ETC 1010L-050

SILICON DESIGNS, INC
! SENSOR: Capacitive Micromachined
Nitrogen Damped
Hermetically Sealed
! Digital Pulse Density Output
! Fully Calibrated
! Responds to DC & AC Acceleration
! -55 to +125 EC Operation
! +5 VDC, 2 mA Power (typical)
! Non-Standard g Ranges Available
! Integrated Sensor & Amplifier
! LCC or J-Lead Surface
Mount Package
! Serialized for Traceability
! TTL/CMOS Compatible
! No External Reference Voltage
! Easy Interface to Microprocessors
! Good EMI Resistance
! RoHS Compliant
Model 1010
DIGITAL ACCELEROMETER
ORDERING INFORMATION
Full Scale
Acceleration
±2 g
±5 g
±10 g
±25 g
±50 g
±100 g
±200 g
Hermetic Packages
20 pin LCC
20 pin JLCC
1010L-002
1010J-002
1010L-005
1010J-005
1010L-010
1010J-010
1010L-025
1010J-025
1010L-050
1010J-050
1010L-100
1010J-100
1010L-200
1010J-200
DESCRIPTION
The Model 1010 is a low-cost, integrated accelerometer for use in zero to medium frequency instrumentation
applications. Each miniature, hermetically sealed package combines a micro-machined capacitive sense element
and a custom integrated circuit that includes a sense amplifier and sigma-delta A/D converter. It is relatively
insensitive to temperature changes and gradients. Each device is marked with a serial number on its bottom surface
for traceability. An optional calibration test sheet (1010-TST) is also available which lists the measured bias, scale
factor, linearity, operating current and frequency response.
OPERATION
The Model 1010 produces a digital pulse train in which the density of pulses (number of pulses per second) is
proportional to applied acceleration. It requires a single +5 volt power supply and a TTL/CMOS level clock of 100kHz1MHz. The output is ratiometric to the clock frequency and independent of the power supply voltage. Two forms of
digital signals are provided for direct interfacing to a microprocessor or counter. The sensitive axis is perpendicular
to the bottom of the package, with positive acceleration defined as a force pushing on the bottom of the package.
External digital line drivers can be used to drive long cables or when used in an electrically noisy environment.
APPLICATIONS
COMMERCIAL
! Automotive
Air Bags
Active Suspension
Adaptive Brakes
Security Systems
! Shipping Recorders
! Appliances
INDUSTRIAL
! Vibration Monitoring
! Vibration Analysis
! Machine Control
! Modal Analysis
! Robotics
! Crash Testing
! Instrumentation
Silicon Designs, Inc. ! 1445 NW Mall Street, Issaquah, WA 98027-5344 ! Phone: 425-391-8329 ! Fax: 425-391-0446
web site: www.silicondesigns.com
[page 1]
Mar 07
Model 1010 Digital Accelerometer
SIGNAL DESCRIPTIONS
VDD and GND (power): Pin 14 (VDD) & pin 19 (GND). Additionally tie pins 3 & 11 to VDD & pins 2, 5, 6 & 18 to GND.
CLK (input): Pin 8. Reference clock input. This hysteresis threshold input must be driven by a 50% duty cycle square wave
signal. Factory Calibration is performed at 250 kHz which is the recommended clock frequency for best results. Operation
at frequencies as low as 100 kHz or as high as 1 MHz are possible, however a slight bias shift may result.
CNT (output): Pin 10. Count output. A return-to-zero type digital
pulse stream whose pulse width is equal to the input CLK logic
high time. The CNT pulse rate increases with positive
acceleration.
The device experiences positive (+1g)
acceleration with its lid facing up in the earth’s gravitational
field. ___
This signal is meant to drive an up-counter directly.
DIR and DIR (output): Pins 12 & 16 respectively. Direction output. This output is updated at the fall of each clock cycle. It is
high during clock cycles when a high going CNT pulse is present and low during cycles when no CNT pulse is present. A
non-return-to-zero signal meant to control the count direction
(i.e. up or down) of a counter. DIR can be low pass filtered
___
to produce an analog measure of the acceleration. DIR is the complement of DIR and is provided for use in driving
differential transmission lines.
DV (input): Pin 4. Deflection Voltage. Normally left open. A test input that applies an electrostatic force to the sense element,
simulating a positive acceleration. The nominal voltage at this pin is aVDD. DV voltages higher than required to bring the
output to positive full scale may cause device damage.
VR (input): Pin 3. Voltage Reference. Tie directly to VDD (+5V). A 0.1µF bypass capacitor is recommended at this pin.
CLK/2 (output): Pin 15. Clock divided by 2. A buffered clock output whose frequency equals CLK divided by 2.
PERFORMANCE - by Model: VDD=VR=5.0 VDC, FCLK=250kHz, TC=25EC.
MODEL NUMBER
Input Range
Frequency Response (Nominal, 3 dB)
Sensitivity (FCLK=250kHz)
Max. Mechanical Shock (0.1 ms)
1010x-002 1010x-005 1010x-010 1010x-025 1010x-050 1010x-100 1010x-200
±2
±5
±10
±25
±50
±100
±200
0 - 400
0 - 600 0 - 1000 0 - 1400 0 - 1600 0 - 1800 0 - 2000
62.5
25.0
12.5
5.00
2.50
1.25
0.625
2000
5000
UNITS
g
Hz
kHz/g
g
PERFORMANCE - all Models: Unless otherwise specified VDD=VR=5.0 VDC, FCLK=250kHz, TC=25EC.
PARAMETER
Cross Axis Sensitivity
Bias Calibration Error
1
MIN
-002
-005 thru -200
-002
-005 thru -200
Bias Temperature Shift
(TC= -55 to +125EC) 1
Scale Factor Calibration Error 1, 2
Scale Factor Temperature Shift (TC= -55 to +125EC) 1
Non-Linearity
-002 thru -100
(-90 to +90% of Full Scale) 1, 2
-200
Power Supply Rejection Ratio (VDD=VR)
Operating Voltage (VDD vs GND)
Operating Current (IDD+IVR) 1
Clock Input Voltage Range (with respect to GND)
Mass: ‘L’ package (add 0.06 grams for ‘J’ package)
Note 1: Tighter tolerances available on special order.
40
4.5
TYP
2
2
1
150
100
1
+300
MAX
3
4
2
400
300
2
UNITS
%
% of FCLK (span)
0.5
0.7
1.0
1.5
% of span
5.0
2
5.5
3
(ppm of FCLK)/EC
%
ppm/EC
dB
Volts
mA
-0.5
VDD+0.5
Volts
0.62
grams
Note 2: 100g and greater versions are tested from -65 to +65g.
SPECIFICATIONS SUBJECT TO CHANGE WITHOUT NOTICE
Silicon Designs, Inc. ! 1445 NW Mall Street, Issaquah, WA 98027-5344 ! Phone: 425-391-8329 ! Fax: 425-391-0446
web site: www.silicondesigns.com
[page 2]
Mar 07
Model 1010 Digital Accelerometer
ABSOLUTE MAXIMUM RATINGS *
Case Operating Temperature . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . -55 to +125EC
Storage Temperature . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . -55 to +125EC
Acceleration Over-range . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2000g for 0.1 ms
Voltage on VDD to GND . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . -0.5V to 6.5V
Voltage on Any Pin (except DV) to GND 4 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . -0.5V to VDD+0.5V
Voltage on DV to GND 5 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ±15V
Power Dissipation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 50 mW
Note 4: Voltages on pins other than DV, GND or VDD may exceed 0.5 volt above or below the supply voltages provided the current is limited to 1 mA.
Note 5: The application of DV voltages higher than required to bring the output to positive full scale may cause device damage.
* NOTICE: Stresses greater than those listed above may cause permanent damage to the device. These are stress ratings only.
Functional operation of the device at or above these conditions is not implied. Exposure to absolute maximum rating conditions
for extended periods may affect device reliability.
D.C. CHARACTERISTICS: VDD=VR=5.0 VDC, TC= -55 to +125EC.
SYMBOL
VTVT+
VH
VOL
VOH
II
CIO
IDD+IVR
PARAMETER
Negative Going Threshold Voltage (CLK)
Positive Going Threshold Voltage (CLK)
Hysteresis Voltage (CLK)
Output Low Voltage (CNT, DIR, CLK/2)
Output High Voltage (CNT, DIR, CLK/2)
Input Leakage Current (CLK)
Pin Capacitance
Operating Current
MIN
0.9
TYP
1.7
3.0
1.3
0.5
MAX
3.7
0.4
VDD - 0.4
2
10
10
3
UNITS
V
V
V
V
V
µA
pF
mA
TEST CONDITIONS
IOL = 2.0 mA
IOH = 2.0 mA
VI = 0 to VDD
1 MHz, TA = 25EC
FCLK = 250kHz
A.C. CHARACTERISTICS: VDD=VR=5.0 VDC, TC= -55 to +125EC, Load Capacitance=50pF.
PARAMETER
CLK input frequency
CLK input rise/fall time
CLK duty cycle
CLK fall to DIR fall
CLK fall to DIR rise
CLK rise to valid CNT out
CLK fall to CNT fall
CLK fall to CLK/2 rise/fall
MIN
100
TYP
250
45
40
40
40
40
40
50
85
90
90
85
90
MAX
1000
50
55
195
205
230
205
210
UNITS
kHz
ns
%
ns
ns
ns
ns
ns
+5V
11
100 kHz to 1 MHz
8
14
VDD
3
VR
CLK
1010x-xxx
TEST INPUT
4
0.1 uF
16
DIR
12
DIR
CNT
DV
CLK/2
2
GND
5
19
6
10
15
COMPLEMENT OF DIR
TO PULSE COUNTER
CLOCK ÷ 2
18
RECOMMENDED CONNECTIONS
PINOUT
(LCC & JLCC)
SPECIFICATIONS SUBJECT TO CHANGE WITHOUT NOTICE
Silicon Designs, Inc. ! 1445 NW Mall Street, Issaquah, WA 98027-5344 ! Phone: 425-391-8329 ! Fax: 425-391-0446
web site: www.silicondesigns.com
[page 3]
Mar 07
Model 1010 Digital Accelerometer
USING THE COUNT (CNT) OUTPUT: Pulses from the CNT output are meant to be accumulated in a hardware counter. Each
pulse accumulation or sample, reflects the average acceleration (change in velocity) over that interval. The sample period or
“gate time” over which these pulses are accumulated determines both the bandwidth and quantization of the measurement.
Quantization (g' s) =
g SPAN • f SR
fCLK
 1 g FORCE 

f CNT = f CLK  +
 2 g SPAN 
 f
1
g FORCE = g SPAN  CNT − 
 f CLK 2 
Where:
gSPAN = 2 * ( full scale acceleration in g' s)
f SR = CNT sample rate in Hertz
fCLK = accelerometer clock rate in Hertz
fCNT = CNT pulse rate in pulses / sec
g FORCE = acceleration in gravity units
1 g = 9.8085 m / s2 or 32.180 ft / s2
The first equation above shows that as the
sample rate is reduced (i.e. a longer
sample period), the quantization becomes
finer but bandwidth is reduced.
Conversely, as the sample rate is
increased, quantization becomes coarser
but the bandwidth of the measurement is
increased. The second and third equations
show how the CNT pulse frequency
equates to the applied g-force. When
using a frequency counter to monitor the
CNT output pulse rate, a counter with a DC
coupled input must be used. The CNT
output is a return-to-zero signal whose duty
cycle varies from zero to fifty percent, from
minus full scale to positive full scale
acceleration. A frequency counter with an
AC coupled input will provide an erroneous
reading as the duty cycle varies
appreciably from fifty percent. The figure to
the left illustrates how the CNT and DIR
outputs vary as the accelerometer is
subjected to accelerations from minus full
scale (-FS) to plus full scale (+FS).
DEFLECTION VOLTAGE (DV) TEST INPUT: This test input applies an electrostatic
force to the sense element, simulating a positive acceleration. It has a nominal input
impedance of 32 kΩ and a nominal open circuit voltage of aVDD. For best accuracy during
normal operation, this input should be left unconnected or connected to a voltage source
equal to a of the VDD supply. The change in output pulse rate (∆f) is proportional to the
square of the difference between the voltage applied to the DV input (VDV) and aVDD. Only
positive shifts in the output pulse rate may be generated by applying voltage to the DV
input. When voltage is applied to the DV input, it should be applied gradually. The
application of DV voltages greater than required to bring the output to positive full scale
may cause device damage. The proportionality constant (k) varies for each device and is
not characterized.
1


∆ f ≈ k  VDV − VDD 


3
2
ESD and LATCH-UP CONSIDERATIONS: The model 1010 accelerometer is a CMOS device subject to damage from large
electrostatic discharges. Diode protection is provided on the inputs and outputs but care should be exercised during handling
to assure that the device is placed only on a grounded conductive surface. Individuals and tools should be grounded before
coming in contact with the device. Do not insert the model 1010 into (or remove it from) a powered socket.
SPECIFICATIONS SUBJECT TO CHANGE WITHOUT NOTICE
Silicon Designs, Inc. ! 1445 NW Mall Street, Issaquah, WA 98027-5344 ! Phone: 425-391-8329 ! Fax: 425-391-0446
web site: www.silicondesigns.com
[page 4]
Mar 07
Model 1010 Digital Accelerometer
BIAS STABILITY CONSIDERATIONS
Bias temperature hysteresis can be minimized by temperature cycling your model 1010 accelerometer after it has
been soldered to your circuit board. If possible, the assembled device should be exposed to ten cycles from -40 to
+85EC minimum (-55 to +125EC recommended). The orientation to the Earth's gravitational field during temperature
cycling should preferably be in the same orientation as it will be in the final application. The accelerometer does not
need to have power applied during this temperature cycling.
PACKAGE DIMENSIONS
"L" SUFFIX PACKAGE (20 PIN LEADLESS CERAMIC CHIP CARRIER)
*T
C
K
F
*U
L
*M
A
E
TERMINAL 1
H
J
Positive
Acceleration
TERMINAL 20
A
G
D
"J" SUFFIX PACKAGE (20 PIN LEADED CHIP CARRIER)
P
B
R
N
DIM
A
B
C
D
E
F
G
H
J
K
L
*M
N
P
R
*T
*U
INCHES
MIN
MAX
0.342 0.358
0.346 0.378
0.055 TYP
0.095 0.115
0.085 TYP
0.050 BSC
0.025 TYP
0.050 TYP
0.004 x 45°
0.010 R TYP
0.016 TYP
0.048 TYP
0.050 0.070
0.017 TYP
0.023 R TYP
0.085 TYP
0.175 TYP
MILLIMETERS
MIN
MAX
8.69
9.09
8.79
9.60
1.40 TYP
2.41
2.92
2.16 TYP
1.27 BSC
0.64 TYP
1.27 TYP
0.10 x 45°
0.25 R TYP
0.41 TYP
1.23 TYP
1.27
1.78
0.43 TYP
0.58 R TYP
2.16 TYP
4.45 TYP
NOTES: 1. * DIMENSIONS 'M', 'T' & 'U' LOCATE ACCELERATION SENSING ELEMENT'S CENTER OF MASS .
2. LID IS ELECTRICALLY TIED TO TERMINAL 19 (GND).
3. CONTROLLING DIMENSION: INCH.
4. TERMINALS ARE PLATED WITH 60 MICRO-INCHES MIN GOLD OVER 80 MICRO-INCHES MIN NICKEL.
(THIS PLATING SPECIFICATION DOES NOT APPLY TO THE METALLIZED PIN-1 IDENTIFIER MARK ON
THE BOTTOM OF THE J-LEAD VERSION OF THE PACKAGE).
5. PACKAGE: 90% MINIMUM ALUMINA (BLACK), LID: SOLDER SEALED KOVAR.
SOLDERING RECOMMENDATIONS:
RoHS Compliance: The model 1010 does not contain elemental lead and is RoHS compliant.
WARNING: If no-lead solder is to be used to attach the device, we do not recommend the use of reflow soldering
methods such as vapor phase, solder wave or hot plate. These methods impart too much heat for too long of a
period of time and may cause excessive bias shifts. For no-lead soldering, we only recommend the manual "Solder
Iron Attach" method (listed on the next page of this data sheet). We also do not recommend the use of ultrasonic
bath cleaners because these models contain internal gold wires that are thermo sonically bonded.
SPECIFICATIONS SUBJECT TO CHANGE WITHOUT NOTICE
Silicon Designs, Inc. ! 1445 NW Mall Street, Issaquah, WA 98027-5344 ! Phone: 425-391-8329 ! Fax: 425-391-0446
web site: www.silicondesigns.com
[page 5]
Mar 07
Model 1010 Digital Accelerometer
SOLDERING RECOMMENDATIONS (continued):
Reflow of Sn62 or Sn63 type solder using a hotplate is the preferred method for assembling the model 1010 surface mount
accelerometer to your Printed circuit board. Hand soldering using a fine tipped soldering iron is possible but difficult without
a steady hand and some form of visual magnification due to the small size of the connections. When using the hand solder
iron method, it’s best to purchase the J-Leaded version (1010J) for easier visual inspection of the finished solder joints.
Pre-Tinning of Accelerometer Leads is Recommended: To prevent gold migration embrittlement of the solder joints,
it is best to pre-tin the accelerometer leads. We recommend tinning one lead at a time, to prevent excessive heating of
the accelerometer, using a fine-tipped solder iron and solder wire. The solder bath method of pre-tinning is not
recommended due to the high degree of heat the interior of the device gets subjected to which may cause permanent shifts
in the bias and/or scale factor.
Hotplate Attach Method using Solder Paste or Solder Wire: Apply solder to the circuit board’s pads using Sn62 or Sn63
solder paste or pre-tin the pads using solder and a fine tipped soldering iron. If pre-tinning with an iron, apply flux to the
tinned pads prior to placing the components. Place the accelerometer in its proper position onto the pasted or tinned pads
then place the entire assembly onto a hotplate that has been pre-heated to 250EC. Leave on hotplate only long enough
for the solder to flow on all pads (DO NOT OVERHEAT!)
Solder Iron Attach Method using Solder Paste: Apply solder paste to the circuit board’s pads where the accelerometer
will be attached. Place the accelerometer in its proper position onto the pasted pads. Press gently on the top of the
accelerometer with an appropriate tool to keep it from moving and heat one of the corner pads, then an opposite corner
pad with the soldering iron. Make sure the accelerometer is positioned so all 20 of its connections are centered on the
board’s pads. Once the two opposite corner pads are soldered, the part is secure to the board and you can work your way
around soldering the remaining 18 connections. Allow the accelerometer to cool in between soldering each pin to prevent
overheating.
Solder Iron Attach Method using Solder Wire: Solder pre-tin two opposite corner pads on the circuit board where the
accelerometer will be attached. Place the accelerometer in its proper position onto the board. Press gently on the top of
the accelerometer and heat one of the corner pads that was tinned and the part will drop down through the solder and seat
on the board. Do the same at the opposite corner pad that was tinned. Make sure the accelerometer is positioned so all
20 of its connections are centered on the board’s pads. Once the two opposite corner pads are soldered, the part is secure
to the board and you can work your way around soldering the remaining 18 connections. Allow the accelerometer to cool
in between soldering each pin to prevent overheating.
LCC & JLCC Solder Contact Plating Information: The plating composition and thickness for the solder pads and
castellations on the “L” suffix (LCC) package are 60 to 225 micro-inches thick of gold (Au) over 80 to 350 micro-inches thick
of nickel (Ni) over a minimum of 5 micro-inches thick of moly-manganese or tungsten refractory material. The leads for
the “J” suffix (JLCC) package are made of an Iron-Nickel sealing alloy and have the same gold over nickel plating
thicknesses as for the LCC pads.
Recommended Solder Pad Pattern: The recommended solder pad size and shape for both the LCC and J-LCC
packages is shown in the diagram and table below. These dimensions are recommendations only and may or may not
be optimum for your particular soldering process.
DIM
A
B
C
D
E
F
G
inch
.230
.430
.100
.033
.050
.013
.120
mm
5.84
10.92
2.54
0.84
1.27
0.33
3.05
SPECIFICATIONS SUBJECT TO CHANGE WITHOUT NOTICE
Silicon Designs, Inc. ! 1445 NW Mall Street, Issaquah, WA 98027-5344 ! Phone: 425-391-8329 ! Fax: 425-391-0446
web site: www.silicondesigns.com
[page 6]
Mar 07
Model 1010 Digital Accelerometer
APPLICATION NOTE
ACCELERATION MEASUREMENT WITH A MICROCONTROLLER:
The CNT (count) pulse density modulation output of the model 1010 accelerometer was designed to drive the type of
hardware pulse counter that is sometimes present in microcontrollers. The schematic (below) shows a model 1010
accelerometer driving the T0 counter of an Intel 80C51 microcontroller. The accelerometer's clock is provided by the
Address Latch Enable (ALE) output of the 80C51 after being divided by a factor of four by the two 74HC74 "D-Type"
flip/flops. The divide by 4 is needed because the maximum count rate of the 80C51's T0 counter is 1/24th of the 8051's
clock oscillator frequency (FOSC) and the frequency of ALE is 1/6th of FOSC. Divisors of greater than four should be used if
FOSC is greater than 12 MHz to keep the accelerometer's clock frequency at or below the recommended 1 MHz maximum.
Use of ALE for the accelerometer clock is only recommended for applications where no external memory is connected to
the 80C51. ALE is missing an output pulse for each MOVX instruction which is used to access external memory.
Alternatively, any available clock source asynchronous with the 8051's clock may be used to drive the accelerometer so
long as its frequency is between 100 kHz and 1 MHz and is no greater than 1/48th of FOSC.
MODEL 1010 CONNECTION TO A MICROCONTROLLER
To obtain each interval's average acceleration, the software needs to poll counter T0's value at fixed intervals then subtract
each new counter value from its previous value to obtain a delta (difference) count for each interval. Of course the software
must also account for wraparound of the counter which requires that the counter contain enough bits to prevent more than
one counter overflow during each sample period. The delta count relates to the average applied acceleration according
to the following equation.
∆C =
Ag 
1

f CLK  +
 2 g SPAN 
f SR
Where:
∆C
fCLK
Ag
gSPAN
fSR
= the change in the counter’s value over each sample interval
= the accelerometer's input clock frequency
= the average acceleration force in g's during the sample interval
= 2 * (full scale acceleration rating of accelerometer)
= the software sample rate of the counter in samples/sec
At minus full-scale acceleration, the difference count (∆C) is zero. Zero acceleration results in a difference count of onehalf of the maximum difference count value; plus full scale acceleration results in the maximum value (fCLK / fSR). The
actual difference value achieved at zero acceleration [which will be near ½(fCLK / fSR)], may be subtracted from each
interval's difference count to obtain the acceleration count in sign-magnitude format.
SPECIFICATIONS SUBJECT TO CHANGE WITHOUT NOTICE
Silicon Designs, Inc. ! 1445 NW Mall Street, Issaquah, WA 98027-5344 ! Phone: 425-391-8329 ! Fax: 425-391-0446
web site: www.silicondesigns.com
[page 7]
Mar 07
Model 1010 Digital Accelerometer
APPLICATION NOTE
CONVERTING DIR TO AN ANALOG VOLTAGE
It is best to use a model 1210 or 1221 for analog applications but if a proportional
analog voltage is desired from a model 1010, one can be easily generated by the
connection of a low-pass filter to the DIR output as shown in the schematic
(below). The table (at right) lists values for R1 and C2 for various cutoff
frequencies (-3 dB frequency). R1 is chosen to be at least 100 times the
maximum output impedance of DIR which is 200Ω. The circuit or instrument that
the 0 to +5V analog output is connected to, must have an input impedance at
least 100 times the value of R1. This simple passive RC filter can be used as
long as it provides sufficient rejection of the switching noise present on the DIR
output for the specific application.
CUTOFF
FREQUENCY
(Hz)
R1
(kΩ)
C2
(µF)
200
36.0
.022
800
35.7
.0056
1000
34.0
.0047
1600
30.1
.0033
2000
36.0
.0022
SINGLE POLE RC FILTER
If greater rejection of switching noise is needed, a two pole active filter can be used as shown in the schematic (below).
This circuit has the added advantage of providing a very low output impedance compared with the single pole circuit. Its
disadvantages include greater complexity and the need for 1 or 2 additional supply voltages for the op-amp. For both filter
types, tight tolerance, temperature stable resistors and capacitors should be used. To reject common mode noise over
long signal transmission line lengths, DIR and its complement can be used to drive a pair of wires with a differential filter
placed at the far end of the wires.
TWO POLE ACTIVE FILTER
Cutoff Frequency
(Hz)
R1 & R2
(kΩ)
R3
(kΩ)
R4 & R5
(kΩ)
C6
(µF)
C7
(µF)
200
21.5
36.0
93.1
.012
.068
800
19.1
43.0
105
.0027
.018
1000
18.2
42.2
102
.0022
.015
1600
17.4
38.3
93.1
.0015
.010
2000
21.5
36.0
93.1
.0012 .0068
SPECIFICATIONS SUBJECT TO CHANGE WITHOUT NOTICE
Silicon Designs, Inc. ! 1445 NW Mall Street, Issaquah, WA 98027-5344 ! Phone: 425-391-8329 ! Fax: 425-391-0446
web site: www.silicondesigns.com
[page 8]
Mar 07
APPLICATION NOTE
Model 1010 Digital Accelerometer
ACCELERATION THRESHOLD DETECTION:
For applications where it is desired to know when acceleration has exceeded a threshold value, the simple circuit shown
in the schematic (below) can be used. This circuit uses a 74HC161 synchronous binary counter to detect when the DIR
logic output goes high for a minimum of 16 clock cycles in a row. The 74HC74 D-type flip/flop is connected in a "onescatch" configuration so that once the threshold is exceeded, the flip/flop stores the event. The clear input sets the counter
value to zero and clears the flip/flop, making the circuit ready to detect the next 16 ones in a row sequence. When driven
by the DIR (true) output, this circuit provides a threshold of approximately 7/8ths
___ of full scale (+43.75g for a ±50g device).
Negative acceleration pulses can be detected by connecting the counter to DIR instead of DIR.
THRESHOLD DETECTION CIRCUIT
SPECIFICATIONS SUBJECT TO CHANGE WITHOUT NOTICE
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Mar 07