HMC1021S-TR Honeywell, HMC1021S-TR Datasheet - Page 12
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HMC1021S-TR
Manufacturer Part Number
HMC1021S-TR
Description
Manufacturer
Honeywell
Datasheet
1.HMC1021S-TR.pdf
(15 pages)
Specifications of HMC1021S-TR
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HMC1001/1002/1021/1022
360k-ohm feedback and reference resistors are chosen to provide a nominal 230mV/V/gauss gain characteristic or
1.15V/gauss gain with VDD at 5 volts. Other values than 360k-ohms may be chosen; with smaller resistances for larger
fields and larger resistances for lower field strengths. Be aware that sensor bridge offsets factor into the signal gain
selection as the offsets may be as large as the signal to be measured. See application note AN212 on methods to handle
bridge offset voltages.
As a magnetometer, the circuit outputs (Xout and Yout) should be measured against VREF and scaled for 1.15 volts per
gauss using a 5 volt sensor/amplifier power supply (VDD). Since the sensor’s bandwidth is 5 MHz, the sampling rate of
the outputs can be very fast, to the point were the filtering and speed of the amplifiers begins to effect the measurements.
Resolution will be mostly to the size of the Analog-to-Digital Converter (ADC), where a 10-bit ADC would spread its 1024
counts across the power supply or tighter.
As a compass, the two outputs constrain the earth’s magnetic field measurement to horizontal orientations with the Xout
and Yout feeding the heading equation of arctan (Yout/Xout) in degrees. The Xout direction of the HMC1002 should be
mounted to the forward direction of the product for proper orientation. If a tilt-compensated compass is desired, a third
axis could be made from the spare LMV324N amplifier and a HMC1001 sensor. Refer to the technical papers on
compassing from the website for more detail on compass implementation.
Field Detector or Current Sensor
A simple sensor implementation is shown in Figure 6 for a single axis sensor and signal conditioning circuitry for detecting
a magnetic disturbance, or as a current sensor when placed near a current carrying conductor. For more details on
current sensing, see application note AN209 on the website.
From Figure 6, the HMC1021 sensors are different from the HMC100x parts in that the bridge resistances increase to
1100 ohms and the set/reset strap resistance increases to 4.5 ohms. Because the minimum set/reset peak current is
down to 0.5 amperes, the set/reset drive circuit can now be run at common supply rails of 5 or 3 volts (VDD). Due to the
increased resistance of the set/reset strap, capacitor C3 can be reduced to about 0.22uf to maintain the desired 1 to 2
microsecond time constant. Capacitor C2 is typically chosen to be about ten times the series capacitor value, or 2.2uf.
The same pulse transition scheme in Figure 5 applies to Figure 6.
The sensor/amplifier circuit is likewise similar but the 1mV/V/gauss sensitivity requires a gain boost by increasing
feedback/reference resistors for sensing low fields like earth’s magnetic field. If a 2 or 3-axis compass is to be designed
with the HMC102x series sensor, parts like the HMC1022 plus the HMC1021Z can be used, with replication of the
difference amplifier stages for each axis. By choosing the 1 Meg-ohm and 4.99k-ohm resistors, the gain with a 5 volt
supply produces about a 1V/gauss transfer characteristic and centered at half supply (2.5 volts).
An instrumentation amplifier could be substituted for the operational amplifier to minimize external discrete components,
but the very low cost of op-amps like the LMV741/LMV358/LMV324 family is hard to beat if price is more important than
printed circuit board footprint. The signal output of the amplifier can be directly placed on the input of an ADC and further
processed in digital form. If the ADC range spans the power supply range, then a 10-bit ADC can have count 512 of 1024
used as the zero gauss point when the output rests at half-supply. If 3 volt operation is required, the designer can
substitute the IRF7507 part for the IRF7105 for 2.7 volt logic drive of the complementary MOSFET gates.
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