This invention relates to eddy current sensors for sensing the movement of an electrically conductive member along a path. Such sensors are used as speed or torque sensing probes for example for sensing the speed of the blades of the compressor or turbine of a gas turbine. Torque in a rotating member may be assessed by using two sensing probes for sensing the rotation of the member at two axially-spaced positions and determining the phase difference between the outputs of the probes.
An example of such a probe is disclosed in GB 2 265 221. The probe uses a strong and large magnet to form a strong magnetic field. When a metal object such as a turbine blade passes through the field, eddy currents are generated in the blade. The probe includes a pick-up coil for detecting the very small magnetic fields generated by the eddy currents induced in the tip of a moving blade. To do this task, the coil needs to have a large number of turns, typically 5,000, wound on a core or pole piece made of a soft magnetic material having a high permeability. As a result of this coil construction, its inductance is very large, typically 1 or 2 henries.
For gas turbine applications, the probe is mounted outside on the turbine casing, resulting in a large air gap between the sensor and the tips of the blades. To increase the signal picked up in the coil, the magnetic field should be as strong as possible at the operating distance. This is achieved by selecting a very long wide magnet.
According to the present invention, there is provided an inductive sensor for sensing the movement of an electrically conductive member as the member moves along a path, comprising a magnet having a pole adjacent the path of the member for generating a magnetic flux pattern in the path of the member, and an eddy current detector element positioned adjacent the said path to receive magnetic pulses caused by eddy currents generated in the said member as it moves through the flux pattern generated by the magnet pole wherein the detector element has minimal magnetic susceptibility so as to leave substantially undistorted the flux pattern generated by the magnetic pole in the path of the member. Conveniently, the detector element is in the form of a pick-up coil devoid of a core of any soft magnetic material and thus effectively an air-cored coil.
With the known arrangement, the pick-up coil has to be as close to the magnet as possible to minimise space and to maximums the signal picked up. As a result the magnetic field is attracted to the core of the pick-up coil so the strength of the field through which the blade tips pass is reduced. Thus, the portions of the blade passing at a distance of typically 10 to 12 mm from the magnet are not exposed to a strong magnetic field and the resulting eddy currents are weakened.
The magnetic core of the coil increases the coil inductance resulting in a low resonance frequency and high impedance of the coil. The presence of resonance in the coil distorts the output signal amplitude of the probe. The signal may well have superimposed on it an oscillating signal resulting in several zero crossings giving a false speed reading. Moreover, the current in a coil having a large inductance decays very slowly affecting the amplitude of the subsequent signals and changing the position of the zero crossings.
Further sensors with coils having a large impedance are much more susceptible to electromagnetic interference. A sensor having a large inductance cannot be used in areas which must be intrinsically safe because the inductance stores a lot of energy and could generate a spark igniting an explosive gas mixture.
To solve the above problems the invention removes the conventional soft magnetic core from the probe coil.
The invention will now be further described by way of example with reference to the accompanying diagrammatic drawings in which:
As shown in
This arrangement is also shown in
In the arrangement shown in
In the modified arrangement shown in
The body 61 has two further boxes 67a, 67b, one on each side of the pair of magnets 63, to receive the pick-up coils 68a, 68b. The cylindrical surface of the body 61 is formed with channels 69 leading to apertures 70 in the mounting flange 62 to receive the connecting wired for the coils.
By providing the or each coil with a further coil without a core in a configuration as shown in GB 2 265 221 it is possible to make the probe less susceptible to the interference of external magnetic fields.
Thus, a further coil (not shown) again without a core of soft magnetic material, maybe positioned coaxially with the or each pick up coil 28, 38, 48, 58 or 68 but further from the path of the blades. By connecting the pick up and further coils in opposition, the effects of external electromagnetic field may be largely cancelled out with only minor reduction in the pick up signal since the further coil will only pick up a much reduced signal as the result of its greater distance from the path of the blades.
The probes shown in FIGS. 3 to 10 may be used to measure the speed of any metallic non-ferromagnetic object with at least one discrete member such as the tooth of a gearwheel, a phonic wheel, a shaft with a slot or protrusion or the blades of a fan in which eddy currents are generated in the member as it rotates through the flux pattern.
While the magnets will normally be permanent magnets for convenience, it would be possible to use electromagnets provided that they are fully saturated in use.
Number | Date | Country | Kind |
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0328049.2 | Dec 2003 | GB | national |