Analog Devices AN-411 Application Notes

AN-411

6

8

9

10

2

3

5

0.022µF

C2

ADXL05

PRE-AMP

0.022µF

COM

C1

C1

V

PR

+1.8V

BUFFER

AMP

+5VDC

C3

0.1µF

V

ACCEL

R1

R2

C5

V

IN–

R3

4

1

1

2

4

5

6

7

8

R

T

R

T

LOGIC

COM

F

OUT

R5
1kΩ to 10kΩ

FREQUENCY
OUTPUT

+V

S

+V

S

C4

0.1µF

C

T

C

T

C

T

–V

S

+V

IN

DRIVER

OSC

AD654

3

0g FREQ SF CTR1 R2 R3
Hz Hz/

g

µF kΩ kΩ kΩ

10 10 10 14.7 464 182
100 10 1 40.2 127 49.9
100 100 1 14.7 464 182
1000 10 0.1 133 42.2 16.5
1000 100 0.1 40.2 127 49.9
1000 1000 0.1 14.7 464 182
10,000 10 0.01 1370 43.2 16.9
10,000 100 0.01 137 43.2 16.9
10,000 1000 0.01 40.2 127 49.9
100,000 10 0.001 137 0.43 0.169
100,000 100 0.001 137 4.32 1.69
100,000 1000 0.001 137 43.2 16.9

DESIGN EQUATIONS

0.25

RT C

T

0g FREQUENCY =

R2 FOR A +2.5V 0

g

LEVEL = 2.57 R3

SCALE FACTOR (Hz/

g

) = =

∆ FREQ

g

200 R3

1000 R1 RT C

T

3dB ACCELERATION BW =

1

2π R3 C5

IN4733

R

S

+V

S

+5VDC TO
PIN 1
ADXL05

+V

S

+VSR

S

+12V 432Ω
+9V 249Ω

a

ONE TECHNOLOGY WAY • P.O. BOX 9106

Acceleration to Frequency Circuits

by Charles Kitchin, Dave Quinn, and Steve Sherman

INTRODUCTION

Low cost monolithic accelerometers may be paired with
a circuit whose output changes with frequency (V/F) to
provide a TTL level frequency output. A microprocessor
can be easily programmed to read this signal and
directly compute the applied acceleration, and the out­put of a V/F circuit can be sent down a long transmission
line and still be reliably recovered at the other end.

A High Performance Acceleration-to-Frequency Circuit

A circuit whose output frequency varies directly with
applied acceleration is shown in Figure 1. The circuit
operates from a single +9 V or +12 V power supply.

•

NORWOOD, MASSACHUSETTS 02062-9106

APPLICATION NOTE

617/329-4700

•

An ADXL05, ±5 g accelerometer directly converts any
applied acceleration into an analog output voltage
which then controls the output frequency of an AD654
low cost voltage-to-frequency converter IC. The fre­quency output appears at Pin 1 of the AD654. Total chip
cost for this circuit is approximately $20.00 (in 1000s).

The voltage output at Pin 8 of the ADXL05 is +2.5 volts
with no acceleration and varies 200 mV above or below
that value for each 1
acceleration.

g

(positive or negative) of applied

Figure 1. A High Performance Acceleration-to-Frequency Circuit

The output scale factor of the accelerometer (at Pin 9) is
set by the resistors R3 & R1 of the on-chip buffer ampli­fier. Resistor R2 is used to change the 0

g

output level to
a convenient +2.5 V (which provides the maximum out­put voltage swing). Capacitor C5 and Resistor R3 form a
low-pass filter which improves the circuit’s signal-to­noise ratio.

Figure 2 shows the same circuit modified for use with
the ADXL50, a ±50

g

accelerometer. The accelerometer’s
3 dB bandwidth is again set by R3 & C5. In Figure 2, both
a zero

g

offset and a scale factor trim potentiometer
have been added to allow the user to adjust the circuit to
extremely high accuracy; trim potentiometers may also
be added to the circuit of Figure 1. R1a should be ap­proximately 50% the value of R1b (for a ±20% trim
range). Note: for the best mechanical stability the trim
potentiometers should be measured (after calibration is
complete) and replaced with 1% resistors.

Design example: Circuit of Figure 2

Design example: Wanted . . . 0
Scale Factor = 100 Hz/

g

, BW = 200 Hz.

g

frequency = 10 kHz,

A 50 g signal will cause a frequency variation of 5 kHz.

Therefore:

F

for

±50

OUT

Let

C

gs = 10 kHz ± 5 kHz = 5 kHz – 15 kHz

= 0.01 µF, then for a 0 g frequency of 10 kHz:

T

R

0.25

=

T

kHz C

10

=2.5kΩ

T

Let R3 = 49.9 kΩ, for a scale factor of 100 Hz/g:

mV/g×R

100

19

Hz/g

10,000

R

1=

3

RTC

=52.7kΩ

T

For R1, use a 42.2 kΩ fixed resistor & a 20 kΩ trim
potentiometer.

For a 200 Hz bandwidth:

C

5 =

1

2π 200

R

3

= 0.016 µ

F

The accelerometer may be self-calibrated by using the
Earth’s gravity. With the accelerometer’s tab pointed
90° to the vertical (i.e., to either side), the accelerometer
will measure 0

g

, allowing the 0 g offset to be adjusted.
With the accelerometer’s tab pointing down, its output
at Pin 9 will correspond to +1
rotated 180° it will then measure –1

g

. If the accelerometer is

g

. The 2 g difference

in the readings can then be used to set the circuit’s over-

DESIGN EQUATIONS

∆ FREQ

g

0.022µF

COM

OPTIONAL

0

C2

C1

C1

g

LEVEL

0.25

RT C

+3.4V

TRIM

0g FREQUENCY =

SCALE FACTOR (Hz/g) = =

3dB ACCELERATION BW =

0.022µF

T

1000 R1 RT C

2π R3 C5

4

2

3

5

6

REF

19 R3

1

R4
50kΩ

TRIM

T

ADXL50

PRE-AMP

V

PR

8

SF

0g FREQ SF CTR1a R1b R2 R3
Hz Hz/
10 10 10 5 12.1 100 2MΩ
100 10 1 10 34.8 100 499
100 100 1 5 12.1 100 2MΩ
1000 10 0.1 50 107 100 165
1000 100 0.1 10 34.8 100 499
1000 1000 0.1 5 12.1 100 2MΩ
10,000 10 0.01 500 1MΩ 100 169
10,000 100 0.01 50 107 100 169
10,000 1000 0.01 10 34.8 100 499
100,000 10 0.001 50 107 100 1.69
100,000 100 0.001 50 107 100 16.9
100,000 1000 0.001 50 107 100 169

R1a

100kΩ

R2

R1b

+1.8V

10

g

µF kΩ kΩ kΩ kΩ

1

BUFFER

AMP

9

V

IN–

R3

R2

C5

V

LOW-PASS
FILTERING

+5VDC

C3

0.1µF

ACCEL

+V

S

R5
1kΩ to 10kΩ

F

OUT

LOGIC

COM

R

T

5.9kΩ

+V

R

S

+V

S

IN4733

1

2

R

IN

AD654

T

3

4

FREQUENCY
OUTPUT

DRIVER

+5VDC TO
PIN 1
ADXL50

+V

SRS

+12V 348Ω
+9V 200Ω

OSC

+V

S

+V

S

8

C4

0.1µF

C

T

7

C

T

0.1µF

6

C

T

–V

S

5

Figure 2. A ±50 g Acceleration-to-Frequency Circuit

–2–