INFINEON FP212L100-22

Differential Magnetoresistive Sensor
FP 212 L 100-22
Features
•
•
•
•
•
High output voltage
High operating temperature
Robust plastic housing
Biasing magnet build in
Signal amplitude is speed
independent
• Marking silver
Typical applications
•
•
•
•
•
Detection of speed
Detection of position
Detection of sense of rotation
Angle encoder
Linear position sensing
Dimensions in mm
Type
Ordering Code
FP 212 L 100-22
Q65212-L1004
The differential magnetoresistive sensor FP 212 L 100-22 consists of two series coupled
magneto resistors (L-type InSb/NiSb semiconductor resistors whose value can be
magnetically controlled) which are mounted onto an insulated ferrite substrate. The
sensor is encapsulated in a plastic package and has three connecting terminals.
The basic resistance of the total system is 2×100 Ω. A permanent magnet which supplies
a biasing magnetic field is fixed on the base of the sensor.
Semiconductor Group
1
07.96
FP 212 L 100-22
Maximum ratings
Parameter
Symbol
Value
Unit
Operating temperature
TA
Tstg
Ptot
VIN
VI
– 40 / + 140
°C
– 40 / + 150
°C
450
mW
10
V
> 60
V
GthA
≥5
mW/K
5
V
Total resistance, (δ = ∞, I ≤ 1 mA)
VIN N
R1-3
220…400
Ω
Center symmetry3) (δ = ∞)
M
≤ 10
%
Offset
(at VIN N and δ = ∞)
V0
≤ 130
mV
Open circuit output voltage5)
(VIN N and δ = 0.2 mm)
Vout pp
> 1000
mV
Cut-off frequency
fc
> 20
kHz
Storage temperature
Power dissipation1)
Supply voltage2)
Insulation voltage between
terminals and magnet
Thermal conductivity
(when soldered)
Characteristics (TA = 25 °C)
Nominal supply voltage
voltage4)
Measuring arrangements
By approaching a soft iron part close to the sensor a change in its resistance is obtained.
The potential divider circuit of the magneto resistor causes a reduction in the
temperature dependence of the output voltage VOUT.
1) Corresponding to diagram Ptot = f(TA)
2) Corresponding to diagram VIN = f(TA)
3)
R1 – 2 – R2 – 3
M = ---------------------------- × 100% for R1-2 > R2-3
R1 – 2
4) Corresponding to measuring circuit in Fig. 2
5) Corresponding to measuring circuit in Fig. 2 and arrangement as shown in Fig. 1
Semiconductor Group
2
FP 212 L 100-22
1. Digital revolution counting
For digital revolution counting, the sensor should be actuated by a magnetically soft iron
toothed wheel. The tooth spacing should correspond to about twice the magneto resistor
intercenter spacing i.e 2×1.6 mm (see Fig. 1).
The two resistors of the sensor are supplemented by two additional resistors in order to
obtain the sensor output voltage as a bridge voltage VOUT. The output voltage VOUT
without excitation then is 0 V when the offset is compensated.
Fig. 1
Schematic representation of a toothed wheel actuating an FP 212 L 100-22
Fig. 2
Measuring circuit and output voltage VOUT waveform
Semiconductor Group
3
FP 212 L 100-22
2. Linear distance measurement
To convert small distances into a proportional electric signal, a small soft iron part of
definite width (e.g. b = 1.8 mm) is moved over the face of the sensor.
Proportional signals for distances up to 1.5 mm can be obtained in this way. The
sinusoidal output signal gives a voltage proportional to distance in the zero crossover
region (see Fig. 3).
Fig. 3
Measuring arrangement for analogue application
Maximum supply voltage
versus temperature
VIN = f(TA)
Semiconductor Group
4
FP 212 L 100-22
Output voltage (typical) versus
temperature VOUTpp = f(TA), δ = 0.2 mm
VOUTpp at TA = 25 °C ^= 100%
Output voltage (typical) versus
airgap VOUTpp = f(δ), TA = 25 °C
VOUTpp at δ = 0.2 mm ^= 100%
Total resistance (typical)
versus temperature
R1-3 = f(TA), δ = ∞
Max. power dissipation
versus temperature
Ptot = f(TA), δ = ∞
Semiconductor Group
5