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Omnipolar Switch Hall-Effect IC Basics
Introduction
There are four general categories of Hall-effect IC devices
that provide a digital output: unipolar switches, bipolar
switches, omnipolar switches, and latches. Omnipolar
switches are described in this application note. Similar
application notes on bipolar switches, unipolar switches, and
latches are provided on the Allegro™ website.
Omnipolar Hall-effect sensor ICs, often referred to as
“omnipolar switches,” are a type of digital output Halleffect latching switches that operate with either a strong
positive or strong negative magnetic field. This simplifies
application assembly because the operating magnet can
be mounted with either pole toward the omnipolar device.
A single magnet presenting a field of sufficient strength
(magnetic flux density) will cause the device to switch to
its on state. After it has been turned-on, the omnipolar IC
will remain turned-on until the magnetic field is removed
and the IC reverts to its off state. It latches the changed state
and remains turned-off, until a magnetic field of sufficient
strength is again presented.
An application for detecting the position of a vehicle gearshift lever is shown in figure 1. The gear-shift lever incorporates a magnet (the purple cylinder). The line of miniature
black boxes is an array of omnipolar switch devices. When
the vehicle operator moves the lever, the magnet is moved
past the individual Hall devices. The devices near the magnet are subjected to the magnetic field and are turned-on, but
more remote devices are not affected and remain turned-off.
Either the south pole or the north pole of the magnet can be
oriented toward the Hall devices, and the branded face of
the Hall device package is toward the magnet.
Magnet
Hall ICs
Figure 1. An application using omnipolar switch sensor ICs. The ultra-small Hall ICs switch as the magnet
(purple cylinder) moves past them during gear-shifting.
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Magnetic Switchpoint Terms
The following are terms used to define the transition points, or
switchpoints, of Hall switch operation:
• B − The symbol for Magnetic Flux Density, the property of
a magnetic field used to determine Hall device switchpoints.
Measured in gauss (G) or tesla (T). The conversion is
1 G = 0.1 mT.
B can have a north or south polarity, so it is useful to keep in
mind the algebraic convention, by which B is indicated as a
negative value for north-polarity magnetic fields, and as a positive value for south-polarity magnetic fields. This convention
allows arithmetic comparison of north and south polarity values,
where the relative strength of the field is indicated by the absolute value of B, and the sign indicates the polarity of the field.
For example, a −100 G (north) field and a 100 G (south) field
have equivalent strength, but opposite polarity. In the same way,
a −100 G field is stronger than a −50 G field.
• BOP − Magnetic operate point; the level of a strengthening
magnetic field at which a Hall device switches on. The result-
ing state of the device output depends on the individual device
electronic design.
• BRP − Magnetic release point; the level of a weakening magnetic field at which a Hall device switches off (or for some types of
Hall devices, the level of a strengthening negative field given a
positive BOP ). The resulting state of the device output depends
on the individual device electronic design.
• BHYS − Magnetic switchpoint hysteresis. The transfer function of a Hall device is designed with this offset between the
switchpoints to filter out small fluctuations in the magnetic field
that can result from mechanical vibration or electromagnetic
noise in the application. BHYS = | BOP − BRP |.
Typical Operation
The switchpoint ranges of omnipolar sensor ICs are symmetrical
around the neutral field level, B = 0 G, as shown in figure 3. The
switchpoints are at equivalent field strengths, but at opposite
polarities. For example, assume the positive (south) polarity
switchpoints were operate point, BOP(S) , 60 G, and release point,
Figure 2. The Hall effect refers to the measurable voltage present when an
applied current is influenced by a perpendicular magnetic field.
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BRP(S) , 30 G. Then the negative (north) polarity switchpoints
would be operate point, BOP(N) , − 60 G, and release point,
BRP(N), − 30 G. Latching the latest state prevents the devices
from switching while subject to weak fields.
magnetic field strength is in the switchpoint hysteresis ranges,
BHYS . In addition, latching the switch state prevents the device
from switching while the magnetic field is relatively weak,
between the release points, BRP(N) and BRP(S) . It is not necessary
for the 0 G point to be crossed before switching can occur again.
A given switching event can be followed by a switching event of
either the same or the opposite polarity.
An omnipolar switch turns on in a strong magnetic field of either
polarity, and the resulting output signal can be either at logic high
(up to full supply voltage, VCC ) or logic low (at the output transistor saturation voltage, VOUT(sat) , usually <200 mV), depending
on the design of the device IC output stage. An omnipolar switch
turns off in a moderate magnetic field, and the resulting output
signal is the opposite of the polarity in the on state. Like other
types of Hall digital switch, these devices do not switch while the
Although the device could power-on with the magnetic flux
density at any level, for purposes of explanation of figure 3, start
at the far left, where the magnetic flux (B, on the horizontal axis)
is more negative than the north polarity operate point, BOP(N) .
Here the device is on, and the output voltage (VOUT , on the verti-
BOP(N) BRP(N)
BRP(S) BOP(S)
BHYS
BHYS
VCC
Switch to High
VOUT
Switch to Low
Switch to Low
Switch to High
VOUT(on)
VOUT(off)(sat)
0
B–
B+
0
Magnetic Flux Density, B (G)
BOP(N) BRP(N)
BRP(S) BOP(S)
BHYS
BHYS
VCC
Switch to High
VOUT
Switch to Low
Switch to Low
Switch to High
VOUT(off)
VOUT(on)(sat)
0
B–
0
B+
Magnetic Flux Density, B (G)
Figure 3. Omnipolar switch output characteristics. The top panel displays
switching to logic high in the presence of a strong magnetic field, and the
bottom panel displays switching to logic low, also in a strong magnetic field.
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cal axis) depends on the device design: high (top panel), or low
(bottom panel).
Following the arrows toward the right, the magnetic field
becomes less negative. When the field is weaker than BRP(N) , the
device turns off. This causes the output voltage to change to the
opposite state (either to high or to low, depending on the device
design).
While the magnetic field remains weaker than BOP(N) and BOP(S)
(near B = 0 G, the center of figure 3), the device remains turnedoff, and the latched output state remains unchanged. This is true
even if B becomes slightly stronger than BRP(N) or BRP(S) , within
the built-in zone of switching hysteresis, BHYS .
At the next strong magnetic field, if it is positive, following the
arrows toward the right, the magnetic field becomes more positive. When the field is stronger than BOP(S) , the device turns on.
This causes the output voltage to change to the opposite state
(either to high or to low, depending on the device design). If
instead the next strong magnetic field is negative, following the
arrows toward the left, the magnetic field becomes more negative. When the field is stronger than BOP(N) , the device turns on.
This causes the output voltage to change back to the original
state.
ground pins and between the supply and ground pins.
• For designs with chopper stabilization − A 0.1 μF capacitor must be placed between the supply and ground pins, and
a 0.01 μF capacitor is recommended between the output and
ground pins.
Power-On State
An omnipolar device powers-on in a valid state only if the
magnetic field strength exceeds either BOP or BRP when power is
applied. If the magnetic field strength is in the hysteresis band,
that is between BOP and BRP , the device can assume either an
on or off state initially, and then attains the correct state at the
first excursion beyond a switchpoint. Devices can be designed
with power-on logic that sets the device off until a switchpoint is
reached.
Power-On Time
Power-on time depends to some extent on the device design.
Digital output sensor ICs, such as the latching device, reach stability on initial power-on in the following times.
Pull-Up Resistor
A pull-up resistor must be connected between the positive supply
and the output pin (see figure 4). Common values for pull-up
resistors are 1 to 10 kΩ. The minimum pull-up resistance is a
function of the sensor IC maximum output current (sink current)
and the actual supply voltage. 20 mA is a typical maximum output current, and in that case the minimum pull-up would be VCC
/ 0.020 A. In cases where current consumption is a concern, the
pull-up resistance could be as large as 50 to 100 kΩ.
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 device is magnetically off. This
is not a device problem but is rather a leakage that occurs in the
conductors between the pull-up resistor and the sensor ICs output
pin. Taken to the extreme, this can drop the sensor IC output voltage enough to inhibit proper external logic function.
Device type
Power-on time
Non-chopped designs
<4 μs
Chopper-stabilized
<25 μs
V+
VCC
CBYPASS
0.1 μF
RPULLUP
Hall Device
VOUT
GND
Output
CBYPASS
0.1 μF
Use of Bypass Capacitors
Refer to figure 4 for a layout of bypass capacitors. In general:
• For designs without chopper stabilization − It is recommended
that a 0.01 μF capacitor be placed between the output and
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Figure 4. Typical application diagram.
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115 Northeast Cutoff
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Basically, this means that prior to this elapsed time after providing power, device output may not be in the correct state, but after
this time has elapsed, device output is guaranteed to be in the
correct state.
front-side approach (for example, if the south pole was nearer
the device in the front-side approach, then the north pole would
be nearer the device in the back-side approach). The north pole
would then generate a positive field relative to the Hall element,
while the south pole would generate a negative field.
Power Dissipation
Q: Are there trade-offs to approaching the device back side?
Total power dissipation is the sum of two factors:
• Power consumed by the sensor IC, excluding power dissipated
in the output. This value is VCC times the supply current. VCC
is the device supply voltage and the supply current is specified
on the datasheet. For example, given VCC = 12 V and Supply
current = 9 mA. Power dissipation = 12 × 0.009 or 108 mW.
• Power consumed in the output transistor. This value is
V(on)(sat) times the output current (set by the pull-up resistor). If
V(on)(sat) is 0.4 V (worst case) and the output current is 20 mA
(often worst case), the power dissipated is 0.4 × 0.02 = 8 mW.
As you can see, because of the very low saturation voltage the
power dissipated in the output is not a huge concern.
Total power dissipation for this example is 108 + 8 = 116 mW.
Take this number to the derating chart in the datasheet for the
package in question and check to see if the maximum allowable
operational temperature must be reduced.
Frequently Asked Questions
Q: How do I orient the magnets?
A: The magnet poles are oriented towards the branded face of the
device. The branded face is where you will find the identification
markings of the device, such as partial part number or date code.
Q: Can I approach the device back side with the magnet?
A: Yes, however bear this in mind: if the poles of the magnet
remain oriented in the same direction, then the orientation of
the flux field through the device remains unchanged from the
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A: Yes. A “cleaner” signal is available when approaching from
the package front side, because the Hall element is located closer
to the front side (the package branded face) than to the back side.
For example, for the “UA” package, the chip with the Hall element is 0.50 mm inside the branded face of the package, and so
approximately 1.02 mm from the back-side face. (The distance
from the branded face to the Hall element is referred to as the
“active area depth.”)
Q: Can a very large field damage a Hall-effect device?
A: No. A very large field will not damage an Allegro Hall-effect
device nor will such a field add additional hysteresis (other than
the designed hysteresis).
Q: Why would I want a chopper-stabilized device?
A: Chopper-stabilized sensor ICs allow greater sensitivity with
more-tightly controlled switchpoints than non-chopped designs.
This may also allow higher operational temperatures. Most new
device designs utilize a chopped Hall element.
Possible Applications
• Cellular phones
• Cordless telephones
• Pagers
• Palmtop computers
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115 Northeast Cutoff
Worcester, Massachusetts 01615-0036 U.S.A.
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Suggested Devices
• Standard Allegro latches are listed in the selection guides on the company website, at
http://www.allegromicro.com/en/Products/Categories/Sensors/latches.asp.
• Low-power latches are listed at
http://www.allegromicro.com/en/Products/Categories/Sensors/low_power_latches.asp.
Application Notes on Related Device Types
• Bipolar switches − http://www.allegromicro.com/en/Products/Design/bipolar/index.asp
• Unipolar switches − http://www.allegromicro.com/en/Products/Design/unipolar/index.asp
• Latching switches (latches) − http://www.allegromicro.com/en/Products/Design/latching/index.asp
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The information contained in this document does not constitute any representation, warranty, assurance, guaranty, or inducement by Allegro to the
customer with respect to the subject matter of this document. The information being provided does not guarantee that a process based on this information will be reliable, or that Allegro has explored all of the possible failure modes. It is the customer’s responsibility to do sufficient qualification
testing of the final product to insure that it is reliable and meets all design requirements.
For the latest version of this document, visit our website:
www.allegromicro.com
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115 Northeast Cutoff
Worcester, Massachusetts 01615-0036 U.S.A.
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