CN103487662B - Capacitive detection circuit - Google Patents
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Abstract
本发明涉及检测电路,公开了一种电容检测电路。该电容检测电路,包含积分电容Ci、待检测电容Cs、电流源A、运算放大器A0和信息处理芯片;待检测电容Cs、积分电容Ci和电流源A的一端分别与运算放大器A0的负输入端相连,待检测电容Cs和电流源A的另一端接地,积分电容Ci的另一端与运算放大器A0的输出端相连,运算放大器A0的正输入端接地,这样接通电路后,待检测电容Cs上的电荷将一部分通过一个电流源A转移,另一部分电荷则转移至积分电容Ci上,这样就可以在不额外增加积分电容Ci面积的前提下减小一次电荷转移过程中运算放大器A0输出端电压变化的大小△Vout,进而增大检测的电容值范围,由于在检测过程中并不降低检测电压,也不会引起信噪比的下降。
The invention relates to a detection circuit and discloses a capacitance detection circuit. The capacitance detection circuit includes an integrating capacitor Ci, a capacitor to be detected Cs, a current source A, an operational amplifier A0 and an information processing chip; one end of the capacitor to be detected Cs, the integrating capacitor Ci and the current source A is respectively connected to the negative input terminal of the operational amplifier A0 The other end of the capacitor Cs to be detected is connected to the current source A, the other end of the integrating capacitor Ci is connected to the output terminal of the operational amplifier A0, and the positive input terminal of the operational amplifier A0 is grounded. After the circuit is connected, the capacitor Cs to be detected Part of the charge will be transferred through a current source A, and the other part of the charge will be transferred to the integral capacitor Ci, so that the voltage change at the output terminal of the operational amplifier A0 during a charge transfer process can be reduced without additionally increasing the area of the integral capacitor Ci. The size of △Vout, and then increase the detection range of capacitance value, because the detection voltage is not reduced during the detection process, it will not cause a decrease in signal-to-noise ratio.
Description
技术领域technical field
本发明涉及电子领域,特别涉及电容检测电路。The invention relates to the field of electronics, in particular to a capacitance detection circuit.
背景技术Background technique
目前,电容触摸技术发展迅速,给人们生活带来了很大便利,该技术首先将触控检测区域划分为若干横竖相交的格点,再通过检测格点电容值的变化,得出的触摸点的位置信息。At present, the rapid development of capacitive touch technology has brought great convenience to people's life. This technology first divides the touch detection area into a number of grid points that intersect horizontally and vertically, and then detects the change of the capacitance value of the grid points to obtain the touch point location information.
电容触摸技术如果按照具体实现来分类,则包括电容按键,自感电容屏,互感电容屏。其中电容按键和自感电容屏中,其待测电容大小变换范围很大,一些小的触摸电路板中,自感电容容值只有几皮法,而在一些大的电容触摸屏,或者大的电容按键中,其自感电容值可能达到上百皮法。If the capacitive touch technology is classified according to the specific implementation, it includes capacitive buttons, self-inductance capacitive screens, and mutual-inductance capacitive screens. Among them, in capacitive buttons and self-inductance capacitive screens, the capacitance to be measured can vary widely. In some small touch circuit boards, the self-inductance capacitance is only a few picofarads, while in some large capacitive touch screens, or large capacitance In the button, its self-inductance capacitance value may reach hundreds of picofarads.
传统的检测方式的检测原理为:当积分开始时,在第一个阶段,如图1所示,积分电容Ci进行清零复位,待检测电容Cs则被充电至参考电压Vref,这个阶段可以称之为采样阶段。在第二个阶段,通过开关将Cs上端与运算放大器A0的负输入端相连,如图2所示。假设运算放大器理想,则在第二个阶段结束时,运算放大器输入端电压相等;此时,采样电容Cs两端电位均为零,即待检测电容Cs上的电荷全部转移至了积分电容Ci,此阶段称为电荷转移阶段或积分阶段。这两个阶段合起来称为一个电荷转移周期或者称为积分周期,在实际使用中,会根据需要进行反复的电荷转移,即实现积分,值得注意的是,积分电容Ci的清零只有在积分开始的第一个积分周期发生。根据电荷守恒原理,可以得出每次电荷转移后,运算放大器输出电压的变化为:The detection principle of the traditional detection method is: when the integration starts, in the first stage, as shown in Figure 1, the integration capacitor Ci is reset to zero, and the capacitor Cs to be detected is charged to the reference voltage Vref. This stage can be called It is the sampling stage. In the second stage, the upper end of Cs is connected with the negative input end of operational amplifier A0 through a switch, as shown in Fig. 2 . Assuming that the operational amplifier is ideal, at the end of the second stage, the voltage at the input terminal of the operational amplifier is equal; at this time, the potential at both ends of the sampling capacitor Cs is zero, that is, all the charges on the capacitor Cs to be detected are transferred to the integrating capacitor Ci, This phase is called the charge transfer phase or the integration phase. These two stages together are called a charge transfer cycle or an integration cycle. In actual use, repeated charge transfers will be performed as needed, that is, to achieve integration. It is worth noting that the reset of the integration capacitor Ci is only Beginning of the first integration cycle occurs. According to the principle of charge conservation, it can be concluded that after each charge transfer, the change of the output voltage of the operational amplifier is:
其中ΔVout为一次电荷转移引起运算放大器的输出电压的变化大小。该电压大小通过模数转换器检测送往数字电路处理,便可判断出待检测电容Cs的电容值。Among them, ΔVout is the variation of the output voltage of the operational amplifier caused by a charge transfer. The magnitude of the voltage is detected by an analog-to-digital converter and sent to a digital circuit for processing, so that the capacitance value of the capacitor Cs to be detected can be determined.
然而,在实际应用中,为提高抗干扰能力,Vref尽可能取高,为方面描述,假定电容检测电路的电源为3.3V,Vref也为3.3V,这在常规应用中是很普遍的,假设待检测电容为100皮法,积分电容为20皮法,则每个转移周期引起的运算放大器的输出电压变化为16.5V,这严重超过了电源电压值3.3V。如果通过增大积分电容的方式去减少每次转移引起的输出电压变化,则需要100皮法以上的积分电容才能保证一次转移不会超出运算放大器的承受范围,然而,实现100皮法的电容在集成电路中需要很大的面积。即使是20皮法电容的面积也相当可观,而且如果通过增大积分电容的方式去解决输出电压变化太大的问题,则该电路应用于外部待检测电容Cs很小的情况时,每次转移引起运放输出电压的变化将会非常微小,这样会降低运放输出的信噪比。However, in practical applications, in order to improve the anti-interference ability, Vref should be as high as possible. For the sake of description, it is assumed that the power supply of the capacitance detection circuit is 3.3V, and Vref is also 3.3V. This is very common in conventional applications. Suppose The capacitance to be detected is 100 picofarads, and the integrating capacitance is 20 picofarads, so the output voltage change of the operational amplifier caused by each transfer cycle is 16.5V, which seriously exceeds the power supply voltage value of 3.3V. If the output voltage change caused by each transfer is reduced by increasing the integral capacitor, an integral capacitor of more than 100 picofarads is required to ensure that a transfer will not exceed the tolerance range of the operational amplifier. However, the capacitance of 100 picofarads is achieved in A large area is required in an integrated circuit. Even the area of a 20 picofarad capacitor is quite considerable, and if the problem of too much output voltage variation is solved by increasing the integral capacitor, the circuit is applied to the case where the external capacitor Cs to be detected is small, and each transfer The change in the output voltage of the op amp will be very small, which will reduce the signal-to-noise ratio of the output of the op amp.
由此可见,采用传统的电容检测技术,待检测电容值的范围将被限制在大约3皮法~30皮法的范围。It can be seen that, using the traditional capacitance detection technology, the range of the capacitance value to be detected will be limited to a range of approximately 3 picofarads to 30 picofarads.
发明内容Contents of the invention
本发明的目的在于提供一种电容检测电路,通过在电路中额外添加电流源,使该电容检测电路可以在待检测电容很大的情况下也可以对其进行检测。The object of the present invention is to provide a capacitance detection circuit. By adding an additional current source in the circuit, the capacitance detection circuit can detect the capacitance to be detected even when it is very large.
为解决上述技术问题,本发明提供了一种电容检测电路,包含积分电容、待检测电容、电流源、运算放大器和信息处理芯片;In order to solve the above technical problems, the present invention provides a capacitance detection circuit, which includes an integrating capacitance, a capacitance to be detected, a current source, an operational amplifier and an information processing chip;
所述待检测电容的一端与所述运算放大器的负输入端相连,另一端接地;One end of the capacitance to be detected is connected to the negative input end of the operational amplifier, and the other end is grounded;
所述积分电容的一端与所述运算放大器的负输入端相连,另一端与所述运算放大器的输出端相连;One end of the integrating capacitor is connected to the negative input end of the operational amplifier, and the other end is connected to the output end of the operational amplifier;
所述电流源的一端与所述运算放大器的负输入端相连,另一端接地;One end of the current source is connected to the negative input end of the operational amplifier, and the other end is grounded;
所述运算放大器的正输入端接地;The positive input terminal of the operational amplifier is grounded;
所述信号处理芯片的一端与所述运算放大器的输出端相连,另一端输出所述电容检测电路检测到的电容值。One end of the signal processing chip is connected to the output end of the operational amplifier, and the other end outputs the capacitance value detected by the capacitance detection circuit.
与现有技术相比,本发明中的电容检测电路增加了一个电流源,该电流源可以吸取或灌送Cs上的部分电荷,Cs上的另一部分电荷则转移至Ci上,这样就可以在不额外增加积分电容Ci面积的前提下减小△Vout,进而增大检测的电容值范围。并且在检测过程中并不降低检测电压,因此也不会引起信噪比的下降。Compared with the prior art, the capacitance detection circuit in the present invention adds a current source, which can absorb or pour part of the charge on Cs, and another part of the charge on Cs is transferred to Ci, so that it can be Decrease △Vout without additionally increasing the area of the integrating capacitor Ci, thereby increasing the range of detected capacitance values. And the detection voltage is not lowered during the detection process, so the signal-to-noise ratio will not be reduced.
优选地,本发明中的电流源在电荷转移过程中可以根据应用情况合理设置该电流源的电流大小和开通时间,使△Vout始终保持在运算放大器A0的承受范围之内,进一步准确地检测出大范围的电容值。Preferably, the current source in the present invention can reasonably set the current size and turn-on time of the current source according to the application during the charge transfer process, so that ΔVout is always kept within the tolerance range of the operational amplifier A0, and further accurately detects wide range of capacitance values.
另外,本发明根据电荷转移理论,利用以下公式计算所述待检测电容的电容值:In addition, the present invention uses the following formula to calculate the capacitance value of the capacitor to be detected according to the charge transfer theory:
Vref*Cs=ΔVout*Ci+I*TVref*Cs=ΔVout*Ci+I*T
其中,所述ΔVout为一次电荷转移后所述运算放大器的输出端电压变化的大小,所述Vref为所述待检测电容在采样阶段中被充至的参考电压,所述Cs为所述待检测电容的电容值,所述Ci为所述积分电容的电容值,所述I为所述电流源的电流值,所述T为所述电流源开通的时间。Wherein, the ΔVout is the magnitude of the voltage change at the output terminal of the operational amplifier after a charge transfer, the Vref is the reference voltage to which the capacitor to be detected is charged in the sampling phase, and the Cs is the voltage to be detected The capacitance value of the capacitor, the Ci is the capacitance value of the integrating capacitor, the I is the current value of the current source, and the T is the opening time of the current source.
由于上述公式中的ΔVout、Vref、Ci、I、T均为已知数,因此可以很方便的计算出待检测电容Cs的电容值。Since ΔVout, Vref, Ci, I, and T in the above formula are all known numbers, the capacitance value of the capacitor Cs to be detected can be easily calculated.
进一步,本发明中的电容检测电路有两种工作模式,一种是Cs向Ci灌送电荷的反向积分模式,一种是Cs从Ci吸取电荷的正向积分模式,适用范围更加广泛。Further, the capacitance detection circuit in the present invention has two working modes, one is the reverse integration mode in which Cs feeds charge to Ci, and the other is the forward integration mode in which Cs absorbs charge from Ci, and the scope of application is wider.
此外,本发明中电容检测电路中的信号处理芯片还包含模数转换器和数字电路处理器,该模数转换器将运算放大器的输出端电压进行模数转换,得到该输出端电压的数字信号,并将该数字信号输送给数字电路处理器,该数字电路处理器再根据公式Vref*Cs=ΔVout*Ci+I*T,计算出待检测电容的电容值。In addition, the signal processing chip in the capacitance detection circuit in the present invention also includes an analog-to-digital converter and a digital circuit processor, and the analog-to-digital converter performs analog-to-digital conversion on the output terminal voltage of the operational amplifier to obtain a digital signal of the output terminal voltage , and send the digital signal to the digital circuit processor, and the digital circuit processor calculates the capacitance value of the capacitor to be detected according to the formula Vref*Cs=ΔVout*Ci+I*T.
附图说明Description of drawings
图1是根据现有技术中电容检测电路的采样阶段示意图;FIG. 1 is a schematic diagram of a sampling stage according to a capacitance detection circuit in the prior art;
图2是根据现有技术中电容检测电路的电荷转移阶段示意图;2 is a schematic diagram of a charge transfer stage according to a capacitance detection circuit in the prior art;
图3是根据本发明第一实施方式的电容检测电路的采样阶段示意图;3 is a schematic diagram of a sampling stage of a capacitance detection circuit according to a first embodiment of the present invention;
图4是根据本发明第一实施方式的电容检测电路示意图;4 is a schematic diagram of a capacitance detection circuit according to a first embodiment of the present invention;
图5是根据本发明第二实施方式中的正向积分模式电容检测电路示意图。FIG. 5 is a schematic diagram of a capacitance detection circuit in a forward integration mode according to a second embodiment of the present invention.
具体实施方式detailed description
为使本发明的目的、技术方案和优点更加清楚,下面将结合附图对本发明的各实施方式进行详细的阐述。然而,本领域的普通技术人员可以理解,在本发明各实施方式中,为了使读者更好地理解本申请而提出了许多技术细节。但是,即使没有这些技术细节和基于以下各实施方式的种种变化和修改,也可以实现本申请各权利要求所要求保护的技术方案。In order to make the object, technical solution and advantages of the present invention clearer, various embodiments of the present invention will be described in detail below in conjunction with the accompanying drawings. However, those of ordinary skill in the art can understand that, in each implementation manner of the present invention, many technical details are provided for readers to better understand the present application. However, even without these technical details and various changes and modifications based on the following implementation modes, the technical solution claimed in each claim of the present application can be realized.
本发明的第一实施方式涉及一种电容检测电路。具体如图3和图4所示。A first embodiment of the present invention relates to a capacitance detection circuit. Specifically shown in Figure 3 and Figure 4.
该电容检测电路包含积分电容Ci、待检测电容Cs、电流源A、运算放大器A0和信息处理芯片;The capacitance detection circuit includes an integrating capacitor Ci, a capacitor to be detected Cs, a current source A, an operational amplifier A0 and an information processing chip;
待检测电容Cs的一端与运算放大器A0的负输入端相连,另一端接地;One end of the capacitor Cs to be detected is connected to the negative input end of the operational amplifier A0, and the other end is grounded;
积分电容Ci的一端与运算放大器A0的负输入端相连,另一端与运算放大器A0的输出端相连;One end of the integrating capacitor Ci is connected to the negative input terminal of the operational amplifier A0, and the other end is connected to the output terminal of the operational amplifier A0;
电流源A的一端与运算放大器A0的负输入端相连,另一端接地;One end of the current source A is connected to the negative input end of the operational amplifier A0, and the other end is grounded;
运算放大器A0的正输入端接地;The positive input terminal of the operational amplifier A0 is grounded;
信号处理芯片的一端与运算放大器A0的输出端相连,另一端输出电容检测电路检测到的电容值。One end of the signal processing chip is connected to the output end of the operational amplifier A0, and the other end outputs the capacitance value detected by the capacitance detection circuit.
具体的说本实施方式中电容的检测过程分两个阶段:Specifically, the detection process of the capacitance in this embodiment is divided into two stages:
第一个阶段,如图3所示,积分电容Ci进行清零复位,而待检测电容Cs被充电至参考电压Vref,这与传统的方法一致;In the first stage, as shown in Figure 3, the integrating capacitor Ci is reset, and the capacitor Cs to be detected is charged to the reference voltage Vref, which is consistent with the traditional method;
第二个阶段,如图4所示,通过开关将待检测电容Cs、积分电容Ci和电流源A的一端分别与运算放大器A0的负输入端相连,将待检测电容Cs和电流源A的另一端接地,将积分电容Ci的另一端与运算放大器A0的输出端相连,并将运算放大器A0的正输入端接地,这样接通电路后,待检测电容Cs上的电荷将一部分通过一个电流源A转移,另一部分电荷则转移至积分电容Ci上,此阶段称为电荷转移阶段或积分阶段。In the second stage, as shown in Figure 4, one end of the capacitor Cs to be detected, the integrating capacitor Ci, and the current source A are respectively connected to the negative input terminal of the operational amplifier A0 through a switch, and the capacitor Cs to be detected and the other end of the current source A are connected to each other. One end is grounded, and the other end of the integrating capacitor Ci is connected to the output terminal of the operational amplifier A0, and the positive input terminal of the operational amplifier A0 is grounded, so that after the circuit is turned on, a part of the charge on the capacitor Cs to be detected will pass through a current source A Transfer, another part of the charge is transferred to the integral capacitor Ci, this stage is called the charge transfer stage or integration stage.
假设运算放大器A0理想,则在第二个阶段结束时,运算放大器A0输入端电压相等,此时,待检测电容Cs两端电位均为零,即待检测电容Cs上的电荷全部转移至积分电容Ci和电流源A上;Assuming that the operational amplifier A0 is ideal, at the end of the second stage, the voltage at the input terminal of the operational amplifier A0 is equal, at this time, the potential at both ends of the capacitor Cs to be detected is zero, that is, the charges on the capacitor Cs to be detected are all transferred to the integration capacitor On Ci and current source A;
上述第二阶段中两部分的电荷转移引起运算放大器A0输出端电压Vout的变化,经运算放大器A0放大后输出,由信息处理芯片中的模数转换器接收一次电荷转移过程中运算放大器A0输出端电压变化的大小ΔVout,经模数转换后传送给信息处理芯片中的数字电路处理器处理,该数字电路处理器再根据电荷转移理论,由表达式Vref*Cs=ΔVout*Ci+I*T方便地得到待测试电容Cs的电容值。The charge transfer of the two parts in the above-mentioned second stage causes the voltage Vout of the output terminal of the operational amplifier A0 to change, which is amplified by the operational amplifier A0 and then output, and is received by the analog-to-digital converter in the information processing chip during the charge transfer process. The magnitude of the voltage change ΔVout, after analog-to-digital conversion, is sent to the digital circuit processor in the information processing chip for processing. The digital circuit processor is then based on the charge transfer theory, which is convenient by the expression Vref*Cs=ΔVout*Ci+I*T Obtain the capacitance value of the capacitor Cs to be tested.
上述第一阶段和第二阶段合起来称为一个电荷转移周期或者称为积分周期,在实际使用中,会根据需要进行反复的电荷转移,即实现积分,值得注意的是,积分电容Ci的清零只有在积分开始的第一个积分周期发生。The above-mentioned first stage and the second stage are collectively called a charge transfer cycle or an integration cycle. In actual use, repeated charge transfers are performed as required, that is, integration is realized. It is worth noting that the clearing of the integration capacitor Ci Zero occurs only at the first integration cycle at the beginning of integration.
由于本实施例中的电容检测电路增加了一个电流源A,该电流源A可以吸取或灌送待检测电容Cs上的部分电荷,待检测电容Cs上的另一部分电荷则转移至积分电容Ci上,这样就可以在不额外增加积分电容Ci面积的前提下减小一次电荷转移过程中运算放大器A0输出端电压变化的大小△Vout,进而增大待检测电容Cs的电容值范围,并且在检测过程中并不降低检测电压,因此也不会引起信噪比的下降。Since a current source A is added to the capacitance detection circuit in this embodiment, the current source A can absorb or feed part of the charge on the capacitor Cs to be detected, and another part of the charge on the capacitor Cs to be detected is transferred to the integrating capacitor Ci , so that the size △Vout of the voltage change at the output terminal of the operational amplifier A0 during a charge transfer process can be reduced without additionally increasing the area of the integrating capacitor Ci, thereby increasing the capacitance value range of the capacitor Cs to be detected, and during the detection process The detection voltage is not reduced, so it will not cause a decrease in the signal-to-noise ratio.
为方便描述,此处假设电流源A的电流为I,电流源开通的时间为T,根据电荷转移理论,得到如下表达式:For the convenience of description, here it is assumed that the current of the current source A is I, and the time when the current source is turned on is T. According to the charge transfer theory, the following expression is obtained:
表达式中ΔVout代表一次电荷转移过程中运算放大器A0输出电压变化的大小。假设待检测电容Cs为100pf,积分电容Ci为20pf,参考电压Vref为3.3V,电流源A电流值I取为150uA,电流源A开启时间T取为2us,则可以得到:In the expression, ΔVout represents the magnitude of the output voltage change of the operational amplifier A0 during a charge transfer process. Assuming that the capacitance Cs to be detected is 100pf, the integrating capacitance Ci is 20pf, the reference voltage Vref is 3.3V, the current value I of the current source A is 150uA, and the turn-on time T of the current source A is 2us, then we can get:
这是一个合理的电压值。另一方面,如果待检测电容Cs较小时,我们可以适当降低电流源A的电流值I或者开通时间T,使△Vout始终保持在运算放大器A0的承受范围之内,进一步准确地检测出大范围的电容值。This is a reasonable voltage value. On the other hand, if the capacitance Cs to be detected is small, we can appropriately reduce the current value I of the current source A or the turn-on time T, so that △Vout is always kept within the tolerance range of the operational amplifier A0, and further accurately detect the large-scale capacitance value.
在实际的电容测量过程中,由于上述公式中的ΔVout、Vref、Ci、I、T均为已知数,因此可以很方便的计算出待检测电容Cs的电容值。In the actual capacitance measurement process, since ΔVout, Vref, Ci, I, and T in the above formula are all known numbers, the capacitance value of the capacitance Cs to be detected can be easily calculated.
本发明第二种实施方式涉及一种电容检测电路,如图5。第二实施方式与第一实施方式大致相同,主要区别之处在于:在第一实施方式中,待检测电容Cs是向积分电容Ci灌送电荷的,称为反向积分模式;而在本发明第二实施方式中,待检测电容Cs是从积分电容Ci吸取电荷的,称为正向积分模式。也就是说,在本实施方式中,积分电容Ci上的部分电荷灌送到待测试电容Cs上,另一部分电荷被电流源A分担。其工作原理与第一实施方式相同,在此不再赘述。The second embodiment of the present invention relates to a capacitance detection circuit, as shown in FIG. 5 . The second embodiment is roughly the same as the first embodiment, the main difference is that: in the first embodiment, the capacitor Cs to be detected is to fill the charge to the integration capacitor Ci, which is called the reverse integration mode; and in the present invention In the second embodiment, the capacitor Cs to be detected absorbs charge from the integrating capacitor Ci, which is called the forward integrating mode. That is to say, in this embodiment, part of the charge on the integrating capacitor Ci is poured into the capacitor Cs to be tested, and the other part of the charge is shared by the current source A. Its working principle is the same as that of the first embodiment, and will not be repeated here.
本领域的普通技术人员可以理解,上述各实施方式是实现本发明的具体实施例,而在实际应用中,可以在形式上和细节上对其作各种改变,而不偏离本发明的精神和范围。Those of ordinary skill in the art can understand that the above-mentioned embodiments are specific examples for realizing the present invention, and in practical applications, various changes can be made to it in form and details without departing from the spirit and spirit of the present invention. scope.
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