycle. However, if the input carrier leads the outputcarrier by a few degrees, the XOR gate is turned on for the shorttime span that the two signals are mismatched. Because Q2 islow during the mismatch time, a negative current is fed into theintegrator, causing its output voltage to rise. This in turnincreases the frequency of the AD650 slightly, driving thesystem towards synchronization. In a similar manner, if theinput carrier lags the output carrier, the integrator is forceddown slightly to synchronize the two signals.

Using a mathematical approach, the 25 A pulses from thephase detector are incorporated into the phase-detector gain (K d).

radian/amperes1042A25 6=

=d K (9)

Also, the V/F converter is configured to produce 1 MHz inresponse to a 10 V input so its gain (Ko) is

sec voltradians103.6

V10Hz1012 5

6

=

=OK (10)

The dynamics of the phase relationship between the input andoutput signals can be characterized as a second order systemwith natural frequency ( n).

C K K d o

n = (11)

and damping factor () is

2d oK CK R= (12)

For the values shown in Figure 22, these relations simplify to anatural frequency of 35 kHz with a damping factor of 0.8.

For a simple approach to determine component values for otherPLL frequencies and VFC full-scale voltage, follow these steps:

1. Determine Ko (in units of radians per volt second) from themaximum input carrier frequency f MAX (in hertz) and themaximum output voltage V MAX.

MAX

MAX o V

F K

= 2 (13)

2. Calculate a value for C based upon the desired loopbandwidth f n. Note that this is the desired frequency rangeof the output signal. The loop bandwidth (f n) is not themaximum carrier frequency (f MAX). The signal can be very narrow even though it is transmitted over a 1 MHz carrier.

secRad101 72

= F V f K

C n

o (14)

where: C units = farads f n units = hertzK o units = rad/volt sec

3. Calculate R to yield a damping factor of approximately 0.8using this equation:

V K f

Ro

n = Rad105.2 6 (15)

where: R units = ohms f n units = hertzK o units = rad/volt sec

If in actual operation the PLL overshoots or hunts excessively before reaching a final value, the damping factor can be raisedby increasing the value of R. Conversely, if the PLL isoverdamped, a smaller value of R should be used.


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AD65


OUTLINE DIMENSIONS

CONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FORREFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN.

14

17

80.310 (7.87)0.220 (5.59)

PIN 1

0.080 (2.03) MAX0.005 (0.13) MIN

SEATINGPLANE

0.023 (0.58)0.014 (0.36)

0.060 (1.52)0.015 (0.38)

0.200 (5.08)MAX

0.200 (5.08)0.125 (3.18) 0.070 (1.78)

0.030 (0.76)

0.100 (2.54)BSC

0.150(3.81)MIN

0.765 (19.43) MAX

0.320 (8.13)0.290 (7.37)

0.015 (0.38)0.008 (0.20)

Figure 23. 14-Lead Side-Brazed Ceramic Dual In-Line Package [SBDIP]

(D-14)Dimensions shown in inches and (millimeters)

COMPLIANT TO JEDEC STANDARDS MS-001-AACONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FORREFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN.CORNER LEADS MAY BE CONFIGURED AS WHOLE OR HALF LEADS.

0.022 (0.56)0.018 (0.46)0.014 (0.36)

0.150 (3.81)0.130 (3.30)

0.110 (2.79)

0.070 (1.78)0.050 (1.27)0.045 (1.14)

14

1 7

8

0.100 (2.54)BSC

0.775 (19.69)0.750 (19.05)0.735 (18.67)

PIN 1

0.060 (1.52)MAX

0.430 (10.92)MAX

0.014 (0.36)0.010 (0.25)0.008 (0.20)

0.325 (8.26)0.310 (7.87)0.300 (7.62)

0.015 (0.38)GAUGEPLANE

0.210(5.33)MAX

SEATINGPLANE

0.015(0.38)MIN

0.005 (0.13)MIN

0.280 (7.11)0.250 (6.35)0.240 (6.10)

0.195 (4.95)0.130 (3.30)0.115 (2.92)

Figure 24. 14-Lead Plastic Dual In-Line Package [PDIP]

(N-14)Dimensions shown in inches and (millimeters)


20/20

AD650

COMPLIANT TO JEDEC STANDARDS MO-047-AACONTROLLING DIMENSIONS ARE IN INCHES; MILLIMETER DIMENSIONS(IN PARENTHESES) ARE ROUNDED-OFF INCH EQUIVALENTS FORREFERENCE ONLY AND ARE NOT APPROPRIATE FOR USE IN DESIGN.

0.020 (0.50)R

BOTTOMVIEW

(PINS UP)

0.021 (0.53)0.013 (0.33)

0.330 (8.38)0.290 (7.37)0.032 (0.81)

0.026 (0.66)

0.056 (1.42)0.042 (1.07)

0.20 (0.51)MIN

0.120 (3.04)0.090 (2.29)

3

4

19

18

89

1413

TOP VIEW(PINS DOWN)

0.395 (10.03)0.385 (9.78)

SQ

0.356 (9.04)0.350 (8.89)

SQ

0.048 (1.22 )0.042 (1.07)

0.048 (1.22)0.042 (1.07)

0.020(0.51)

R

0.050(1.27)BSC

0.180 (4.57)0.165 (4.19)

0.045 (1.14)0.025 (0.64)

R

PIN 1IDENTIFIER

Figure 25. 20-Lead Plastic Leaded Chip Carrier [PLCC]

(P-20A)Dimensions shown in inches and (millimeters)

ORDERING GUIDE

Model

Gain Tempcoppm/C100 kHz

1 MHzLinearity

TemperatureRange Package Description

PackageOption

AD650JN 150 typ 0.1% typ 0C to 70C 14-Lead Plastic Dual In-Line Package [PDIP] N-14AD650JNZ1 150 typ 0.1% typ 0C to 70C 14-Lead Plastic Dual In-Line Package [PDIP] N-14AD650KN 150 typ 0.1% max 0C to 70C 14-Lead Plastic Dual In-Line Package [PDIP] N-14AD650KNZ1 150 typ 0.1% max 0C to 70C 14-Lead Plastic Dual In-Line Package [PDIP] N-14AD650JP 150 typ 0.1% typ 0C to 70C 20-Lead Plastic Leaded Chip Carrier [PLCC] P-20AAD650JPZ1 150 typ 0.1% typ 0C to 70C 20-Lead Plastic Leaded Chip Carrier [PLCC] P-20AAD650AD 150 max 0.1% typ 25C to +85C 14-Lead Side-Brazed Ceramic Dual In-Line Package [SBDIP] D-14AD650BD 150 max 0.1% max 25C to +85C 14-Lead Side-Brazed Ceramic Dual In-Line Package [SBDIP] D-14AD650SD 200 max 0.1% max 55C to +125C 14-Lead Side-Brazed Ceramic Dual In-Line Package [SBDIP] D-14

AD650SD/883B 200 max 0.1% max 55C to +125C 14-Lead Side-Brazed Ceramic Dual In-Line Package [SBDIP] D-14AD650ACHIPS Die

1 Z = Pb-free part.

2006 Analog Devices, Inc. All rights reserved. Trademarks andregistered trademarks are the property of their respective owners.

C00797-0-3/06(D)

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AD650 Freq to Voltage