Acceleration Sensor

The invention is directed to an acceleration sensor. Known sensors use liquids, e.g. oil, as damping means; however, this has the disadvantage that the damping or the frequency response is dependent upon viscosity and, accordingly, vary dependent upon temperature. Accordingly, an additional measurement error results in the measurement of accelerations which change with respect to time. Moreover, sealing means are necessary in order to separate the electric or electronic signal processing device from the liquid in an absolutely leakproof manner and to prevent the leakage of liquid. This makes the acceleration sensor more expensive.

An acceleration sensor according to the invention provides for a damping or frequency response to have only a slight dependence on temperature and is designed so as to be very simple, inexpensive, and also light.

By means of using a leaf spring or spring band or a torsion spring and, for example, a Hall element as sensor, the device is constructed so as to be particularly compact and light. The sensor can also be constructed, in particular, as an angular acceleration sensor.

Two embodiment examples of the invention are shown in the following drawing and are explained in more detail in the description.

FIG. 1 shows a side view of a first acceleration sensor;

FIG. 2 shows a top view;

FIG. 3 shows a view in the direction of the arrow;

FIG. 4 shows a diagram;

FIG. 5 shows a side view of an angular acceleration sensor;

FIG. 6 shows a view from the back; and

FIG. 7 shows a top view of an individual part of the sensor.

A base plate 10 of an acceleration sensor is shown and from which a web 11 extends upwardly at a right angle. A leaf spring 12, which is constructed so as to be approximately rectangular and extends so as to be parallel edgewise to the base plate 10, is fastened at the web 11, particularly by means of spot welding. An eddy current disk 13, which is likewise constructed so as to be approximately rectangular and extends in a horizontal manner transversely relative to the leaf spring 12, is fastened at the free end of the leaf spring 12, also paticularly by means of spot welding. The eddy current disk immerses in a cage-shaped flux conducting piece 15 which preferably consists of low-reluctance material. Two square brake magnets 16, 17, which extend toward the brake disk 13 but do not contact it, are arranged in the flux conducting piece 15 at a distance from one another. The width of the flux conducting piece 15 is somewhat greater than the width of the eddy current disk 13, so that the latter can oscillate without difficulty in the flux conducting piece.

At the free end of the leaf spring 12, that is, where the eddy current disk 13 begins, a prolongation 18 extends toward the base plate 10. A sensor magnet 19 is arranged at the lower end of the prolongation 18 and cooperates with a Hall element 20 which is located opposite it and which is fastened at the base plate 10. Evaluating circuits 21 are applied to the base plate adjacent to the Hall element by means of thick- or thin-film technology.

The eddy current disk 13, together with the flux conducting piece 15 and the brake magnets 16, 17, forms an eddy current brake. The brake magnets are magnetized in opposite directions. Because of this magnetization in opposite directions, the magnetic field in the air gap between the eddy current disk 13 and the brake magnets 16, 17 is very inhomogenous, so that the eddy current generation is benefited during the oscillation of the eddy current disk.

By way of example, the acceleration sensor is arranged so as to be perpendicular with respect to the traveling direction of a motor vehicle. The inertia mass in the form of the eddy current disk 13 at the end of the leaf spring 12 is deflected in proportion to the acceleration acting perpendicular relative to the leaf spring. The deflection is determined by means of the spring constant of the leaf spring and the inertia mass. The eddy current damping is effected by means of the movement of the inertia mass--particularly the eddy current disk 13--in the air gap of the magnetic circuit. The oscillation energy is decreased by means of the eddy currents induced during the oscillation. Every desired damping can be achieved by means of a suitable design of the system comprising the leaf spring and magnetic circuit system. The lift of the inertia mass is measured by means of the sensor magnet 19 and the Hall element 20 and is converted into a proportional output voltage, see the diagram according to FIG. 4.

The eddy current disk 13 advisably consists of high-grade aluminum or copper, the leaf spring advisably consists of tombac.

Aside from oscillation damping, the magnetic circuit simultaneously serves as a mechanical stop so that the leaf spring is prevented from being damaged during the occurrence of acceleration peaks. For example, by means of the acceleration sensor, passenger safety devices, e.g., belt tighteners, can be actuated in a motor vehicle, or, in another instance, the delay occurring during deceleration of the vehicle can be measured and the action of an antiskid system can be improved with this signal.

In the angular acceleration sensor, according to FIGS. 5, 6 and 7, a torsion rod 25 is fastened vertically on the base plate 10 and a double arm 26, which extends parallel to the base plate 10, is fastened at its tip. The sensor magnet 19 is fastened, in turn, on one of these, the opposite end forming the eddy current brake disk 26A which immerses in the flux conducting piece 15. The latter is fastened on the base plate 10 and receives the two brake magnets 16, 17. The manner of operation follows in a self-evident manner from the embodiment example which was described first, the only difference being that an acceleration of the angle of rotation is now detected, measured and damped by means of rotating the torsion rod. A torsion wire or another low friction support can also be used instead of a torsion rod.

It is advantageous if the magnetization of the sensor magnet is directed in the movement direction so that there is a linear relationship between the acceleration to be measured and the output voltage of the Hall element.