The invention relates to a non-contact working sensor, especially an inductive or capacitive sensor, preferably for measuring the distance or position of an object, with an inductive or capacitive sensor element, wherein measuring elements of the sensor element are embedded in a multilayered substrate and together with the substrate form the sensor element. Furthermore, the invention relates to a sensor element, such as is used in the sensor according to the invention.
For the detecting of distance, displacement, position and similar measured quantities, noncontact measurement methods are also used preferably in industry alongside tactile measurement methods, in order to avoid an unwanted interaction (on the one hand, wear on the measurement device, on the other hand influence on the measurement object) between the measurement device and the measurement object. Field-bound sensors are an often used category of such sensors. Thanks to a suitable arrangement, an analogy is achieved between the change in the electric or magnetic field and the change in displacement, position, or distance.
Examples of such sensors are capacitive displacement transducers, or inductive displacement transducers in general, such as eddy current displacement transducers, or also transformer-based principles, such as inductive displacement transducers working by the LVDT principle or coil arrangements whose magnetic coupling changes relative to each other through the relative spacing. In order to keep as low as possible the influence of perturbing factors, which falsify the analogy between change in field and change in displacement, such measurement systems often have a differential design. The most simple example of this is a half-bridge arrangement, in which two identical measuring elements are electrically interconnected in two branches of a Wheatstone bridge circuit so that perturbing factors cancel each other out. In this way, perturbing factors such as temperature changes can be suppressed. In practice, however, this is only possible in limited fashion, since the principle of differential signal evaluation only suppresses the perturbing factors when they are acting equally on both partial pathways.
However, in the case of temperature changes gradients occur not only over time, but also over location. These are not equalized by the differential arrangement. An example of this is inductive distance sensors, whose measuring elements (coils) are installed in a housing. One coil arranged for example at the end face is oriented toward the measurement object and measures its distance dynamically, a second coil in the housing measures statically against a reference object in the housing. In a half-bridge arrangement, an electrically symmetrical arrangement of the measuring elements can be achieved. However, this holds only at a certain distance and under static relations. If the temperature of the measurement object and thus that on the measuring coil changes other than the temperature of the sensor housing and thus that on the reference coil, this leads to (local) temperature gradients which disturb the symmetry and thus influence the measurement result. Likewise, mechanical extensions or compressions in the sensor element due to temperature changes result in non-deterministic and thus noncompensated movements or deformations of the sensor element, which likewise falsify the measurement.
The same holds for changes in humidity. Here as well, the differential approach only applies if both sensor pathways experience exactly the same change at the same time. This is not the case with the designs known in practice, since moisture usually acts only on the end-face measuring element, but not on the reference element integrated in the housing. The situation is similar with other perturbing factors, such as pressure and vibration.
Summarizing, the known sensors have the following problems: due to the design and the placement of the sensor element in a housing, perturbing factors on the one hand cause gradients which result in measurement errors. On the other hand, further measurement errors occur due to non-deterministic changes in the sensor element, caused by the perturbing factors or changes (aging) over the course of time.
Therefore, the problem which the invention proposes to solve is to avoid these drawbacks and to design and modify a sensor such that precise and stable measurements are possible. The same holds for the sensor element.
The above indicated problem is solved by the features of the coordinated claims 1 and 10. The sensor according to the invention is characterized in that the sensor element is constructed geometrically and/or electrically symmetrical in regard to its measuring elements and in that a mounting spaced apart from a holder is realized with the least possible contact surfaces on the sensor element. The sensor element according to the invention is designed accordingly.
The basis for this is a differential measurement system working by the capacitive or inductive principle. Differential here means first of all that the electrical arrangement already corresponds to a half-bridge or full-bridge arrangement. Thus, the problem is to also obtain a mechanically symmetrical arrangement, so that ambient factors such as temperature, pressure, moisture, etc., act symmetrically on the sensor element and do not falsify the measurement. Sensor element means in this context the essential element of a sensor or transducer, consisting of one or more measuring elements. In an inductive sensor, the sensor element is for example a coil with a central tap point, so that two partial coils are produced, serving as measuring elements. In the capacitive sensor, the sensor element consists of at least one measuring electrode and one reference electrode.
It is important that the sensor element has a symmetrical construction of the measuring elements and also in addition is symmetrically installed in the measurement arrangement.
The symmetrical construction of the sensor element can be achieved in that the measuring elements on both the front side and the back side of the sensor have the same distance from the housing surface. In the case of sensors where the measuring elements are embedded in a substrate consisting of multilayered circuit boards or multilayered ceramic (LTCC), this is achieved for example in that the layer makeup (number of layers and the position of the measuring elements) is chosen to be symmetrical. For example, 8 layers of substrate material would be used for a 7-layer coil.
It is advantageous for the substrate material to have the same thickness, so that the distance of the coil layers from the surface is the same in both directions. Thus, for example, a temperature change in the surroundings acts equally on both sides of the sensor element. At first, a local temperature gradient is established from the outside of the sensor element to the coils embedded in the interior. But since these are arranged at equal distances from the surface, the temperature change ultimately acts on the measuring elements in the same way. Thus, once again a symmetrical influencing is assured, and this is compensated by the differential evaluation. One could also arranged two measuring elements one above another, for example by integrating two 3-layer coils one on top of another in the multilayered substrate.
In the case of capacitive sensors, the measuring electrode is arranged near the end face in the first layer of the substrate. The reference electrode is arranged on the back side, away from the measurement object, in the last layer. In capacitive sensors a so-called shield is usually also employed, being maintained at the same potential as the measuring electrode, and shielding the measurement field against side influences. The arrangement of the shield electrodes (one each for the measuring electrode and the reference electrode) is likewise symmetrical. It is then further advantageous to introduce a grounding surface between the electrode arrangement of measuring and reference electrodes with corresponding shield electrodes. In this way, a symmetrical layout is achieved in regard to the arrangement of the electrodes in the substrate.
The measuring elements can also be arranged alongside each other. For example, multilayered coils can be arranged alongside each other in the mentioned ceramic substrate. In a rectangular substrate, one will arrange rectangular coils alongside each other. In a round substrate, the measuring elements could be distributed evenly over the circumference in the form of sectors, e.g., four partial coils in the form of four sectors. A nesting of the coils would also be conceivable, e.g., each layer of one coil is alternately coordinated with another partial coil. In this way, an especially uniform influencing of the partial coils could be achieved.
The measuring and reference electrodes could also be arranged alongside each other in capacitive sensors.
Usually the sensor element must be arranged on an object. However, a full-surface fastening to the object would defeat the symmetrical arrangement. If the sensor element or the coil arrangement which is embedded in a multilayered ceramic were to be fastened by its full surface to a holder, temperature changes would act more intensively or more delayed on the sensor element across the holder. For example, if the holder is heated intensively (because it fastens the sensor element to a machine part which is heated), the higher temperature will act at first on the back side of the sensor element. This produces a temperature gradient across the sensor element, which cannot be compensated by the differential arrangement of the measuring elements.
This can be accomplished in that the sensor element is also arranged almost symmetrical in regard to its holder. This is done with a pointlike attachment, e.g., a three-point bearing, which minimizes the bearing surface. For example, if balls are used for the three points, the bearing surface consists of only three point contacts. The heat input across such point contacts is greatly reduced, because the thermal mass is decoupled in this way. Thanks to the three-point bearing, the sensor element is almost free floating, so that ambient influences from all directions act equally and thus once more symmetrically on the (already symmetrically designed) sensor element. Thanks to a suitable choice of the balls, the heat transfer can be controlled. If the least possible heat transfer is desired, balls are used which are made from a material with slight heat transfer coefficient (such as Si3N4, Al2O3, ZrO2).
Besides the heat transfer, the coefficient of thermal expansion can also be controlled suitably by the ball material. Balls with low coefficient of thermal expansion alter the distance to the holder only slightly, while balls with higher coefficient of thermal expansion can achieve a temperature-dependent change in distance. Thus, a specific tilting could also be achieved with different ball material.
The choice of the ball material is also influenced by the measurement principle. For inductive or capacitive sensors it is advisable to use nonmetallic balls of ceramic or similar materials, since then an influencing of the measuring element is ruled out.
Instead of balls, tips or similar configurations with slight bearing surface could also be chosen. The deciding factor is the thermal decoupling from the substrate material, while at the same time exposing the sensor element to the surrounding atmosphere.
Thanks to an arrangement of the balls with one ball as a fixed bearing and two balls as loose bearings, a decoupling in the sideways direction from different expansion of sensor element and substrate material of the holder is additionally possible. This arrangement is also especially advantageous in regard to a replacement of the sensor element. If the sensor element needs to be replaced, the position of the replaced sensor element is clearly defined by the three-point arrangement. The fixed bearing, for example one in the form of a cup or a prism in which the first ball is situated, defines a fixed point. The second ball lies in a V-shaped groove, defining one degree of freedom in one direction. The third ball lies on a surface, so that there is an additional degree of freedom in a second direction. In this way, a relative lengthwise expansion between sensor element and holder due to different materials can be balanced out, without causing stresses in the sensor element. Furthermore, the need for an exact fit is reduced when replacing the sensor element, so that mechanical tolerances can also be balanced out during the replacement. The bearing surfaces (cup, groove, surface) can be as hard as possible, so that the balls are not pressed in and only a point contact is produced.
Thanks to the positioning of the bearing points relative to the sensor element and the suitable choice of the fixed point, the thermal expansion of the sensor element can be designed such that it is minimized relative to a particular position. For example, the fixed point will advantageously lie at the point of the measuring element which detects the measured quantity with the highest requirements.
As long as the sensor element is lying against the holder, gravity is sufficient for the stable fixation on the three-point bearing. In other installation situations, the sensor element must be pressed against the balls. This is done, for example, by means of a spring, which produces an adjustable force and presses the sensor element against the balls and holder.
In order to avoid an influencing of the measurement in the case of field-bound sensors, it is advisable to make the spring and the fastening element from nonmetallic material. For example, a plastic spring can be used, which is pretensioned with a plastic screw. Other nonmetallic materials are also conceivable, such as ceramic. The installation of the spring is advisedly done inside the three bearing points of the balls, for example, at the center of gravity of the triangle. The force and the holding of the spring and the fastening element must be designed such that the movement of the sensor element is not restricted by thermal expansions.
Now, there are various ways of embodying and modifying the teaching of the present invention in advantageous manner. For this, refer on the one hand to the claims coordinated with claim 1 and on the other hand to the following explanation of preferred embodiments of the invention with the aid of the drawings. Generally preferred embodiments and modifications of the teaching will also be explained in connection with the explanation of the preferred embodiments of the invention with the aid of the drawings. The drawing shows
In regard to further advantageous embodiments of the teaching of the invention, in order to avoid repetition, reference is made to the general portion of the specification and the accompanying claims.
Finally, it is expressly pointed out that the above described sample embodiments of the teaching of the invention serve only to explain the teaching claimed, but do not limit it to the sample embodiments.
Number | Date | Country | Kind |
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10 2016 202 637.2 | Feb 2016 | DE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/DE2017/200016 | 2/9/2017 | WO | 00 |