Classifications

• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01C—MEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
  • G01C19/00—Gyroscopes; Turn-sensitive devices using vibrating masses; Turn-sensitive devices without moving masses; Measuring angular rate using gyroscopic effects
  • G01C19/56—Turn-sensitive devices using vibrating masses, e.g. vibratory angular rate sensors based on Coriolis forces
  • G01C19/5705—Turn-sensitive devices using vibrating masses, e.g. vibratory angular rate sensors based on Coriolis forces using masses driven in reciprocating rotary motion about an axis
  • G01C19/5712—Turn-sensitive devices using vibrating masses, e.g. vibratory angular rate sensors based on Coriolis forces using masses driven in reciprocating rotary motion about an axis the devices involving a micromechanical structure

Definitions

• the invention is based on a rotation rate sensor with a substrate, a bearing, a vibration structure suspended on the bearing by means of springs for the purpose of carrying out a planar drive vibration movement, and drive means for generating the planar drive oscillation movement
• Micromechanical rotation rate sensors with one sensing axis are used for a wide variety of applications. In motor vehicles, these are for example the anti-skid program ESP, navigation and rollover measurement, in home electronics there are applications in the field of image stabilization, motion detection and navigation.
• a micromechanical rotation rate sensor with a sensing axis is known from the German patent application DE 195 23 895 A1, in which a rotor mass suspended centrally via bending springs is excited to rotational oscillations and tilts when a rotation rate occurs due to the Coriolis effect. This deflection is detected by means of electrodes placed in a conductive layer above a substrate.
• the invention is based on a rotation rate sensor with a substrate, a
• the core of the invention consists in that the rotation rate sensor has first evaluation means for detecting a rotation in a first rotation axis and second evaluation means for detecting a rotation in a second rotation axis.
• the invention provides a rotary yaw rate sensor with two sensitive axes. This allows two measuring axes to be evaluated simultaneously on a single chip.
• the sensor is sensitive to both axes of rotation x, y lying in the chip plane.
• the sensor core is only marginally larger than a single-channel sensor with comparable specification requirements.
• the power consumption is significantly lower than for two single-channel sensors.
• only a single drive circuit is required for both measuring axes, and on the other hand, larger functional blocks of the circuit can be shared by temporal multiplexing for both detection channels, in particular when using digital evaluation circuits.
• the device In combination with the highly symmetrical sensor design, the device guarantees a well-matched performance and sensitivity of the two measurement channels.
• the relative orientation of the two measuring axes is given by design and is not impaired by tolerances in the assembly and connection technology, as in the case of the assembly of two single-channel sensors. drawing
• FIG. 1 shows the micromechanical functional part of a rotational speed sensor according to the prior art.
• Fig. 2 shows the schematic representation of the micromechanical functional part of a rotation rate sensor of FIG. 1 in plan view.
• FIG. 3 shows a rotation rate sensor according to the invention with two sensitive axes.
• FIGS. 4 A and B show two embodiments of the suspension structure of a rotation rate sensor according to the invention.
• FIG. 5 shows a rotation rate sensor according to the invention
• FIG. 6 shows a rotation rate sensor according to the invention with enlarged drive means.
• Fig. 1 shows the micromechanical functional part of a rotation rate sensor according to the prior art.
• the rotation rate sensor is shown in a schematic Thomasdar- position. Shown is a substrate or a carrier 10, a hub 20 with
• the hub 20 is connected to the carrier 10. About the oscillating springs 30, the hub is also connected to the oscillating mass 40.
• the rotation rate sensor has drive means in the form of comb structures C A i, C A2 , which serve to drive the vibration V.
• the drive of the excitable to the vibration seismic Mass, the oscillating mass 40 takes place in that the two crests of a drive structure, such as C A i, represent two electrodes that are charged to different electrical potentials.
• the complementary combs are drawn into each other due to the electrostatic attraction, and the oscillating mass 40 is thereby deflected. Furthermore, the
• Rate of rotation sensor comb structures C D i, C 02 which are adapted to detect the amplitude of the drive vibration and the signal is generally used to control this amplitude.
• the rotation rate sensor has detection means in the form of capacitor structures C S i, C S2 , which serve to measure the deflection of the vibration mass as a result of an acting Coriolis force F 0 .
• the oscillating mass 40 oscillates on a spherical path V about the hub 20.
• the yaw rate sensor detects rotations about the sensitive axis, the axis of rotation ⁇ , as intended.
• Coriolis forces F 0 occur, which lead to a deflection of the oscillating mass 40 in the direction indicated by arrows perpendicular to the vibration plane.
• the sense of direction of the Coriolis forces F 0 changes in each case with the sense of direction of the torsional vibration V of the oscillating mass 40.
• Fig. 2 shows the schematic representation of the micromechanical functional part of a rotation rate sensor of FIG. 1 in plan view.
• the drive combs CAU, C A i2, C A 2i, C A 22 and the detection combs C D n, C D i2, C D2 i, C D22 are shown .
• the drive combs CAU, C A i 2 serve to drive the oscillating mass 40 in FIG.
• the drive combs C A2 i, C A22 serve to drive the oscillating mass 40 in the direction -V.
• the detection combs C D n, C D i 2 , C D2 i, C D22 serve to measure the amplitude of the drive deflection in the two directions + V and -V.
• the capacity of this capacitor-like comb structures C D n, D i C 2, C i D2, D22 C depends on the depth of immersion of the combs into each other and thus from the
• the electrodes CTL and CT2 represent test electrodes. By applying a voltage to the test electrodes CTL and CT2, a deflection of the oscillating weight 40 in the direction of the Coriolis forces F can be got 0. Thus, the effect of the Corio lis guide F 0 simulated and the deflectability of the oscillating mass 40 of the tested. This allows the functionality of the sensor to be tested.
• FIG. 3 shows a rotation rate sensor according to the invention with two sensitive axes.
• the yaw rate sensor according to the invention is developed from the gyroscope sensor described above in the prior art.
• the inventive two-channel (because equipped with two sensitive axes) rotation rate sensor can be manufactured in the same surface micromechanical process. While the single-channel angular rate sensor in the prior art has a large asymmetry in the spring stiffness and moments of inertia of the suspension structure with the
• the design of the two-channel structure is highly symmetrical with respect to these two axes.
• the rotor 40 is connected to the substrate 10 via springs 30, which lead centrally inwards and are suspended near the center on a hub 20.
• the structure is set over drive combs in rotation about the vertical axis (z-axis).
• Drive detection combs measure the deflection of the system and feed the signal to a control loop that allows the sensor to operate stably at its drive frequency.
• Axis is below the four “rotor arms", ie the springs 30, in the buried conductor track plane of a substrate 10 are detection means in the form of structured electrode surfaces which detect the tilting of the rotor via the resulting capacitance changes From the difference signals Cx, p-Cx, n or Cy , p - Cy, n of the respectively opposite electrodes of first detection means and second detection means, respectively, the yaw rates can be derived around the x and y axes respectively and vice versa.
• Figures 4 A and B show two embodiments of the suspension structure of a rotation rate sensor according to the invention.
• the exact position of the natural frequencies in the drive and detection movement has a significant influence, inter alia, on the sensitivity and power consumption of the sensor.
• the spring geometry must therefore be designed accordingly to achieve the desired frequencies.
• AIIg. simple bending springs, as they are schema Table are shown in Figure 2, to use.
• the springs 30 will have more complicated geometries. These may be, for example, meander-shaped springs as shown in FIGS. 4 A and B.
• the number of springs 30 may also vary, but for symmetry reasons it will advantageously be a multiple of four.
• more than eight springs make little sense because they require too much space and the resulting spring stiffness would be too high for most applications.
• FIG. 5 shows a rotation rate sensor according to the invention with self-test electrodes.
• a simple self-test of the sensor is possible.
• FIG. 6 shows a rotation rate sensor according to the invention with enlarged drive means. To increase the drive amplitude or to reduce the required drive voltage (and thus the power consumption) compared to the
• Prior art embodiments may desire to increase drive capacity via additional drive combs.
• the micromechanical rotation rate sensors described here are cost-effectively manufactured in surface micromechanics.
• a semiconductor substrate with many sensors after processing is separated into rectangular pieces, each carrying a sensor element.
• the drive electrode trunks extend essentially along the diagonals of the rectangular substrate 10. Since the extension of the electrodes into the chip diagonals shows, without enlargement of the rectangular chip area, an extension of the drive electrode dams beyond the actual rotor radius and thus a larger number of drive or drive detection combs can be realized. Since just the outer ridges are particularly efficient in generating the drive torque, even a small increase in the comb number is very beneficial.

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• Physics & Mathematics (AREA)
• Engineering & Computer Science (AREA)
• General Physics & Mathematics (AREA)
• Radar, Positioning & Navigation (AREA)
• Remote Sensing (AREA)
• Gyroscopes (AREA)

Applications Claiming Priority (1)

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• 2007
  • 2007-11-08 KR KR1020107010148A patent/KR20100080555A/ko not_active Application Discontinuation
  • 2007-11-08 JP JP2010532443A patent/JP2011503557A/ja active Pending
  • 2007-11-08 CN CN200780101448A patent/CN101855515A/zh active Pending
  • 2007-11-08 US US12/513,834 patent/US20110088469A1/en not_active Abandoned
  • 2007-11-08 EP EP07822375A patent/EP2210060A1/de not_active Withdrawn
  • 2007-11-08 WO PCT/EP2007/062073 patent/WO2009059639A1/de active Application Filing

Non-Patent Citations (1)

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