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by Joe Gilbert, Sensor Application Engineer
Unipolar Hall-effect sensors, often referred to
as Hall effect switches, operate using only a positive magnetic field.
A single south pole magnet, with sufficient magnetic strength (flux
density) greater than the sensor's operate point (BOP),
will cause the device to switch to its on state. Once on, the unipolar
sensor will remain on until the magnetic field is reduced to below
the sensors release point (BRP). When the magnetic field
reaches BRP, or flux densities less than BRP,
the unipolar sensor will switch off (see figure 1).
BOP magnetic operate point. A positive magnetic field > BOP will switch the sensor on (output low).
BRP release point. Removal of the magnetic field < BRP will switch the sensor off (output high).
Bhys hysteresis. Bhys = |BOP| + |BRP| (Hysteresis is designed into every Hall-effect switch).
Figure
1 is a pictorial showing the two possible states of the unipolar digital
switch. When reading the chart from left to right, at the far left
the magnetic field is less than BRP, the sensor is off,
and the output voltage is high (full supply voltage). Moving to the
right, at some point the magnetic field will become greater than BOP and
the sensor will then switch on. Output voltage will transition from
high to low, with the low voltage (Vsat) being typically <200
mV with a normal data sheet maximum of 400 mV. As long as the magnetic
field remains above BRP the output remains low. When the
magnetic field again drops below BRP, the sensor will transition
from low to high. (As stated earlier, note the designed-in hysteresis.)
A pull-up resistor from a positive supply to the output pin is required. Common values for pull-up resistors are 1K to 10K ohms. The minimum pull-up resistance is a function of the sensors maximum output current (sink current) and the actual supply voltage. Twenty milliamps is a typical maximum output current and in this case the minimum pull-up would be VCC/0.020 A. In some cases, where current consumption is a concern, the pull-up resistance could be as large as 50K to 100K ohms. Caution: With large pull-up values it is possible to invite external leakage currents to ground, which are high enough to drop the output voltage even when the sensor is magnetically off. This is not a sensor problem rather a leakage issue in the conductors between the pull-up resistor and the sensors output pin. Taken to the extremes this can drop the sensors output voltage enough to inhibit proper external logic function.
Total power dissipation is the sum of two factors.
Total power dissipation for this example is 108 + 8 = 116 mW. Take this number to the derating chart for the package in question and check to see if the maximum allowable operational temperature must be reduced.
An important characteristic of a unipolar sensor is that the sensor will always power-up* with its output in a known state. For a magnetic field less than BRP the sensor is normally off, and for a magnetic field greater than BOP the sensor is normally on. This characteristic is referred to as "true power-on state" or TPOS.
The bandwidth of Hall-effect sensors is typically 25 kHz to 30 kHz. In this era of 2 GHz microprocessors 25 kHz appears to be rather slow. In reality it is very rare for bandwidth to be a concern. Few mechanical systems will require or are capable of moving or spinning magnets fast enough to approach 25 kHz.
Power-up time depends to some extent on the sensor design. Digital output sensors, such as the unipolar sensor, reach stability on initial power up in the following times.
| Sensor type | Power-up time |
| Non-chopped designs | <1 µs |
| Chopper-stabilized | < 40 µs |
Allegro unipolar digital output data sheets often list the power-up time as <50 µs. Basically this says that prior to this time the sensors output may not be in the correct state and that after this time the output is guaranteed to be in a correct state.
It is recommended that 0.01 µF capacitors be placed across the output-to-ground and supply to ground pins.
A 0.1 µF capacitor must be placed across the supply-to-ground pins, and a 0.01 µF capacitor is recommended for the output to ground pins.
Q: How do I direct the magnet?
A: The south pole is directed towards the branded face of the
sensor. The branded face is where you will find the Allegro "A" as
well as a partial part number and temperature code.
Q: How does the north pole or negative magnetic field affect
a Unipolar sensor?
A: A north pole or negative field has no effect on a unipolar
sensor.
Q: Can a very large field damage a Hall-effect sensor.
A: No. A very large field will not damage or affect an Allegro
Hall-effect sensor nor will such a field add additional hysteresis
(other than the designed hysteresis).
Q: Can I approach the sensor backside with the magnet?
A: Yes, however now the north pole must be directed towards
the back side of the sensor. Note: The orientation of the flux field
through the sensor is identical for the above two scenarios.
Q: Are there trade-offs to approaching the sensor backside.
A: Yes. The "active area depth", or the location of the Hall-element,
is closer to the package front-side. For example, for the "UA" package,
the sensor IC is 0.018" from the front side or 0.042" from the package
backside.
Q: Why would I want a chopper-stabilized sensor?
A: Chopper-stabilized sensors have greater sensitivity with
more tightly controlled switch points than non-chopped designs. This
may also allow higher operational temperatures. Most new sensor designs
utilize a chopped hall element.
| Allegro Part Number | Temperature Range(s) |
Package Type(s) | Tape & Reel Available |
Comments |
|---|---|---|---|---|
| A1142 | E, L | LH, UA | Yes | two-wire unipolar |
| A1143 | E, L | LH, UA | Yes | two-wire unipolar |
| A3212 | E, L | LH, UA | Yes | low power unipolar |
| A3240 | E, L | LH, UA | Yes | unipolar |
| A3250 | J, L | LT, UA | Yes | programmable unipolar |
| A3251 | J, L | LT, UA | Yes | programmable unipolar |