This invention relates to a magnetic absolute angular position sensor for valves controlled by part-turn electric actuators.
These valves are shut-off members which are fitted on pipes or machines in which the supply or discharge flow is to be controlled or stopped; fluid flow rate may be stopped or reduced by using parts to be lifted from a stationary seat, on which they sealably abut, or parts that rotatably uncover a port of variable width.
Valves are actuated by electric part-turn actuators which control the rotation of the valve shaft by electric remote controls, particularly when valves are located in hardly reachable positions, such as desert areas or sea bottoms.
This type of actuation, which uses electric actuators, imperatively requires the angular position of the valve shaft to be exactly known at any time, so that its opening degree may be determined, as well as the corresponding electric control: such angular position value of the shaft is detected by a sensor.
In prior art, several different angular position sensors are provided, such as:
The drawbacks of prior art are:
The object of this invention is to allow accurate determination of the angular position of an electrically actuated valve shaft, by using a magnetic sensor.
The advantages achieved by using the magnetic angular position sensor of this invention are:
These objects and advantages are achieved by the magnetic sensor of this invention, which is characterized by the annexed claims.
These and other characteristics will be more apparent from the following description of a few embodiments, which are shown by way of example and without limitation in the accompanying drawings, in which:
Referring to
The case 1 has three flange rims 1a, which are connected by bolts to a one-position stationary support, which might be the actuator of the shut-off valve to be controlled.
A circuit board 7 is also secured to the housing 1, in the vicinity of a permanent magnet 8 located in the support disk 2.
The circuit board 7, which has an essentially rectangular shape, has a widened central portion for housing electric circuits which, as the magnetic field direction changes due to the rotation of the support disk 2 connected to the valve actuator, provide the signals for determining the angle of rotation.
The circuit board 7 is introduced in two housings 1d formed in the case 1 and secured thereto by a pair of screws 5; the end portion of such circuit board 7 protrudes from the case 1 to allow the acquisition of the generated signals.
The support disk 2 is accommodated between the case 1 and the circuit board 7, and directly lies on the bottom of the case 1, while being held in contact with the case 1 by an elastic ring 4.
The support disk 2 contains the permanent magnet 8 on one side and the shaft of the valve to be controlled on the other side.
Also, the support disk 2 has a slot 2a which engages a pin 1b of the case 1; the angular width of such slot determines the maximum angle of rotation (about 110°) of the valve shaft.
The combined arrangement of the flange rims 1a, the pin 1b and the slot 2a which engages the pin 1a, provides a unique electrical and mechanical assembly, which requires no initial calibration.
The cover 3 is fastened by two screws 6 to the support disk 2.
A rotation α of the shaft 10 causes a change in the direction of the magnetic field generated by the magnet 8: this change is detected by the Wheatstone bridge of the circuit board 7 in the form of a sinusoidal electric signal X, which is proportional to twice the angle of rotation α.
Hence, one Wheatstone bridge may be used to determine angles of rotation up to 90°.
In this arrangement, two electric signals X and Y are generated, which are offset a an angle of 90°, i.e. a sinusoidal and a cosinusoidal signal, each being proportional to twice the angle of rotation α.
In this arrangement, the amplitude of the signals changes with the sensor temperature, however both bridges are simultaneously embedded in the same silicone substrate and have the same characteristics: hence, both electric signals X and Y have no phase displacement and no compensation therebetween is required.
The signals X and Y, which are generated by a rotation α of the shaft 10, may be mathematically described as follows:
X(α,T)=Xo(T)·Sin(2α)
Y(α,T)=Yo(T)·Cos(2α)
Also, by assuming that both electric signals X and Y have the same amplitude, i.e. Xo=Yo, the angle α may be determined in a failsafe manner from the acquired electric signals X and Y, thanks to the following
Such result does not depend on the amplitude of the acquired electric signals X and Y. Therefore, temperature has no effect on measurements, and no further compensation coefficients are required.
Number | Date | Country | Kind |
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PR2004A0037 | May 2004 | IT | national |
Number | Name | Date | Kind |
---|---|---|---|
5055781 | Sakakibara et al. | Oct 1991 | A |
6326781 | Kunde et al. | Dec 2001 | B1 |
6498479 | Hamaoka et al. | Dec 2002 | B1 |
20040095132 | Carlson et al. | May 2004 | A1 |