CAPACITANCE MEASURING CIRCUIT

Abstract: In a capacitance measuring circuit comprising an oscillator circuit, the capacitance (CT) to be measured forms a link of a series connected frequency-determining impedance set (RT, CT). This is connected to the oscillator circuit only at its end terminals, one end terminal (G) being connected to a constant voltage, while the other end terminal (H) is connected to a point (2) of the oscillator circuit, where this maintains a constant voltage in each half-cycle. The oscillator circuit senses the charging current flowing to the capacitance (CT) and is triggered at the moment when the charging current has dropped to a predetermined value. Hereby influence of the stray and input impedances (C0) on the oscillator frequency, which is representative of the subject capacitance, is avoided.

Description: • CAPACITANCE MEASURING CI RCU IT. The invention relates to a capacitance measuring circuit comprising an oscillator circuit, where the capacitance to be measured forms a link of a series connected frequency-determining set of impe- dances, which is connected to the oscillator circuit only at the end terminals of the series connection , in the following referred to as the first end terminal and the second end terminal . From DE-PS 27 12 369 C2 and from the periodical " Industri- el Teknik" 3-1974, page 27, capacitance measuring oscillator circuits of the kind referred to are known in which a constant current is applied to the series connected set of impedances. In these circuits the voltage across the series connection varies continuously during each half-cycle, and the charge on the stray and input capacitances of the voltage detector will therefore vary during the whole of the half-cycle. This charge is to be delivered by a constant current generator belonging to the circuit, and the charging of the subject capacitance, and thereby the oscillator frequency, will therefore depend on changes of the size of the stray and input capacitances. It is the object of the invention to devise an oscillator cir- cuit of the kind referred to in such a manner as to be capable of measuring capacitances without undesired influence of stray and input capacitances, whereby a high stability and linearity of the measurement can be obtained . This is achieved, according to the invention, by so arrang- ing the circuit that the first end terminal is connected to a constant voltage, while the second end terminal is connected to a point of the oscillator circuit where that circuit maintains a constant voltage during each half-cycle, while at the same time sensing the charging current flowing into the capacitance so as to be triggered at the moment when the charging current thus sensed has dropped to a predetermined va¬ lue. It will be seen that when the voltage across the series con¬ nection is maintained constant in each half-cycle, the charge on the * stray and input capacitances is likewise constant in each half-cycle, and since the recharging of the stray and input capacitances to the constant voltage takes place at the start of each half-cycle, the size of this constant charge and thereby the size of the stray and input capacitances has no influence on the subsequent charging of the subject capacitance and consequently no influence on the frequen- cy of the oscillator circuit, which is representative of the value of the subject capacitance. Thus, it is a distinguishing feature of the measuring circuit according to the invention that a constant voltage is applied to the frequency-determining series connected impedances, and the frequency is determined by measurement of the charging current of the capacitance, as contrasted to the known capacitance measuring circuits in which a constant current is applied to the frequency-determining series connected impedances, and the frequency is determined by measurement of the voltage * From GB 2.006.442 A a capacitance measuring circuit is known in which the influence of the stray capacitances has been reduced by including the subject capacitance in an integrator connected to a Schmitt- trigger. Here the series connection of the frequency-determining im¬ pedances is not connected to the measuring circuit at its end terminals only, but both terminals of the subject capacitance are connected di¬ rectly to the output and the inverting input of the amplifier. Hereby the stray capacitances to ground are in fact elϊminat- ed, but the coupling capacitance between the input and the output of the amplifier, which is frequently substantial , is in this case connect¬ ed directly in parallel to the subject capacitance. Since this coupling capacitance depends on many parameters, such as temperature, amplification, voltage supply etc. , it will have an appreciable influence on the accuracy of measurement. Besides, this capacitance measuring circuit cannot function with the most widespread group of capacitive transducers, viz. those having one terminal grounded . The invention will now be described in further detail with reference to the drawing, in which Fig . 1 shows a particularly advantageous embodiment of the invention , in which the current-sensing, con- stant-voltage-maintaϊning circuit consists of an inverting operational amplifier in conjunction with a comparator, Fig . 2 a graph of the output voltage U κ of the compara¬ tor of Fig. 1 , Fig. 3 a graph of the output voltage U . of the operatio¬ nal amplifier of Fig . 1 , Fig . 4 shows a capacitance measuring circuit according to the invention, illustrating a method of establish- ing the reference voltage for the comparator. Fig . 5 shows a capacitance measuring circuit according to the invention in which an inverting amplifier is inserted between the current-sensing operational amplifier and the comparator, Fig . 6 a graph of the output voltages U . 1 of the invert¬ ing amplifier of Fig . 5, fig . 7 a graph of the output voltage U . of the compara¬ tor of Fig . 5, Fig . 8 a capacitance measuring circuit according to the invention in which the charging current for the series connected frequency-determining impedances is superposed on a constant current. Fig. 9 a capacitance measuring circuit according to the invention with alternative switching of a plurality of series connected frequency-determining sets of impedances to the same current-sensing operational amplifier, and Fig . 10 a capacitance measuring circuit according to the invention with alternative switching of a plurality of current-sensing operational amplifiers to the same comparator and buffer. I n the capacitance measuring circuit of Fig . 1 one end terminal G of the series connected frequency-determining impedances R_C T is connected to a fixed voltage, while their other end terminal H is connected to the inverting input 2 of an operational amplifier A, said input being also connected to the output 6 of the operational amplifier through a resistor R s . The non-inverting input of a compara¬ tor K is connected to the output 6 of the operational amplifier, and the inverting input of the comparator is connected to a reference voltage which has the constant positive value U R EF + and the constant negative value U R E p - in the positive and the negative half-cycle re¬ spectively. The output 7 of the comparator, which can only assume either the positive maximum voltage U κ + or the negative maximum voltage OMPI WIPO U„-, cf. the graph of Fig . 2, is connected to the non-inverting input 3 of the operational amplifier. CO symbolizes the sum of the stray and input capacitances of the Inverting input 2 of the operational amplifier. Assuming the operational amplifier to be Ideal , meaning in the present context that no current flows into the Inputs 2 and 3, and that the feed-back through s causes the input 2 to assume exactly the same voltage as that applied to the input 3, the function of this capacitance measuring circuit is as follows: At the time T1 , U κ is assumed to have its positive maximum value U κ +, which is also applied to the Input 3 of the operational am¬ plifier A. The output 6 consequently assumes a positive voltage which through the resistor R g will raise the voltage on the input 2, and thereby the voltage across the series connection of R_C T , to the constant voltage U κ +. This positive voltage change across the series connection will cause a current J R C to flow into R_C T . Since no current flows into the input 2, the said current must be delivered via R_, and the output voltage U . of the compara¬ tor must therefore assume the value U . = U + R ς J R C - The current J R C drops exponentially, and thereby U . drops, and when suitably selecting the constant value U R FF +, which can advantageously be made proportional to U κ +, U . will pass U R FF +, and the output of the comparator will shift to Its negative maximum value U κ ~, which is now applied to the input 3 of the operational amplifier, cf. the graph of Fig . 3. As a consequence, the output 6 will assume a negative vol¬ tage which through the resistor R_ will lower the voltage on input 2 and thereby on the series connection R T C T to the constant voltage u κ -. This negative voltage change on the series connection R- r -C- will cause a current J RC to flow out of R- r -C- / and , like before, this current must be delivered via R g , and the output voltage U . will therefore assume the value U . = u κ " " R ςJ RC - Like before, the current drops exponentially, whereby U . drops, and when suitably selecting the reference voltage, which now has the constant negative value U R F F -, U . - will pass U R F F -, and the OMPI output of the comparator will be shifted to its positive maximum value 11,,+, which is again applied to the input 3. In this manner the oscil- lations continue at a frequency F determined by the time constant R T C T in conjunction with the resistor R s , the charging voltages U κ + and U κ - and the reference voltages U R _ F + and U R F [ _-, which with modern components can all be made very stable. Owing to the fact that the operational amplifier, through the resistor R s , has almost instantly upon the change-over imposed upon its inverting input 2 the same voltage U as that applied to the input 3 from the comparator, the stray capacitance CO has of course just as promptly been charged to the same constant voltage. This charging has been effected by the superposition of a current J cQ of very short duration on the current J RC - This current does not in any way affect the charging cur- rent J RC , which is only determined by C τ and the constant voltage U κ and R τ , and seeing that, even in the case of great values of CO, the current J_ 0 has dropped to 0 long before the charging current J RC reaches its shifting value, it will be seen that the charging of CO, and thereby the size of CO, has no influence on the frequency of this measuring circuit according to the invention . The oscillator circuit of Fig . 4 comprises a buffer amplifier B with the voltage supplies U β + and U β -. The buffer amplifier has the job of driving the terminal 3 of the operational amplifier A and possibly also of driving the associated frequency measuring equipment. The comparator voltage U κ has now been replaced by the buffer voltage U β and is, like before, connected to the input 3 of the operational amplifier A, and is also used as reference for the compara¬ tor K . Since the output voltage of the operational amplifier is U . = U B +R S J RC '* wi " be seen hat if U A ' s d ' rect 'y applied to the non-in¬ verting input of the comparator, the inputs of the comparator will assume the same voltage only when J R _ = 0, i . e. the comparator will not change over. Therefore, a suitable voltage division of U . is established by means of the resistors R- , R~ and R ., whereby the voltage on the input of the comparator will pass the reference U_ when J R C has dropped to a suitable value. O PI ε The resistor R 3 has been provided in order to establish a positive feed-back in the comparator, in a manner known per se, so as to make the comparator change over quickly even if the voltage change on the non-inverting input is relatively slow. The voltage supply U + and U - to the operational ampli¬ fier is so connected as to be bootstrapped with the input 3, when this is changed over between U β + and U β - . By this arrangement the advantage is obtained that the vol¬ tage on the output of the operational amplifier changes over more quickly since also the output follows U +, U - and the Input 3 when the buffer changes over between U R + and U R -, and the operational amplifier therefore only has to contribute the voltage shift R S J R C . Besides, the advantage Is obtained that common mode errors in the operational amplifier are avoided . In the capacitance measuring circuit of Fig . 5, an inverting ι amplifier A is inserted between the operational amplifier A and the Schmitt-trigger S, where the amplification is determined by the propor¬ tion of R . to R e . Since the voltage supply U +, U - for both A and A is bootstrapped with the output voltage of the Schmitt-trigger and thereby with the voltage on the input 3 of A, the graph of the output voltages U . and U . I will be as shown in Figs. 6 and 7. It will be seen that the graph of U . 1 passes the value 0 at dropping current J R C / anc ! f° r tn ' s reason the comparator can be replaced by the Schmitt-trigger S which acts as a comparator with hysteresis and the reference voltage 0. By this measuring circuit according to the invention the further advantage is obtained that the voltage supplied to the Schmitt-trigger/comparator is amplified . Another method of avoiding subdivision of the voltage U . and still making the input voltage of the comparator pass the reference voltage during the discharging of C τ is shown in Fig . 8, where the resistor R- provides a constant positive and a constant negative cur¬ rent into the frequency-determining series connected Impedances in the positive and the negative half-cycle, respectively. When this current exceeds J R / the output voltage U . will shift in relation to the voltage on the input 3 of the operational ampli¬ fier and thereby in relation to the reference voltage of the comparator. r „ ? which is determined by voltage division between Ry and Rg. Fig . 8 also shows two diodes D connected in anti -parallel and serving to obtain the fastest possible charging of the stray and input capacitances on input 2 of the amplifier A . This is of importance when these capacitances assume very high values so that a charging through R s alone will be too slow. These diodes can of course also be used in the other capacitance measuring circuits according to the in¬ vention shown in the drawing . In the use of the capacitance measuring circuit according to the invention it is possible, as illustrated in Fig . 9, in a simple man¬ ner to connect a plurality of sets of series connected frequency-deter¬ mined impedances R T - , C T1 - R TN CTN successively to the same cur¬ rent-sensing operational amplifier, seeing that, as explained above, the stray capacitances from supply conductors and switches have no influence on the frequencies F- -F... Hereby a succession of frequencies is obtained , which by suitable calculation , e.g . in a computer connected to the circuit, can be used for determining a function of the various capacitances C-.-. -C- j - * . and to eliminate drifting and ageing of the components common to a plurality of measurements, such as the amplifier A, the comparator K and the resistors R- , R~, R 3 and R .. At high temperatures leakage currents from the switches in Fig. 9 may, however, affect the charging of the subject capacitances, and it may then be advantageous to connect two or more current- sensing operational amplifiers A 1 ~A N through a switch 0 to a common comparator K and buffer B, as shown in Fig . 10. In the capacitance measuring circuit according to the invention, the series connected frequency-determining impedances may in principle be RC , LC or RCL combinations or mechanical resonators . However, a great advantage is obtained by using a RC-oscil- lator, because the frequency of this is proportional to the electrode spacing of a capacitive transducer. This is, however, only the case when the influence from the stray and input capacitances can be eli¬ minated, such as has been achieved by the present invention . An advantage can also be obtained by connecting series connected reference impedance sets, having a fixed , known value, to a capacitance measuring circuit according to the invention in succession with the subject impedance sets . These reference impedance sets may deliver signals which can be utilized for the complete correction for drifting in the components common to a plurality of measurements, and for producing fault Indication signals, if as a consequence of faults the signal frequencies from one or more subject impedance sets go beyond certain tolerances relatively to the reference frequencies . The use of reference impedance sets also makes it possible to perform an accurate absolute measurement of capacitances . In the practical use of the measuring circuit according to the invention it may be particularly advantageous to arrange the resi¬ stor R τ with one supply terminal directly on the capacitor electrode of a capacitive transducer, whereby stray capacitances in the point of junction of the series connection are totally avoided . The other end of R-_ may, owing to the advantageous pro¬ perties of the capacitance measuring circuit, be connected to this circuit through a relatively long conductor, such as is In practice frequently desirable. As will be seen, the measuring circuit according to the In¬ vention can in a simple manner provide a stable and linear measuring result which is accurately representative of the subject capacitance. OMPI

Claims: P A T E N T C L A I S: 1. Capacitance measuring circuit comprising an oscillator circuit, where the capacitance (C-.) to be measured forms a link of a series connected frequency-determining set of impedances (R T ,C- f -), which is connected to the oscillator circuit only at the end terminals of the series connection, in the following referred to as the first end terminal and the second end terminal, c h a r a c t e r i z e d in that the first end terminal (G) is connected to a constant voltage, while the second end terminal (H) is connected to a point (2) of the oscillator circuit where that circuit maintains a constant voltage during each half-cycle while at the same time sensing the charging current flowing into the capacitance so as to be triggered at the moment when the charging current thus sensed has dropped to a predetermined value. 2. Capacitance measuring circuit according to claim I, c h a r a c t e r i z e d in that the second end terminal (H) is connected to the inverting input (2) of a current-sensing operational amplifier (A) having an impedance (R s ) connected between its output (6) and its inverting input (2), and the output (6) is connected to a regenerative circuit in such a manner that upon dropping of the charging current to the capacitance (C τ ), as sensed by the operational amplifier (A), to a predetermined value the output voltage triggers the regenerative circuit, which has an output (7) coupled back to the non-inverting input (3) of the current-sensing operational amplifier (A). 3. Capacitance measuring circuit according to claim 2, c h a r a c t e r i z e d in that the regenerative circuit comprises a comparator (K), the non-inverting input of which is coupled to the output (6) of the current-sensing operational amplifier while its inverting input is coupled to a source of positive and negative referen¬ ce potential (U REF +/U REp -). 4. Capacitance measuring circuit according to claim 3, c h a r a c t e r i z e d in that the output of the comparator (K) is connected to the input of a buffer amplifier (B), the output of which constitutes the output (7) of the regenerative circuit and also serves as source of reference potential for the comparator (K). 5. Capacitance measuring circuit according to claim 3, c h a r a c t e r i z e d in that an inverting amplifier (A ) is inserted between the current-sensing operational amplifier (A) and a f O PI Schmitt-trigger (S) which constitutes the comparator. 6. Capacitance measuring circuit according to any of the be- foregoing claims, c h a r a c t e r i z e d In that a plurality of se¬ ries connected frequency-determining sets of impedances (R T1 ,C T1 ~ R TN ,C Tf .) are alternatively connectable to the same oscillator circuit by means of switches (0). 7. Capacitance measuring circuit according to any of claims 2-5, c h a r a c t e r i z e d in that the outputs of a plurality of current-sensing operational amplifiers (A- -A..) with frequency-deter¬ mining sets of impedances (R- .,C T1 - R_ N ,C TN ) connected thereto are alternatively connectable to the same regenerative circuit by means of switches (0). 8. Capacitance measuring circuit according to any of the be- foregoing claims, c h a r a c t e r i z e d in that the first end ter- minai (G) is connected to ground potential. 9. Capacitance measuring circuit according to claim 8, c h a - r a c t e r i z e d in that the capacitance (C-) to be measured is ar¬ ranged at the end of the set of Impedances (R T ,C T ) connected to ground potential. OMPI ^&S ATiθ

Inventors: EILERSEN NILS AOGE JUUL, EILERSEN, NILS, AOGE, JUUL
Applicants: EILERSEN NILS AOGE JUUL, EILERSEN, NILS, AOGE, JUUL
Application year: 1984
Main classification: G01R27
IPC codes: G01R27