The description relates to inductive (LC) sensors.
One or more embodiments may apply to LC sensors for use, e.g., in fluid metering applications, such as water and gas meters.
Inductive sensing is based on an inductor-capacitor resonant circuit (which explains the current designation of “LC sensing”) which is pumped by an oscillator with the inductor acting as a sensing coil. As a conductive (e.g., metal) object comes in the vicinity of the coil, currents are generated in the object depending on various parameters such as, e.g., the material and dimensions of the object and/or the distance to the sensing coil. The currents thus generated form a magnetic field which reduces the oscillation amplitude of the resonant circuit (tank) thus changing the parallel resonance impedance of the circuit. Detecting/measuring such change may be exploited for various sensing purposes.
Inductive/LC sensing may be used in various industrial fields for, e.g., various types of contactless sensing of moving parts for various purposes such as detecting/measuring distance, speed or flow.
For instance, inductive/LC sensing is being increasingly applied, e.g., in water and gas meter applications with the possibility of offering power/efficient solution adapted to be directly embedded, e.g., in microcontroller units—MCUs.
In such a possible context of use, factors such as, e.g., reducing the number of (analog) components coupled with the sensor, facilitating digital processing of the sensing signals and simplifying control logic while providing reduced consumption may play a significant role.
Reducing the time involved in performing a certain measurement and/or the capability of handling multiple sensors represent a further factors of interest.
Time-based LC sensor excitation using, e.g., a high-speed (e.g., 4 MHz) clock source to control transfer of energy during excitation has been used with potential drawbacks represented, e.g., by power consumption and total measurement times in the range of, e.g., 50 microseconds.
One or more embodiments are directed to a method that includes accumulating excitation energy for an inductive-capacitive (LC) sensor, oscillating the LC sensor using the excitation energy accumulated, detecting the excitation energy accumulated reaching a charge threshold, and terminating accumulating the excitation energy for the LC sensor in response to detecting the excitation energy accumulated reaching the charge threshold.
One or more embodiments also relate to a corresponding system as well as to apparatus (e.g., metering device such as a water or gas meter) including such a system.
The claims are an integral part of the disclosure of one or more embodiments as provided herein.
One or more embodiments may offer one or more of the following advantages:
reduce the power absorption (no high-speed clock needed)
insensitivity to Power Voltage-Temperature—PVT factors, (due to the possibility of resorting to closed-loop control),
robustness against PVT variations also in the field, that is in current operation.
One or more embodiments will now be described, by way of example only, with reference to the annexed figures, wherein:
In the ensuing description, one or more specific details are illustrated, aimed at providing an in-depth understanding of examples of embodiments. The embodiments may be obtained without one or more of the specific details, or with other methods, components, materials, etc. In other cases, known structures, materials, or operations are not illustrated or described in detail so that certain aspects of embodiments will not be obscured.
Reference to “an embodiment” or “one embodiment” in the framework of the present description is intended to indicate that a particular configuration, structure, or characteristic described in relation to the embodiment is comprised in at least one embodiment. Hence, phrases such as “in an embodiment” or “in one embodiment” that may be present in one or more points of the present description do not necessarily refer to one and the same embodiment. Moreover, particular conformations, structures, or characteristics may be combined in any adequate way in one or more embodiments.
The references used herein are provided merely for convenience and hence do not define the extent of protection or the scope of the embodiments.
The schematic diagram of
The schematic diagram of
For instance, the rotary plate P may include complementary portions of different materials (e.g., conductive and non-conductive). One or more LC sensors 10 arranged facing the plate P may thus produce signals indicative of rotation of the plate P (and thus of the flow in the conduit C) for processing in a controller, e.g., a microcontroller unit—MCU.
The general principles underlying the structure and operation of such metering device are otherwise known in the art, which makes it unnecessary to provide a more detailed description herein. Also, it will be appreciated that the application exemplified in
In one or more embodiments, operation of an LC sensor 10 as exemplified herein may generally involve at least one charging phase wherein excitation energy for the sensor 10 is accumulated. The LC sensor (here exemplified as the parallel connection of an inductor Ls and a capacitor Cs) may thus oscillate energized by the energy accumulated to permit sensing to take place as outlined in the introduction to this description.
In conventional solutions, energy accumulation (charging) may be stopped at a certain time as defined, e.g., by a high-frequency (e.g., 4 MHz clock source).
By way of contrast, one or more embodiments as exemplified herein may provide for detecting (e.g., by a charge sensor/energy meter 12) the fact that the energy accumulated has reached a certain charge accumulation threshold, with operation switched towards the sensing phase when the charge threshold is detected to be reached.
In one or more embodiments as exemplified in
One or more embodiments as exemplified in
When the switch S1 is closed, that is conductive, the reference capacitor Cref is set between the source V and ground, and the sensor 10 may be set between the source V and the switch S2, with the switch S2 set between the sensor 10 and ground.
In one or more embodiments, operation of the circuit layout exemplified in
pre-charge of Cref: S2 is open—that is non-conductive—so that the sensor 10 is “floating” with respect to ground, and S1 is closed—that is conductive—until the voltage on Cref reaches a value VCref_INIT (<=V) with S1 subsequently open—that is non-conductive;
energy transfer: S1 is open and S2 closed, so that the energy accumulated on Cref is (partially) transferred onto the sensor 10 (which is substantially in parallel to Cref). Controlled transfer of energy terminates when the voltage across Cref reaches a final target value VCref_FIN, after which the switch S2 is opened. In that way, the amount of energy transferred is (ideally) equal to 0.5 Cref(VCref_INIT−VCref_FIN)2;
measurement: both S1 and S2 are open. The sensor will start oscillating around the voltage value VCref_FIN, with such oscillation adapted to be monitored via the pin towards the switch S2.
The circuit may then be reset and the sequence exemplified in the foregoing repeated for a new measurement.
In one or more embodiments, operation of the circuit layout exemplified in
pre-charge of Cref: S2 is open and the energy meter 12 monitors that Cref is charged to an energy accumulation threshold voltage, e.g., V;
energy transfer: S2 is closed and the energy accumulated on Cref is partially transferred onto the sensor 10. Controlled transfer of energy terminates when the voltage across Cref reaches a final target value VCREF FIN, after which the switch S2 is opened. In that way, the amount of energy transferred is (ideally) equal to 0.5 CreF(V−VCref_FIN)2. The energy from the generator may be neglected due to the high value of the time constant.
measurement: S2 is open. The sensor will start oscillating around the voltage value VCref_FIN, with such oscillation adapted to be monitored via the pin towards the switch S2. The voltage variation on Cref due to re-charging via the generator V may again be neglected due to the time constant T=R*Cref being much higher than the time needed for performing the measurement.
In one or more embodiments as exemplified in
In one or more embodiments as exemplified in
In one or more embodiments as exemplified in
In one or more embodiments, operation as described above may involve both excitation of the sensor 10 and charging the capacitor Cref (that is the sensor 10 is excited by the current flowing through Cref).
Such a charging/excitation process terminates when the charge, that is the voltage on Cref reaches a target threshold value.
By way of reference to the exemplary layouts of
In one or more embodiments as exemplified in
The circuit may then be reset and the sequence exemplified in the foregoing repeated for a new measurement.
In comparison with the exemplary circuit layout of
a second switch S2 (again an electronic switch such as a MOSFET: the same designation of
the energy meter 12 configured for driving the switches S1 and S2 as a function of the voltage at a point between the switch S1 and the sensor 10.
In one or more embodiments, operation of the circuit layout exemplified in
excitation: S1, S2 both closed, with the sensor 10 set between the voltage V and ground. The energy meter 12 is sensitive to the amount of energy transferred; Cref kept uncharged as it is grounded on both sides;
post excitation and generation of Vref: S1 closed and S2 open. Charging of the sensor 10 is completed and the capacitor Cref is charged to a final value VCre_FIN;
measurement: S1 and S2 both open, with the sensor oscillation about the voltage VCref_FIN, and oscillation adapted to be monitored on the “floating” pin of the switch S1 opposed to the source V.
Various other implementations are feasible in one or more embodiments.
Just to mention one possibility, in one or more embodiments, the switch S2 may connect directly Cref to the generator V, so that VCref_FIN may be generated directly instead of via the sensor 10.
The circuit diagrams of
In
The circuit diagrams of
The circuit diagrams of
a clock-less charge sharing scheme, including a pre-charge step where a reference capacitor Cref is preloaded by a PAD IO1 with a maximum voltage (Vdd) and a second step where the accumulated energy is transferred to the sensor 10 to excite and generate the reference voltage on Cref (
a clock-less direct charge scheme, where excitation of the sensor 10 and generation of the reference voltage are driven by two PADs, e.g., IO1, IO2, with two charge steps, e.g., pre-charge and post-charge (
A direct charge mechanism may permit to use a smaller Cref with respect to a charge-sharing scheme.
In one or more embodiments as exemplified in
One or more embodiments as exemplified in
In one or more embodiments, operation of an arrangement as exemplified in
reset and pre-charge: both switches S1 and S2 are closed to Vdd, the sensor 10 will be discharged while Cref is precharged to Vdd. The residual energy in the capacitor (Vmid voltage) is held and used as starting point for this step;
charge sharing: the switch S1 is open while the switch S2 is closed to GND. With this configuration Cref provides the energy required to load the sensor 10. This step will be completed when the trigger IO1 (ZI input) reaches a logic “0” (with the IO1 voltage at VthL). The amount of transferred energy is 0.5 Cref (Vdd−Vthl)2;
sensor oscillation: both switches S1 and S2 are open and the oscillation may be monitored via the IO2/ZI pin.
In fact, the voltage Vmid=VthL about which oscillation takes place may be present on IO1 while VIO2=Vsensor+VIO1=>VIO2=(Vsensor+VthL)/ZI pin.
In the arrangement exemplified in
In one or more embodiments as exemplified in
providing the current to charge/reset the sensor 10 and Cref;
triggering the start of the post-charge phase (IO1 Schmitt trigger 141).
In one or more embodiments as exemplified in
discharging the sensor 10 during a reset state;
triggering the end of a post-charge phase looking at its voltage level (Schmitt trigger 142);
tuning and controlling the voltage on Cref during the oscillation time.
In one or more embodiments, operation of an arrangement as exemplified in
reset: switch S1 and switch S2 are closed to GND, both the sensor 10 and the capacitance Cref are shorted to GND;
pre-charge: the switch S1 is closed to Vdd while the switch S2 is closed to GND. In this initial phase the inductor Ls can be assumed to be an open circuit for an exemplary sensor 10, with the capacitor Cs set between Vdd and GND and Cref connected to GND, so that the sensor capacitor Cs will be charged; the pre-charge duration will be completed when the IO1 trigger (ZI input) reaches, e.g., a “1” logic level, with Cs pre-charged to a value VthH so that the energy transferred to the sensor 10 is 0.5 Cs VthH2;
post-charge: the switch S1 is closed to Vdd while the switch S2 is open (high impedance). In this step sensor excitation will be completed and the reference voltage on Cref generated. The post-charge will be completed when the IO2 trigger (ZI input) will reach a “1” logic level. At the end of this step Cref will be pre-charged to VthH and the sensor fully charged. For high values of Cref the sensor inductor current may not be negligible, and the PAD IO1 will provide both the energy for the inductor Ls plus the energy for Cref;
Vref range stabilization and oscillation measure: when the IO2 voltage reaches VthH, the switch S1 will be open (end of post-charge step) while the switch S2 will be configured to keep the IO2 voltage below VthH: the PAD will drive a logic “0” (PullDown or PushPull depending of register configuration) any time that the IO2/ZI is one. The IO2 configuration ensures that the Cref voltage is kept below the VthH voltage value: for instance, for 5 Volt-tolerant PADs there are some parasitic effects (diode) that may increase the Vref voltage during oscillation of the sensors 10 in case this goes below GND. The dumped oscillation will be observed by the IO1/ZI pin.
In one or more embodiments exemplifies herein, the final part of the smooth oscillation may cross the trigger threshold (Vth) with a reduced slope, which may expose the device at the noise: some extra pulse can be generated if a noise with a sufficient amplitude occurs near the Vth crossing. In one or more embodiments, noise immunity may be pursued by reducing the time over which the smooth oscillation is near the Vth threshold. In one or more embodiments that result may be achieved by moving the detection phase near the first phase of the oscillation where the slope of the waveform is sharpest and/or by moving dynamically the Vmid voltage during the measurement time.
The first solution may be applied by reducing the Vmid voltage value. For a clock-less charge-sharing solution as exemplified in
Without prejudice to the underlying principles, the details and embodiments may vary, even significantly, with respect to what has been described by way of example only, without departing from the extent of protection.
The various embodiments described above can be combined to provide further embodiments. These and other changes can be made to the embodiments in light of the above-detailed description. In general, in the following claims, the terms used should not be construed to limit the claims to the specific embodiments disclosed in the specification and the claims, but should be construed to include all possible embodiments along with the full scope of equivalents to which such claims are entitled. Accordingly, the claims are not limited by the disclosure.
Number | Date | Country | Kind |
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102015000050292 | Sep 2015 | IT | national |
Number | Date | Country | |
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Parent | 15070509 | Mar 2016 | US |
Child | 16136121 | US |