The present application claims the benefit under 35 U.S.C. ยง 119 of German Patent Application No. DE 102020211924.4 filed on Sep. 23, 2020, which is expressly incorporated herein by reference in its entirety.
The present invention relates to a sensor component including a microelectromechanical z inertial sensor, which enables a compensation of measuring errors caused by temperature gradients. The present invention further relates to a method for ascertaining an acceleration in the z direction with the aid of the microelectromechanical z inertial sensor.
Microelectromechanical sensors (so-called MEMS sensors) are used to detect different physical variables, such as pressure, rotation rate or acceleration. Typical MEMS sensors are installed in systems on circuit boards, by which not only interactions exist between the MEMS sensors and the circuit board but also those between MEMS sensors and further components situated on the circuit board, for example microchips. In systems such as smartphones or motor vehicles, CPU chips are thus frequently installed in the vicinity of the MEMS sensors. A particularly close arrangement of the components is unavoidable, in particular in products in the so-called consumer market (e.g., smart watches), due to space limitations (small volume and limited lateral extension). Since CPU chips are generally operated with varying time utilization, the waste heat generated by a microchip of this type is also subjected to corresponding time variations. This results in temporally variable temperature gradients between the CPU chip and the adjacent components, for example a MEMS sensor.
The temporally variable temperature gradient is particularly striking in an acceleration sensor designed in the form of a z rocker. In this type of sensor, a temperature gradient perpendicular to the z rocker results in a varying expansion of the contained gas in the cavity above and below the z rocker. The varying expansion of the contained gas, in turn, results in a deflection of the z rocker and thus in a change in the capacitance of the measuring electrodes, which is erroneously interpreted as acceleration. The system thus generates an acceleration signal, even though no corresponding acceleration is present in the z direction.
One object of the present invention is to provide a possibility for providing the measuring accuracy of a microelectromechanical z inertial sensor in the presence of temporally varying temperature gradients. This object may be achieved with the aid of the particular subject matter of example embodiments of the present invention. Advantageous embodiments of the present invention are disclosed herein.
According to an example embodiment of the present invention, a sensor component including a microelectromechanical z inertial sensor is provided with two sensor elements, each designed in the form of a z rocker, situated on a substrate. The sensor elements each have a seismic mass structure, which is elastically deflectable with respect to the substrate with the aid of a torsion spring, and which has a heavy side and an oppositely situated light side with regard to the torsion spring. The seismic mass structures of the two sensor elements have different perforations on their heavy and/or light sides, which effectuate a different response characteristic of the two sensor elements with respect to a temperature gradient running in the z direction. The sensor component further includes an evaluation circuit, designed to ascertain an acceleration in the z direction by evaluating the deflection of the seismic mass structures of the two sensor elements. With the aid of a sensor component designed in this way, it is possible to detect the presence of vertical temperature gradients within the inertial sensor during the measurement of accelerations in the z direction. In this way, erroneous outputs of the acceleration sensor may be effectively avoided. In addition, an increased measuring accuracy as well as a better reliability of the relevant inertial sensor further result from the use of two sensor elements.
In one specific embodiment of the present invention, it is provided that the evaluation circuit is designed to determine a temperature gradient running in the z direction, based on a deviation of the deflections of the seismic mass structures of the two sensor elements and to use it to correct the ascertained acceleration in the z direction. With the aid of this measure, it is possible to quantitatively detect the influence of the vertical temperature gradient on the acceleration values. A correction of the measured acceleration may thus be carried out. In this way, the measuring accuracy of the inertial sensor may be significantly improved.
In a further specific embodiment of the present invention, it is provided that the different perforations of the relevant sides of the two seismic mass structures are due to holes having a different size, shape, number and/or arrangement. A multiplicity of variation possibilities is offered hereby, which permit a particularly optimal adaptation of the sensitivity of the relevant sensor element with respect to vertical temperature gradients and simultaneously ensure a sufficient undercutting of the seismic mass structures during the manufacturing process.
In a further specific embodiment of the present invention, it is provided that the seismic mass structure of the first sensor element has a perforation formed by holes having a shape deviating from a square on at least one side, while the seismic mass structure of the second sensor element has a perforation formed by square holes on the relevant side. With the aid of square holes, particularly good results may be obtained in the undercutting of the seismic mass structures.
In a further specific embodiment of the present invention, it is provided that the seismic mass structure of the second sensor element has a perforation formed by linear holes on the corresponding side.
In a further specific embodiment of the present invention, it is provided that the two sensor elements are provided with essentially the same design with regard to the mass and mass distribution of their seismic mass structures, the stiffness of their torsion springs and the arrangement of corresponding electrodes for the capacitive detection of their deflection, so that the two sensor elements have the same sensitivity in the z direction. If the two sensor elements have the same sensitivity to z accelerations and different sensitivities to vertical temperature gradients, the model for calculating a corrected acceleration value may be particularly simple.
In a further specific embodiment of the present invention, it is provided that the two sensor elements are situated in parallel to each other, so that the heavy sides of their seismic mass structures are situated on the same side of the torsion springs. In this arrangement, the two sensor elements may be particularly easily manufactured with the same sensitivity to z accelerations.
In a further specific embodiment of the present invention, it is provided that the two sensor elements are situated anti-parallel to each other, so that the heavy sides of their seismic mass structures are situated on opposite sides of the torsion springs. In this arrangement, temperature gradients occurring within a shared cavity may be reduced faster.
According to a further aspect of the present invention, a microelectromechanical z inertial sensor is also provided for the aforementioned sensor component. The advantages already mentioned in connection with the sensor component result for the microelectromechanical z inertial sensor.
Finally, according to a further aspect of the present invention, a method is provided for ascertaining an acceleration in the z direction with the aid of a microelectromechanical z inertial sensor, which includes two sensor elements designed in the form of a z rocker, each including a seismic mass, which is elastically deflectable with the aid of a torsion spring. The two sensor elements have an identical sensitivity to an acceleration in the z direction and a different sensitivity to a temperature gradient running in the z direction. The method includes a separate detection of the deflections of the seismic mass structures of the two sensor elements as well as an ascertainment of an acceleration in the z direction by evaluating the deflections of the seismic mass structures of the two sensor elements, a temperature gradient running in the z direction being ascertained, based on a deviation between the deflections of the seismic mass structures of the two sensor elements, and used to correct the ascertained acceleration in the z direction.
The present invention is described in greater detail below on the basis of the figures.
As is further apparent from
In contrast to their electrical sensitivity, the two sensor elements 110, 130 have, however, different sensitivities to a vertical temperature gradient in cavity 121. To achieve this, the two sensor elements 110, 130 are equipped with differently shaped seismic mass structures 111, 131, the different shaping preferably being achieved by different perforations of at least one side of the two seismic mass structures 111, 131. A different geometry, size and/or number of holes 114, 134 in seismic masses 111, 131 thus typically result in a different response or sensitivity of the two sensor elements 110, 130 to vertical temperature gradients. Changes of the vertical temperature gradient are influenced, among other things, by openings 114, 117, 134, 137 in seismic mass structure 111, 131, which must be present for manufacturing reasons during the gas phase etching. The exact geometry (slit, square, rectangle, circle, ellipsis, etc.) and arrangement of these openings 114, 117, 134, 137 influence the intensity of the deflection of a z rocker in the presence of a vertical temperature gradient. The two sensor elements 110, 130 are therefore designed in such a way that holes 114, 117, 134, 137 on their seismic mass structures 111, 131 have different geometries. The influences of a vertical temperature gradient on the two z rockers 100, 130 are of different intensities. In the exemplary embodiment shown here, mass structures 111, 131 each have the same perforation 116, 136 on their light sides 115, 135 in the form of a matrix-shaped arrangement of square-shaped holes 117, 137. In contrast, heavy sides 112, 132 of the two mass structures 111, 131 each have different perforations 113, 133, heavy side 112 of first sensor element 110 having a total of four linear holes 114, while heavy side 132 of second sensor element 130 has a matrix-shaped arrangement of square holes 134.
A modified variant of z inertial sensor 100 from
A further variant of z inertial sensor 100 shown in
In an alternative design variant, instead of two sensor elements 110, 130 having the same electrical sensitivity to z accelerations, two sensor elements 110, 130 may also be used, which have different electrical sensitivities to z accelerations as well as different sensitivities to vertical temperature gradients. An evaluation of the signals and differentiation between a z acceleration and a vertical temperature gradient may be calculated in the particular evaluation circuit of the individual z rockers by stored tables, functions or models, which depict the sensitivity to a z acceleration and to a vertical temperature gradient. Two arbitrary rocker-shaped sensor elements may thus be used, whose signals are each conducted separately to an evaluation circuit (ASIC), the acceleration being calculated from the effect of a vertical temperature gradient with the aid of a suitable model. The model for the calculation is simpler, the smaller the difference of the electrical sensitivity and the greater the difference of the sensitivity to vertical temperature gradients of the two sensor elements is. For this reason, the z inertial sensor described in greater detail above, in which the two sensor elements 110, 130 have the same electrical sensitivity to z accelerations, is a particularly advantageous specific embodiment.
The perforation of the z rockers may be formed by different geometric shapes or different combinations of these geometric shapes (e.g., squares, rectangles, lines, circles, ellipses, polygons, etc.). The configuration with the aid of the different geometries of the perforation should, however, preferably take place in such a way that the electrical sensitivity between the two rocker-shaped sensor elements 110, 130 remains as uniform as possible, and different sensitivities to vertical temperature gradients are achieved at the same time.
Although the present invention was illustrated and described in greater detail by the preferred exemplary embodiments, the present invention is not limited by the described examples. Instead, other variations may be derived therefrom by those skilled in the art without departing from the scope of protection of the present invention.
Number | Date | Country | Kind |
---|---|---|---|
102020211924.4 | Sep 2020 | DE | national |