The invention described in this application relates to the field of microelectronics, specifically to capacitance measurement circuits and capacitance measurement methods.
The Capacitors typically produce small capacitance outputs, ranging from 0.01 femtofarads (fF) to 10 picofarads (pF). These outputs can be compromised by stray and parasitic capacitances originating from the sensors and their connecting cables. Such interference weakens the capacitance measurement circuit's ability to accurately capture signals. Furthermore, the precision of measurements can be influenced by the capacitive distribution that occurs both before and after the capacitor undergoing tests. This results in a decrease in the overall accuracy of the capacitance measurement circuit.
Therefore, addressing these technical challenges becomes crucial to enhance the circuit's performance and reliability.
The present disclosure presents a few novel circuits and methods for precise capacitance measurements. This comprehensive approach, as outlined across various embodiments, signifies a significant advancement in capacitance measurement technology, promising increased accuracy and reliability in microelectronics applications.
The capacitance measurement circuit comprises an excitation circuit, a regulation circuit, and a capacitor under test. The capacitor being measured connects to the output of the excitation circuit at one end and to the input of the regulation circuit at the other end.
The capacitance measurement circuit also includes an integration comparison circuit, which is electrically connected to the regulation circuit. This integration comparison circuit features first and second timing switch circuits and first and second amplification circuits. The first timing switch is connected to the input of the first amplification circuit and the output of the regulation circuit, while the second timing switch connects to the input of the second amplification circuit and the output of the regulation circuit. These switches are turned on alternately to aid in the measurement process.
Additionally, a capacitance detection circuit, equipped with a differential amplifier and a comparator, enhances the detection accuracy. The differential amplifier's inputs are connected to the outputs of the first and second amplification circuits, facilitating improved signal discrimination.
In some embodiments, the capacitance detection circuit includes: a quantization circuit and a Digital-to-Analog converter (DAC) to further refine measurement precision. The output from the comparator feeds into the DAC, whose outputs link back to the inputs of the first and second amplification circuits.
The DAC is tailored to work with the amplification circuits, ensuring that it accurately processes common-mode signals from the outputs of both amplification circuits for better measurement accuracy.
Each amplification circuit features a unique setup involving an amplifier, a capacitor, and a switch, allowing for precise measurement control. This setup is replicated in both the First and Second Amplification Circuits.
The regulation circuit incorporates a variable capacitor, an amplifier and a switch, enabling fine adjustments to optimize measurement conditions. It also includes a common-mode signal input to further enhance measurement precision.
The detailed design presented here represents a significant improvement in capacitance measurement technology, addressing the issues identified above and offering greater accuracy and reliability for microelectronics applications.
In some embodiments, the output voltage (Vout) from the third amplifier is related to the excitation voltage (Vdrv) produced by the excitation circuit in the following way:
Wherein, A is the amplification factor of the third amplifier, Cs is the capacitance value of the capacitor to be measured, and Cint is the capacitance value of the variable capacitor.
In some embodiments, the capacitance measurement circuit features an additional component: an excitation capacitor. This excitation capacitor is connected at one end to the regulation circuit and at the other end to the integration comparison circuit.
This application also discloses methods for measuring capacitance. One method includes the following steps: First, provide a capacitance measurement circuit from the previously described circuits. During the capacitor's charge sampling phase, connect the capacitor under test to the excitation circuit. Control a first, a second and a third timing switches to the ‘on’ state as dictated by the capacitor control signal. In the integration phase, transfer the sampled charge from the test capacitor into the measurement circuit. Manage the activation of the first timing switch circuit and the sequential activation of the second timing switch circuit based on the control signal. Finally, convert the accumulated charge in the measurement circuit into a voltage signal, and calculate the capacitance value of the test capacitor using this voltage.
The advantages of the invention will become apparent to those skilled in the art considering the following drawings and detailed descriptions.
One or more embodiments are exemplified through the images in the corresponding drawings. These illustrations do not limit the scope of the embodiments, and elements with the same reference numbers in the drawings are similar elements, unless specifically stated otherwise. The drawings are not necessarily to scale.
The embodiments of this application provide capacitor measurement circuits and methods, which address the challenges mentioned above and significantly improve the accuracy of capacitor measurement.
The technical solutions disclosed in this application offer at least the following advantages: The first amplifier circuit, the second amplifier circuit, and the differential amplifier constitute a differential system. If there is low-frequency signal interference from the outside, this interference signal passes through the excitation circuit and is further transmitted to the first and second amplifier circuits. After the differential operation of the differential amplifier, the low-frequency interference signal will be eliminated, thus the entire differential system has strong low-frequency suppression capability. Furthermore, the integration comparison circuit and the capacitor detection circuit form a closed-loop circuit. The signal value collected by the capacitor undergoes multiple comparisons through the integration comparison circuit and the capacitor detection circuit, achieving negative feedback control and conversion of the current signal through the capacitor to be measured. This ensures dynamic balance between the current of the capacitor to be measured and the reference capacitor current, enhancing the stability and acquisition accuracy of the capacitor detection.
To better illustrate the objectives, technical solutions, and advantages of the embodiments of this application, the following disclosure will detail the embodiments of this application in conjunction with the accompanying drawings. However, those skilled in the art will appreciate that the embodiments include numerous technical details to enhance understanding of the application. Despite this, the technical solutions sought to be protected by this application can be realized even without some of these technical details. Various alterations and modifications can be made based on the described embodiments.
The capacitance detection circuit (30) is comprised of two main components: a differential amplifier (AMP4) and a comparator (311). The differential amplifier AMP4 receives two types of input signals: an in-phase input (VinP) and an anti-phase input (VinN). The in-phase input (VinP) is directly connected to the output of the first amplification circuit (21), while the anti-phase input (VinN) is linked to the output of the second amplification circuit (22). The output from the differential amplifier AMP4 is then fed into comparator 311. Following this, the comparator's output passes through a digital-to-analog converter (DAC 321), before being routed to the input ends of both the first and second amplification circuits (21 and 22). This setup ensures a coherent flow of signals for effective capacitance detection and amplification.
The capacitor measurement circuit mentioned above has a wide range of applications, including testing equipment for aerospace, aviation, and naval sectors, as well as electronic devices like laptops, mobile phones, and digital cameras.
In some embodiments, the excitation circuit outputs an excitation voltage Vdrv. The excitation circuit can act as an excitation terminal, generating an excitation signal for the capacitor under test Cs. In other words, the excitation circuit can function as a power source and have Vdrv connecting to the front end of Cs, and the other end of Cs connects to the input to the amplification circuit.
In some embodiments, as can be seen in
One terminal of the variable capacitor (Cint3) is linked to three points: the negative input terminal of AMP3, the input terminal of rst3, and the output from the capacitor being tested (Cs). The opposite terminal of Cint3 connects to two points: the output terminal of AMP3 and the output terminal of rst3. Additionally, the positive input terminal of AMP3 is designed to receive a common-mode signal VCM.
This setup ensures that Cint3 functions within the circuit to facilitate adjustments, potentially affecting the measurement or processing of the signal from the capacitor under test (Cs), with AMP3 amplifying the signal and rst3 providing switching capabilities for circuit configuration or reset purposes.
In some embodiments, the capacitance of the variable capacitor Cint3 can be adjusted within a specific range. This adjustment allows for changes in the gain value of the capacitor measurement circuit, thereby increasing the difference between the maximum and minimum measurable capacitance values. Such an adjustment further enhances the accuracy of the capacitance measurements.
Having detailed the embodiments illustrated in
Rs represents the impedance corresponding to the capacitor under test Cs, and Rint3 represents the impedance corresponding to the variable capacitor Cint3. Based on the formula for calculating impedance, the following equation can be derived:
Here, s=jω, where j is the imaginary unit, and ω is the angular frequency.
Based on the operational amplifier calculation formula for the third op-amp AMP3, we can obtain:
Wherein, A represents the amplification factor of the third amplifier AMP3, and V1 is the voltage between the capacitor under test Cs and the variable capacitor Cint3, which also corresponds to the voltage at the negative input terminal of the third operational amplifier AMP3. From the four equations provided, we can derive equation (5), which expresses the relationship between the output voltage Vout of the third amplifier AMP3 and the excitation voltage Vdrv produced by the excitation circuit.
Since the value of A is generally quite large, often amplifying the voltage by thousands or even tens of thousands of times to meet the amplifier's own performance requirements, equation (5) can be approximated as equation (6).
Based on equation (6), we can determine that by applying a specific excitation voltage Vdrv alongside adjusting the variable capacitor Cint3, it's possible to translate the capacitance of the capacitor under test (Cs) into a corresponding output voltage (Vout). Furthermore, for any given capacitor under test (Cs), altering the capacitance of Cint3 allows for the generation of varying output voltages (Vout) at the same excitation voltage (Vdrv). In essence, modifying the capacitance of the variable capacitor Cint3 is a way to adjust the gain of the circuit.
Turning back to
Similarly, the second amplification circuit (22) includes a second amplifier (AMP2), a second capacitor (Cint2), and a second switch (rst2). One terminal of the second capacitor (Cint2) connects to the negative input terminal of AMP2, a second timing switch circuit (clk2), and the second switch (rst2). The other terminal of Cint2 connects to the output terminal of AMP2 and the other terminal of the second switch (rst2).
Referring to both
Specifically, when rst1, rst2, and rst3 are open, and clk1 is conducting while clk2 is open (non-conducting), Cint1 is charged. For a given drive capacitor (Cdrv) and the first capacitor (Cint1), according to formula (7) below, the first output voltage (V2) after passing through the second stage amplifier can be determined.
By combining formulas (7) and (6), we obtain formula (8), which allows for determining the first amplified output voltage (V2) corresponding to the capacitor under test (Cs) given specified excitation voltage (Vdrv), first capacitor (Cint1), and variable capacitor (Cint3). This achieves the conversion of the capacitor signal of Cs into a voltage signal.
By the same principle, through the second amplification circuit (22), when the first switch (rst1), the second switch (rst2), and the third switch (rst3) are open (non-conducting), with the first timing switch circuit (clk1) open and the second timing switch circuit (clk2) in the conducting state, the second capacitor (Cint2) is charged. Given a specified drive capacitor (Cdrv) and the second capacitor (Cint2), formula (9) can be used to determine the second output voltage (V3) after passing through the second stage amplifier.
By integrating formulas (9) and (6), we obtain formula (10).
This formula indicates that for a specified excitation voltage (Vdrv), the second capacitor (Cint2), and the variable capacitor (Cint3), it is possible to determine the second amplified output voltage (V3) corresponding to the capacitor under test (Cs), facilitating the conversion of Cs's capacitance signal into a voltage signal.
In view of the above and as illustrated in
Specifically, referring to both
Conversely, when the first timing switch circuit (clk1) is in a low state and the second timing switch circuit (clk2) is in a high state, the first timing switch is deactivated (disconnected), and the timing switch corresponding to clk2 is activated (connected). At this rising edge of Vout, the first capacitor (Cint1) remains inactive, while the second capacitor (Cint2) carries out charge transfer. Consequently, the integration comparison circuit 20 outputs the second amplified output voltage V3 corresponding to the capacitor under test (Cs), after being amplified twice by the second amplifier AMP2, which samples and amplifies the high voltage of the output voltage Vout. Through this sequence of control, a differential sampling process of the output voltage Vout signal is achieved.
In some embodiments, see, e.g.,
The fourth amplification circuit includes a fourth capacitor (Cint4) and a fourth switch (rst4), with one end of Cint4 connected to the non-inverting input of AMP4 and rst4, and the other end connected to the output of AMP4 and the other side of rst4.
The fifth amplification circuit consists of a fifth capacitor (Cint5) and a fifth switch (rst5), with one end of Cint5 connected to the inverting input of AMP4 and rst5, and the other end connected to the output of AMP4 and the other side of rst5.
The first measurement circuit is used to collect the capacitance value (C1) corresponding to the first output voltage (V2), and the second measurement circuit is used to collect the capacitance value (C2) corresponding to the second output voltage (V3).
The first measurement circuit is connected at one end to the first amplification circuit (21) and at the other end to the D/A conversion circuit. The first measurement circuit includes a third timing switch circuit (clk3) connected to a capacitor (C1). The second measurement circuit is connected at one end to the second amplification circuit (22) and at the other end to the D/A conversion circuit; it includes a fourth timing switch circuit (clk4) connected to another capacitor (C2).
In some embodiments, the output of the D/A conversion circuit is connected to the inverting input of the first amplifier (AMP1) in the first amplification circuit (21), and similarly, the D/A conversion circuit output is connected to the inverting input of the second amplifier (AMP2) in the second amplification circuit (22).
In some embodiments, the Digital-to-Analog (D/A) conversion circuit features a D/A converter (321). This converter generates the common-mode signal (VCM) using the first output voltage (V2) from the first amplification circuit (21) and the second output voltage (V3) from the second amplification circuit (22). Subsequently, VCM is connected to the non-inverting (positive) input of the first amplifier (AMP1) within the first amplification circuit (21) and to the non-inverting (positive) input of the second amplifier (AMP2) within the second amplification circuit (22), respectively.
In some embodiments, referring to
The positive input terminals of AMP1 and AMP2 receive a common-mode signal (VCM), while their negative input terminals receive a feedback signal (error signal). AMP1 and AMP2 perform a differential (delta) comparison on the input common-mode signal (VCM) and the feedback signal. The differential output from this comparison is fed into the differential amplifier AMP4 (sigma), whose output, in turn, is fed into the comparator (311). Each alternate operation of AMP1 and AMP2 reduces the difference between the first output voltage (V2) and the second output voltage (V3). The result of each operation, comp_out, is transmitted to the DAC (321) along with the readings of the first output voltage (V2) and the second output voltage (V3) from the first and second sub-capacitors (C1 and C2). Thus, each comparison result, comp_out, forms a digital signal in the DAC (321) and is fed back to the negative input terminals of AMP1 and AMP2.
It is noted that after multiple comparison cycles involving alternate activation of the first and second timing switch circuits (clk1 and clk2), a capacitance value for the capacitor under test (Cs) is obtained with certain precision. Here, the integration amplifier circuit (20) and the capacitance detection circuit form a closed-loop, allowing for multiple comparisons of the signal value collected by the capacitance. This proposed process implements negative feedback control and conversion of the current signal through the capacitor under test, achieving dynamic balance between the current through the capacitor under test and the reference capacitor current. This approach enhances the stability and precision of capacitance detection.
When the first switch (rst1), the second switch (rst2), and the third switch (rst3) are closed, the first capacitor (Cint1), the second capacitor (Cint2), and the variable capacitor (Cint3) are discharged and perform charge transfer. Due to the closed-loop characteristics of the amplifiers, the first input voltage (V1) at the negative input of the third amplifier (AMP3), the first output voltage (V2) at the negative input of the first amplifier (AMP1), and the second output voltage (V3) at the negative input of the second amplifier (AMP2) all become a common-mode signal (VCM). This resets the circuit to its state before the capacitance sampling, completing a cycle of the capacitance measurement process.
Furthermore, when there is low-frequency signal interference from the outside, this interference signal is transmitted through the excitation circuit and further to the first amplification circuit (21) and the second amplification circuit (22). After differential processing by the differential amplifier (AMP4), the low-frequency interference is eliminated, giving the entire system a strong low-frequency suppression capability.
Some embodiments also include an excitation capacitor (Cdrv), one end of which is connected to the adjustment circuit (11) and the other end to the integration comparison circuit (20).
In summary, the approach outlined above introduces a differential system that includes the first and second amplification circuits (21 and 22) along with the differential amplifier (AMP4). This configuration is particularly effective in eliminating low-frequency interference signals. It does so by utilizing differential processing with AMP4, which significantly improves the system's ability to filter out low-frequency noise. Furthermore, the integration amplifier circuit (20) works in conjunction with the capacitance detection circuit to create a feedback loop. This setup facilitates repeated comparisons of the signal from the capacitor under test (Cs), enabling negative feedback control and signal conversion. The process ensures a balance between the currents of the test capacitor and a reference capacitor, ultimately enhancing the accuracy and stability of capacitance measurements.
In line with this application, we introduce a method for measuring capacitance that utilizes the capacitance measurement circuit described earlier. The method unfolds in two main phases:
The specifics of this capacitance measurement method have been outlined in the preceding examples and will not be repeated here for brevity.
The various embodiments are categorized for ease of description and do not limit the specific implementations of this application. They can be combined and referenced interchangeably, provided there are no contradictions.
The division of steps in these methods is for clarity of description. In implementation, they can be combined into one step or further divided into multiple steps, if they maintain the same logical relationship. Any minor modifications or non-essential additions to the algorithm or process that do not change its core design are within the scope of this disclosure.
Those skilled in the art will understand that the above embodiments are specific implementations of this application, and various modifications can be made in form and detail in actual applications without departing from the spirit and scope of this application.
Number | Date | Country | Kind |
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202210352792.3 | Apr 2022 | CN | national |
This application is a continuation of an international application with application number PCT/CN2022/099288, filed on Jun. 16, 2022, which claims priority to a Chinese patent application with application number 202210352792.3, filed on Apr. 6, 2022, the entire content of which is hereby incorporated by reference into this application.
Number | Date | Country | |
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Parent | PCT/CN2022/099288 | Jun 2022 | WO |
Child | 18638750 | US |