Switching arrangement and method for a capacitive sensor

A capacitive sensor that includes: a sensing electrode having a capacitance to be measured; an alternating voltage source, configured to apply an alternating voltage to the sensing electrode; a capacitive first transfer device; a measurement circuit configured to measure the capacitance of the sensing electrode; and a switching arrangement. The switching arrangement is configured to alternately, in a first switching state, connect the first transfer device to the sensing electrode to enable a charge transfer from the sensing electrode to the first transfer device and, in a second switching state, connect the first transfer device to the measurement circuit to enable a charge transfer from the first transfer device to the measurement circuit.

TECHNICAL FIELD

The invention relates to a capacitive sensor and to a method for capacitive sensing.

BACKGROUND ART

Capacitive sensors today are used for a vast variety of applications, like input devices (e.g. touchpads, capacitive sliders, touch wheels, etc.), proximity sensors or occupant detection systems.

A capacitive sensor or capacitive sensing device, called by some electric field sensor or proximity sensor, designates a sensor, which generates a signal responsive to the influence of what is being sensed (a person, a part of a person's body, a pet, an object, etc.) upon an electric field. A capacitive sensor generally comprises at least one antenna electrode, to which is applied an oscillating electric signal and which thereupon emits an electric field into a region of space proximate to the antenna electrode, while the sensor is operating. The sensor comprises at least one sensing electrode at which the influence of an object or living being on the electric field is detected. In some (so-called “loading mode”) capacitive occupancy sensors, the one or more antenna electrodes serve at the same time as sensing electrodes. In this case, the measurement circuit determines the current flowing into the one or more antenna electrodes in response to an oscillating voltage being applied to them. The relationship of voltage to current yields the complex impedance between the one or more antenna electrodes and ground. In an alternative version of capacitive sensors (“coupling mode” capacitive sensors), the transmitting antenna electrode(s) and the sensing electrode(s) are separate from one another. In this case, the measurement circuit determines the current or voltage that is induced in the sensing electrode when the transmitting antenna electrode is operating.

While capacitive sensors known in the art are in principle reliable, there is the problem that the sensing electrode is also susceptible to external electric and/or magnetic fields, which can be regarded as “electromagnetic noise”. Since the measurement circuit has to be highly sensitive to perform its normal function, it can also be negatively influenced by such EM noise. This may even lead to erroneous detection or non-detection of an object.

SUMMARY

It is thus an object of the present invention to provide means for a more robust capacitive measurement. This problem is solved by a capacitive sensor and method according to the claims.

The invention relates to a capacitive sensor. The application of the inventive sensor is not limited in any way, but it may in particular be used in automotive systems, e.g. as an occupancy sensor for a vehicle seat or for a smart trunk opener.

The sensor comprises a sensing electrode for capacitively coupling to a counterelectrode to form a capacitance to be measured, and an alternating voltage source, which is configured to operatively coupling an alternating voltage to the sensing electrode.

In one embodiment, the counterelectrode is formed by ground and the alternating voltage of said alternating voltage source is applied to the sensing electrode. In this embodiment operating according in the so-called “loading mode”, the sensing electrode has a capacitance relative to ground, which is influenced by an object between the sensing electrode and ground. The presence of the object can therefore be detected by the change in capacitance of the sensing electrode.

In a different embodiment, the counterelectrode may be a dedicated transmitting antenna electrode for emitting an alternating electric field in response to an alternating signal from the alternating voltage source applied to said counterelectrode. In this case the alternating voltage is induced in said sensing electrode by said alternating electric field coupling into said sensing electrode. In this embodiment operating according in the so-called “coupling mode”, the measurement circuit determines the current or voltage that is induced in the sensing electrode when the transmitting antenna electrode is operating.

The voltage source may be connected directly to the sensing electrode or the transmitting antenna electrode respectively, but there may also be other elements in between. It may also be connected directly or indirectly depending on a switching state of the sensor, as will become clear later. It is preferred that the alternating voltage generated by the alternating voltage source is periodic and thus can be characterized by a (base) frequency. The waveform is in general not limited and may e.g. comprise sinusoidal, triangular, square or rectangular waveforms, although certain waveforms such as are preferred, as will be explained later.

The sensor also comprises a capacitive first transfer device and a measurement circuit configured to measure the capacitance of the sensing electrode. Finally, it comprises a switching arrangement, which is configured to alternately, in a first switching state, connect the first transfer device to the sensing electrode to enable a charge transfer from the sensing electrode to the first transfer device; and, in a second switching state, connect the first transfer device to the measurement circuit to enable a charge transfer from the first transfer device to the measurement circuit.

The first transfer device has a capacitance, which may be the result of one or several capacitive elements being part of the transfer device. In general, the transfer device may also comprise other, non-capacitive elements and of course it may comprise wires, conducting paths, etc for connection purposes.

The switching arrangement normally comprises a plurality of switches, which can be of any suitable type known in the art. In particular, these may be electronic switches, which are controlled by a suitable circuitry to operate synchronously. Even if there is no connection of the individual switches (except for a connection to a common controlled circuitry), they are considered as parts of a single switching arrangement.

The measurement circuit may in principle be a conventional one. It is configured to receive electrical charges (i.e. a current flow) from the first transfer device during the second switching state and uses these electrical charges to measure the capacitance of the sensing electrode. In particular, the measurement circuit may employ an integrating capacitor in combination with a transimpedance amplifier.

An object of the invention is to electrically separate the measurement circuit from the sensing electrode. This is achieved by not transferring electrical charges from the sensing electrode directly to the measurement circuit, but via the first transfer device. The switching arrangement assumes the first and second switching states alternately, i.e. either the connections of the first switching state are established or the connections of the second switching state are established. In the first switching state, the transfer device is connected to the sensing electrode and electrical charges can be transferred from the sensing electrode to the transfer device, i.e. a current flows. In this state, however, the transfer device is not connected to the measurement circuit. Therefore, there is no direct connection between the sensing electrode and the measurement circuit. In the second switching state, the first transfer device is connected to the measurement circuit and electrical charges can be transferred (i.e. a current can flow) to the measurement circuit. In this second switching state, however, the first transfer device is not connected to the sensing electrode and therefore, again, there is no direct connection between the sensing electrode and the measurement circuit.

Therefore, there is at no time a direct connection between the sensing electrode and the measurement circuit. Thus, any electromagnetic noise received by the sensing electrode cannot have an impact on the measurement circuit. The first transfer device works as a protective buffer between the sensing electrode and the measurement circuit. Therefore, the inventive sensor is very robust, even when a sensitive measurement circuit is used, which is susceptible to disturbances from electromagnetic noise. It should also be noted that usually, as will become apparent with the embodiments explained below, the measurement circuit is never connected to the alternating voltage source. In particular, the measurement circuit may always receive a direct voltage, which is easier to handle. It should however be clear that the inventive sensor is not limited to such an embodiment and that other embodiments are also possible.

According to a preferred embodiment, the first transfer device comprises a first transfer capacitor with a first terminal and second terminal, the alternating voltage source is configured to generate an alternating voltage at a first node, and the measurement circuit is connected to a second node and a third node. Moreover, in this embodiment, the switching arrangement is configured to alternately, in the first switching state, connect the first terminal to the sensing electrode and the second terminal to the first node; and in the second switching state, connect the first terminal to the second node and the second terminal to the third node. Here and in the following, “node” refers to a point having a given potential, i.e. if two components are connected to the same node, they are connected to the same potential. This potential, however, may be time-dependent.

It is understood that instead of a single first transfer capacitor, a plurality of capacitors switched in parallel and/or in series could be used. In the embodiment described, the first transfer capacitor and the sensing electrode are connected in series with respect to the alternating voltage source during the first state. During the second switching state, the terminals of the first transfer capacitor are disconnected from the sensing electrode and the alternating voltage source and instead are connected to the measurement circuit via the second and third node. All of the above-mentioned connections are usually direct connections (i.e. without any intermediate elements).

It is also preferred that the measurement circuit comprises an integration capacitor connected to the second node and the third node (i.e. the capacitor has each of its terminals connected to one of these nodes) and a transimpedance amplifier connected to the second node and the third node. Such a configuration is in principle well-known in the art. The integration capacitor usually has a capacitance that is chosen to be much higher than the capacitance of the first transfer device and the expected capacitance of the sensing electrode. The integration capacitor may e.g. have a capacitance with is 100 times larger than expected capacitance of the sensing electrode. Therefore, when the connection between the first transfer device and the measurement circuit is established, the capacitive device(s) of the transfer device will be largely discharged in favor of the integration capacitor.

It is preferred that the alternating voltage source is configured to generate a sinusoidal voltage. While in many common capacitive sensors, a rectangular voltage is used, such a voltage contains, apart from the base frequency, a large amount of higher frequencies, which in turn leads to a considerable amount of radiation. To keep the electromagnetic emissions of the capacitive sensor low, the upper harmonic components should be at least largely eliminated. While in a perfect sine wave, the total harmonic distortion is 0, in a wider sense an alternating voltage may be used that has a total harmonic distortion of less than 5%.

In this context, the switching arrangement may be configured to be in the first switching state when the voltage is rising and is to be in the second switching state when the voltage is dropping. I.e. the switching arrangement is synchronized with the alternating voltage source. Such as synchronization may also be employed in connection with a voltage that is not sinusoidal. If such a non-sinusoidal voltage contains constant portions, the change between the first and second switching state may occur at the start or at the end of such a constant portion.

According to one embodiment, the third node is connected to ground. According to another embodiment, the third node is connected to a constant voltage source. Such a constant voltage source constitutes a bias point for the measurement circuit.

Especially when only a single transfer device is employed, the switching arrangement is preferably configured to connect the sensing electrode to the first node in the second switching state. This means that the sensing electrode will be directly connected to the alternating voltage source during the second switching state. If this is combined with the embodiment where the switching arrangement is synchronized with the alternating voltage source, during the first state, only the sensing electrode is charged by the rising voltage, but in the second switching state, the combination (connection in series) of the sensing electrode and the capacitance of the first transfer device is discharged.

While those embodiments which employ only the first transfer device may be characterized as “asymmetric” with respect to the first and second switching state, there are also embodiments which are more “symmetric”. In these embodiments, the capacitive sensor further comprises a capacitive second transfer device and the switching arrangement is further configured to in the first switching state, connect the second transfer device to the measurement circuit to enable a charge transfer from the second transfer device to the measurement circuit, and, in the second switching state, connect the second transfer device to the sensing electrode to enable a charge transfer from the sensing electrode to the second transfer device.

The second transfer device may be designed in the same way as the first transfer device and therefore will not be explained again. In such an embodiment, there is always a charge transfer enabled between the sensing electrode and one (the first/second) transfer device on the one hand and the other (second/first) transfer device and the measurement circuit on the other hand.

In this context, it is preferred that the second transfer device comprises a second transfer capacitor having a third terminal and a fourth terminal and that the switching arrangement is configured to connect the third terminal to the third node and the fourth terminal to the second node in the first state, and connect the third terminal to the sensing electrode and the fourth terminal to the first node in the second switching state. It should be noted that from the point of view of the alternating voltage source, the first and second transfer capacitor are connected antiparallel with respect to the measurement circuit. In other words, when the switching arrangement is synchronized with the alternating voltage source, the first transfer capacitor receives a rising flank of the voltage (first switching state) while the second transfer capacitor receives a falling flank (second switching state). This leads to the two transfer capacitors being charged with opposite polarity. These polarities are rectified by connecting the capacitors in an antiparallel way to the measurement circuit. It should also be noted that due to the antiparallel arrangement, any direct voltage components are cancelled out.

The invention further provides a method for capacitive sensing with a sensing electrode capacitively coupling to a counterelectrode to form a capacitance to be measured, a capacitive first transfer device and a measurement circuit. According to the method, an alternating voltage is operatively coupled to the sensing electrode. Alternately, in a first switching state, the first transfer device is connected to the sensing electrode to enable a charge transfer from the sensing electrode to the first transfer device, and, in a second switching state, the first transfer device is connected to the measurement circuit to enable a charge transfer from the first transfer device to the measurement circuit. Also, the measurement circuit measures the capacitance of the sensing electrode.

It is understood that an alternating voltage source can be employed to apply the alternating voltage and that the switching arrangement can be employed to establish the connections of the first and second switching state.

Preferred embodiments of the inventive methods correspond to those of the inventive capacitive sensor. For sake of brevity, they will therefore not be discussed again.

DETAILED DESCRIPTION

FIG. 1by way of example illustrates a first embodiment of a capacitive sensor1according to the invention. The sensor1could be arranged in a vehicle seat as an occupancy sensor, in a vehicle bumper as a smart trunk opener, in a handle of a vehicle door as a smart door opener, in a mobile electronic device as part of a touch screen or in other known applications of capacitive sensors. It comprises a sensing electrode2, which is associated with a capacitance CXrelative to ground. The capacitance CXis unknown and varies with the presence of an object approaching or touching the sensing electrode2. The object could be the body of a person, a person's finger or the like.

The sensing electrode2is connectable via a first switch10to an alternating voltage source3. The alternating voltage source3applies a preferably sinusoidal voltage V1(shown inFIG. 3) to a first node7. In a first switching state (indicated by the number1in a circle), the first switch10is open so that there is no direct connection between the sensing electrode2and the alternating voltage source3. In the second switching state (indicated by the number2in a circle), the first switch10is closed so that the sensing electrode2is connected to the first node7and thus to the alternating voltage source3.

A first transfer capacitor Ct1is connected with a first terminal5to a second switch11and with a second terminal6to a third switch12. The first transfer capacitor Ct1basically constitutes a first transfer device4. In the first switching state, as shown inFIG. 1, the first terminal5is connected by the second switch11to the sensing electrode2and the second terminal6is connected by the third switch12to the first node7. In the second switching state, the first terminal5is connected to a second node8and the second terminal6is connected to a third node9. The second node8and the third node are 9 input nodes to a measurement circuit20, which comprises an integrating capacitor Ciand a transimpedance amplifier21. The transimpedance amplifier21is constructed in a known way using an operation amplifier22and an impedance Z, which may be realized by a resistor and a capacitor connected in parallel. The operation amplifier22generates at its output a voltage Voutwhich is indicative of the capacitance CXof the sensing electrode2.

In the embodiment shown, the third node9, which is connected to the non-inverting input of the operation amplifier22, is connected to ground via a direct voltage source15, which generates a constant voltage V2as a bias point for the measurement circuit20. Alternatively, the third node9could also be directly connected to ground.

The first, second and third switch10,11,12are parts of a switching arrangement and change from the first switching state to the second switching state (as indicated inFIG. 1) in a synchronized way. Moreover, they are synchronized to the time evolution of the alternating voltage V1as indicated by the numbers inFIG. 3. When the voltage V1is rising, the switching arrangement assumes the first switching state, and when the voltage V1is dropping, the switching arrangement assumes the second switching state.

In the first switching state, as shown inFIG. 1, the first transfer device4is separated from the measurement circuit20. The first transfer capacitor Ct1is connected in series with the unknown capacitance CX, wherefore a current flows between these two elements.

In the second switching state, the first transfer device4is disconnected from the alternating voltage source3and the sensing electrode2and is instead connected to the measurement circuit20. At this point, the first transfer capacitor Ct1has been charged to a certain amount, which depends on the capacitance CX. Since the capacitance of the integrating capacitor Ciis chosen to be much larger than the capacitance of the first transfer capacitor Ct1, the latter is largely discharged in favor of the integrating capacitor Ci. Also in the second switching state, the sensing electrode2is connected directly to the alternating voltage source3by the first switch10.

Since the measurement circuit20is at no time connected to the sensing electrode2, it is protected from electromagnetic noise which could be received by the sensing electrode2. Therefore, the capacitive sensor1is relatively robust under electromagnetic compatibility (EMC) aspects. Furthermore, the measurement circuit20is at no time exposed to the alternating voltage source3and its alternating voltage V1. It rather is only connected to the first transfer capacitor Ct1, which, for a given capacitance CX, is always charged to a voltage with the same amount and polarity.

Furthermore, since the sensing electrode2is only charged with a sinusoidal voltage, which (at least ideally) does not contain any upper harmonics with higher frequencies, its electromagnetic emissions are largely reduced with respect to e.g. a rectangular voltage.

FIG. 2shows a second embodiment of an inventive capacitive sensor1a, which also comprises a sensing electrode2, an alternating voltage source3and a measurement circuit20. These components are identical to the embodiment shown inFIG. 1and therefore will not be described again.

Again, a first transfer capacitor Ct1of a first transfer device4is connected between two switches11,12, by which, in a first switching state, a first terminal5of the capacitor Ct1is connected to the sensing electrode2and a second terminal6is connected to the first node7connected to the alternating voltage source3. In the second switching state, the first terminal5is connected to the second node8and the second terminal6is connected to the third node9. Like inFIG. 1, the second node8is connected to the inverting input terminal of the operation amplifier22and the third node9is connected to the non-inverting input terminal. UnlikeFIG. 1, the third node9is directly connected to ground.

The sensor1afurther comprises a second transfer device4.1, which comprises a second transfer capacitor Ct2having a third terminal5.1and a fourth terminal6.1, which are connected to two additional switches13,14. In the first switching state, as shown inFIG. 2, the third terminal5.1is connected to the third node9and the fourth terminal6.1is connected to the second node8. In the second switching state, the third terminal5.1is connected to the sensing electrode2while the fourth terminal6.1is connected to the first node7and the alternating voltage source3.

In this embodiment, too, the switches11,12,13,14are part of the switching arrangement, which is synchronized with the alternating voltage V1in the way indicated by the numbers inFIG. 3. In the first switching state, the first transfer device4is connected to the sensing electrode2and the alternating voltage source3. In this state, the alternating voltage V1is rising, which means that the first transfer capacitor Ct1and the capacitance CXare both charged by a positive current. At the same time, the second transfer capacitor Ct2is disconnected from the sensing electrode2and the alternating voltage source3, but connected to the second and third node8,9, which are input nodes to the measurement circuit20. The transfer capacitors Ct1, Ct2have equal capacitance and the integrating capacitor Cihas a capacitance that is much larger. Therefore, in the first switching states, the second transfer capacitor Ct2is discharged in favor of the integrating capacitor Ci.

In the second switching state, when the voltage V1is dropping, the first transfer capacitor Ct1is disconnected from the voltage source3and the sensing electrode2and is instead connected to the second and third node8,9. The second transfer capacitor Ct2, on the other hand, is disconnected from the second and third node8,9and is instead connected between the alternating voltage source3and the sensing electrode2. Now the capacitance CXand the transfer capacitor Ct2are subjected to a negative current, wherefore the second transfer capacitor Ct2is charged with a polarity that is opposite to that of the first transfer capacitor Ct1in the first switching state. Since, however, the terminals5.1,6.1of the second transfer capacitor Ct2are connected to the second node8and the third node9in an opposite way with respect to the terminals5,6of the first transfer capacitor Ct1, the integrating capacitor Ciis charged with the same polarity in both switching states.

It should be noted that in the second embodiment, both the rising flank as well as the falling flank of the voltage V1are used to charge one of the transfer capacitors Ct1, Ct2, both of which are used to charge the integrating capacitor Ci. Therefore, the sensitivity of the capacitive sensor1aaccording to the second embodiment is approximately twice as high as in the first embodiment. Like in the first embodiment, the measurement circuit20is at no time connected to the sensing electrode2, wherefore it is protected from electromagnetic noise which could be received by the sensing electrode2.

The embodiments of the invention shown inFIGS. 1 to 3all relate to a capacitive sensor operating in the so-called “loading mode”. It should however be noted that the principle of the invention applies mutatis mutandis also to a capacitive sensor operating in “coupling mode”.

FIG. 4shows an embodiment of a capacitive sensor in “coupling mode”, which is similar to the embodiment shown inFIG. 1. In the embodiment shown inFIG. 4, the counterelectrode is a dedicated transmitter electrode16and the capacitance to be determined Cxis formed between the sensing electrode2and a dedicated transmitter electrode16. The alternative voltage source3is in this embodiment coupled to the antenna electrode16, while node7is coupled to ground. In operation, the transmitting antenna electrode16emits an alternating electric field in response to the alternating signal from the alternating voltage source3applied to said antenna electrode16. In this case an alternating voltage is induced in said sensing electrode2by said alternating electric field coupling into said sensing electrode2. In this embodiment, the measurement circuit determines the current or voltage that is induced in the sensing electrode when the transmitting antenna electrode is operating.

It should be noted that the operating of the coupling mode sensor ofFIG. 4with respect to the charge transfer is similar to the loading mode sensor ofFIG. 1. It will however be appreciated, that the switching cycles will be inverted with respect to the time evolution of an alternating voltage ofFIG. 3. It will finally be appreciated that the the coupling mode sensor could also be provided with a second transfer device in analogy to the embodiment ofFIG. 2.