JP5767673B2 - Current waveform measuring device - Google Patents

Description

  The present invention relates to a current waveform measuring apparatus for measuring and recording a time waveform of a current flowing through a power line or the like.

  In recent years, from the viewpoint of efficient use of power and energy saving, a power sensor has been installed in the homes of power consumers such as ordinary households and offices, and HEMS performs efficient use of power such as peak cut and remote control of electrical equipment. Development and examination of (Home Energy Management System) and smart grid technology for controlling a power network are in progress.

  In general, a power sensor used for HEMS or the like is installed in a distribution board in a home or individual home appliances, and calculates power consumption by measuring current and voltage. In recent home appliances, switching power supply circuits and inverter control circuits, which are advantageous for low power consumption, are often used, so the current consumption waveform is often a unique waveform that is significantly different from a sine wave. .

  Therefore, in order to accurately measure the power consumption by the method as described above, it is important to measure a waveform including phase information indicating what the current waveform is with respect to the voltage waveform. It is desirable to measure the voltage and current at the same time and obtain a current waveform synchronized with the voltage.

  In general, since the voltage waveform is supplied in a form close to a sine wave, the timing of the zero cross point, which is the point at which the AC voltage becomes 0, is measured instead of measuring the voltage waveform except in special cases. As a result, a current waveform in a form synchronized with the voltage is obtained. When the voltage waveform is approximated to a sine wave, an almost accurate power consumption value is obtained.

  On the other hand, based on the total current waveform of the power supply system obtained from the distribution board in the home, a technology for identifying the types and operating states of multiple home appliances receiving power supply from the power supply system, Recently researched and developed (see Non-Patent Documents 1 and 2). In such a technique, the total current waveform of the power supply system is the sum of the current waveforms consumed by each home appliance, and the power consumption waveform of each home appliance acquired in advance is used as teacher data. Thus, the current waveforms and their feature quantities are compared, and the type, state, etc. of the operating device are identified from the result.

  In these device identification means, it is generally assumed that the current waveform of each device is obtained as a periodic waveform synchronized with the voltage, and when acquiring the current waveform with the distribution board, the voltage waveform or Information on synchronization timing, such as at least voltage zero cross timing, is required.

  As described above, when accurate power measurement or current waveform measurement for equipment identification or the like is performed with a distribution board in the home, it is necessary to acquire a voltage simultaneously with the current. On the other hand, in order to obtain the voltage directly from the distribution board in the home, it is obtained by directly contacting the power line with a probe or the like for measuring the voltage, or a probe or sensor is incorporated in the distribution board in advance. There is a need.

Kazuhiro Takatani, Yasunao Suzuki, Fumihiko Ishiyama, Masaki Kasai, Noboru Iwasaki, Kimihiro Tajima, “Examination of Operational State Estimation of Home Appliances Using Characteristics of Conducted Interference Waves Generated by Home Appliances”, IEICE , May 2012, vol. 112, no. 73, EMCJ2012-14, pp. 29-34 Masaki Kosai, Yasunao Suzuki, Fumihiko Ishiyama, Yoshiharu Akiyama, “Identification of Home Appliances Based on Frequency Characteristics of Normal Mode Current”, Proceedings of the 2011 IEICE General Conference, B-4-25

  However, in order to obtain the voltage directly from the power line of the distribution board, a qualified electrician is required, and for safety, it is also necessary to stop the power supply before installing the probe or sensor. There was a problem. The labor and cost required for installation of probes and sensors is a barrier to the introduction of such sensor systems on existing distribution boards.

  Also, the installation of voltage sensors in addition to current sensors increases the number of sensors that can be placed in a limited distribution board space, and there is a problem that some cases cannot be installed depending on the distribution board. there were.

  The present invention has been made in view of such problems, and the object of the present invention is to simultaneously monitor current and voltage with a non-contact sensor with respect to the wire to be measured, and to measure a current waveform synchronized with the voltage. An object of the present invention is to provide a current waveform measuring apparatus having a small and simple configuration capable of performing the above.

In order to solve the above problems, the invention described in one embodiment is a current waveform measuring apparatus for measuring a current waveform flowing through a load connected between two electric wires to which an AC voltage is applied. A first electrode that is not electrically connected to the first electric wire of the two electric wires, and is disposed so as to surround the first electric wire with a certain distance from the first electric wire; A second electrode that is not electrically connected to the second electric wire of the two electric wires, and is disposed so as to surround the second electric wire with a certain distance from the second electric wire; A voltage measuring unit for measuring a first AC voltage generated between the first electrode and the second electrode by electrostatic induction from the AC voltage; and a magnetic field generated by a current flowing through the first electric wire. A first current measuring transformer for generating an induced current from the fluctuation, and the first current measuring transformer; Yes a first current measuring unit for measuring a first alternating current from variation of the induced current generated in Nsu, not electrically connected to the first wire, a constant distance between the first wire A first shield electrode installed so as to surround the first electric wire and the first current measuring transformer, and means for electrically connecting the first shield electrode and the second electrode; the equipped, positions for said from the measurement values of said first alternating current of the first AC voltage, the first AC voltage time waveform and the first alternating current of the first alternating current It is characterized by measuring a phase difference.

According to another embodiment the invention provides a current waveform measuring apparatus for measuring the waveform of the current flowing through the load connected between the two wires of the AC voltage is applied, the two wires A first electrode that is not electrically connected to the first electric wire and that surrounds the first electric wire with a certain distance from the first electric wire; and a first electrode of the two electric wires A second electrode that is not electrically connected to the second electric wire but has a certain distance from the second electric wire and surrounds the second electric wire, and electrostatic induction from the AC voltage A voltage measuring unit that measures a first AC voltage generated between the first electrode and the second electrode, and a first that generates an induced current from a change in a magnetic field caused by a current flowing through the first electric wire. 1 of the current measuring transformer and the induced current generated by the first current measuring transformer. The first current measuring section, wherein the second current measuring transformer for generating an induced current from changes in the magnetic field caused by the second current through the wire, the second current measuring a first alternating current from the dynamic The second current measuring unit that measures the second alternating current from the fluctuation of the induced current generated in the measurement transformer and the first electric wire are not electrically connected, and a certain distance from the first electric wire is maintained. The first shield electrode, which is installed so as to surround the first electric wire and the first current measuring transformer, and the second electric wire are not electrically connected, and are constant with the second electric wire. And electrically connecting the second shield electrode disposed so as to surround the second electric wire and the second current measuring transformer, and the first shield electrode and the second shield electrode. and means for connecting said first Measurements of the flow voltage, the measured value or these measured values and the second alternating current of a first alternating current, the time waveform of the first alternating current, of the second alternating current time waveforms and their A phase difference with respect to the first AC voltage is measured.

The invention described in still another embodiment is a current waveform measuring device for measuring a waveform of a current flowing through a load connected between two electric wires to which an AC voltage is applied, A first electrode that is not electrically connected to the first electric wire, and that surrounds the first electric wire with a certain distance from the first electric wire; and the two electric wires A second electrode that is not electrically connected to the second electric wire, and is disposed so as to surround the second electric wire with a certain distance from the second electric wire, and the first electric wire. A first current measurement transformer that generates an induced current from a variation in a magnetic field caused by a flowing current, and a first current measurement unit that measures a first alternating current from a variation in the induced current generated in the first current measurement transformer And the fluctuation of the magnetic field caused by the current flowing through the second electric wire. The second current measuring transformer that generates current, the second current measuring unit that measures the second alternating current from the fluctuation of the induced current generated in the second current measuring transformer, and the first electric wire are: A first shield electrode that is not electrically connected and is disposed so as to surround the first electric wire and the first current measuring transformer with a certain distance from the first electric wire; A second shield electrode that is not electrically connected to the electric wire and is disposed so as to surround the second electric wire and the second current measuring transformer with a certain distance from the second electric wire; and means for electrically connecting the first shield electrodes second shield electrodes, the first voltage measurement for measuring a first alternating voltage to said first shield electrode of the first electrode And the second shield electricity of the second electrode A second voltage measuring unit that measures a second alternating voltage with respect to the first electric wire calculated as a difference between the measured value of the first alternating voltage and the measured value of the second alternating voltage From the measured value of the third alternating voltage between the first and second electric wires, the measured value of the first alternating current and the measured value of the second alternating current, the time waveform of the first alternating current, The time waveform of the second alternating current and the phase information for the third alternating voltage are measured.

  The present invention is capable of simultaneously monitoring current and voltage with a non-contact sensor with respect to an electric wire to be measured, can measure a current waveform synchronized with the voltage, and does not require special qualification or power interruption. Can be easily attached to.

It is a figure which shows the basic composition of the current waveform measuring device which concerns on Embodiment 1 of this invention. It is a figure which shows the example of the current waveform measured using the current measurement means. (A) is a figure which shows the current waveform and voltage waveform at the time of single operation of electric equipment A, (b) is a figure which shows the current waveform and voltage waveform at the time of single operation of electric equipment B, (c) It is a figure which shows the synthetic | combination current waveform and voltage waveform when the electric equipments A and B operate | move simultaneously. The figure which shows the basic composition of the current waveform measuring device which concerns on Embodiment 1 of this invention is shown. It is a figure which shows the equivalent circuit of the current waveform measuring device which concerns on Embodiment 1 of this invention. The figure which shows the result of the calculation based on (1) Formula at the time of producing the voltage waveform measuring apparatus 105 in Embodiment 1, measuring the frequency characteristic, and fitting each parameter of C1, C2, Cp, and Rp is there. It is a figure which shows the structure of the current waveform measuring device which concerns on Embodiment 2 of this invention. It is a figure which shows the basic composition of the current waveform measuring device which concerns on Embodiment 3 of this invention. It is a figure which shows the equivalent circuit of the current waveform measuring apparatus in Embodiment 3. It is a figure which shows the basic composition of the current waveform measuring device which concerns on Embodiment 4 of this invention. It is a figure which shows the equivalent circuit of the current waveform measuring apparatus in Embodiment 4. It is a figure which shows the simplified equivalent circuit of the current waveform measuring apparatus in Embodiment 4. It is a figure which shows the basic composition of the current waveform measuring device which concerns on Embodiment 5 of this invention. It is a figure which shows the equivalent circuit of the current waveform measuring device in Embodiment 5. It is a figure which shows the structural example of the current waveform measuring apparatus which heightened the shielding effect of the whole system | strain using the shielded cable in Embodiment 5. It is a figure which shows another structural example of the current waveform measuring apparatus in Embodiment 5. It is a figure which shows the basic composition of the current waveform measuring device which concerns on Embodiment 6 of this invention. It is a figure which shows the equivalent circuit of the current waveform measuring apparatus in Embodiment 6. It is a figure which shows the calculation result of the frequency characteristic of the amplitude of a detection voltage represented by (7) Formula and (8) Formula, and a phase. (A)-(c) is a figure which shows the structure of the clamp type probe provided with the electrode and the electric current measurement trans | transformer. The basic composition of the current waveform measuring device concerning Embodiment 7 of the present invention is shown. 9 shows a configuration example 1 of a current waveform measuring apparatus according to an eighth embodiment of the present invention. 9 shows a configuration example 2 of a current waveform measuring apparatus according to an eighth embodiment of the present invention. It is a figure which shows the structural example of the clamp type probe which shifted the position of the electric current measurement trans | transformer and the electrode for voltage measurement. It is a figure which shows an example of the power supply voltage waveform of the power wire of a household appliance (refrigerator), and the current waveform which flows through the power wire. It is a figure which shows the relationship between the relative value with respect to the true electric power value of the electric power value calculated about the electric current waveform of FIG. 25, and the phase difference of a voltage and an electric current.

  In order to solve the problems described above, in the current waveform measuring apparatus of the present invention, a current measuring transformer for measuring a current flowing through an electric wire by electromagnetic induction from the electric wire to be measured and an electrode surrounding each of the two electric wires to be measured. By using both of the voltage measurement probes for measuring the electrostatic induction voltage generated between them simultaneously, it is possible to measure the current and voltage simultaneously without contacting these wires to be measured. In addition, by configuring these as a single unit, a small and simple sensor can be realized.

  Hereinafter, embodiments of the present invention will be described in detail.

(Embodiment 1)
FIG. 1 shows a basic configuration of a current waveform measuring apparatus according to Embodiment 1 of the present invention. In FIG. 1, the example in the case of installing the current waveform measuring device of this invention in the two electric wires L1 and L2 is shown. This example shows a case in which a time waveform of a current flowing through a power supply circuit (closed circuit) is measured when a load Load such as an electric device is connected to a power supply line such as a commercial AC power supply. .

  In general, as means for measuring the current flowing through such an electric wire, a current measuring transformer using electromagnetic induction and a current measuring means using the Hall effect are known. In these means, a cylindrical or donut-shaped magnetic core is generally installed so as to surround the electric wire to be measured, and the magnetic flux generated in the magnetic core and the amount of change thereof are detected when a current flows. Now measure the current and its waveform. The current measuring transformer uses the fact that an induced electromotive force is generated in a coil wound around a magnetic core. In the drawing of FIG. 1, a current measuring device 104 using the current measuring transformer 103 is shown.

  A voltage to be measured Vo is applied between the two electric wires L1 and L2 in FIG. A cylindrical electrode 101 and an electrode 102 are provided so as to surround these electric wires. The electric wires L1 and L2 pass through the insides of the electrodes 101 and 102, respectively, so that each electric wire coincides with the central axis of each electrode as much as possible, and the electrode and the electric wire do not make electrical contact. To place. That is, the electrode is installed so as to surround the electric wire with a certain distance from the electric wire.

  In general, these wires often have an insulation coating, and in that case they do not make electrical contact with the electrode, but when measuring an uncovered wire, contact between the electrode and the wire should be avoided. In order to prevent this, an insulator or a dielectric may be sandwiched as a spacer. When the dielectric is sandwiched, the values of the capacitances C1 and C2 are larger than when there is no dielectric, and the sensitivity is improved. Moreover, if the shape of these spacers is appropriately designed according to the electric wire, it becomes easy to fix the electric wire on the central axis of the electrode.

  The electrodes 101 and 102 are provided with a voltage measuring device 105 for measuring the voltage between them. As described above, it is desirable from the viewpoint of improving sensitivity that the input impedance of the voltage measuring device 105 be as high as possible. As the voltage measuring device 105, an operational amplifier, a buffer amplifier, a measurement amplifier, or the like having a high input impedance can be used. In the voltage measuring device 105, the read voltage value V may be displayed as it is, or the voltage value or analog / digital converted voltage value may be output and processed or displayed by a device connected to the subsequent stage. .

  It is advantageous to provide the voltage measuring device 105 at a position as close as possible to the electrodes 101 and 102 in terms of preventing intrusion of external noise and improving sensitivity, but a measurement cable is connected to the electrodes 101 and 102 and separated. A voltage measurement device 105 may be provided at a location and measurement may be performed via a measurement cable. In this case, however, the stray capacitance between the electrodes 101 and 102 is increased by the measurement cable, leading to deterioration of sensitivity. In such a case, it is preferable to select a measurement cable having a small stray capacitance as necessary.

  FIG. 1 shows a current measuring transformer 103 and a current measuring device 104 installed outside the electric wire L1 and the electrode 101. With these functions, the value of the current I flowing through the electric wire L1 can be measured. When the electric wires L1 and L2 are power supply lines and a load Load such as an electric device is connected between them, the time waveform of the current flowing through the load can be measured.

  At this time, as described above, when accurately measuring power consumption or when performing identification estimation of connected electrical equipment, it is necessary to obtain a phase difference with respect to the voltage of the current waveform as information. is there. Here, from the output information of the voltage measuring device 105, timing information such as a voltage zero-cross point can be obtained from the voltage waveform. In the frequency range where the phase characteristic shown in FIG. 6 is almost flat (in FIG. 6, the region of 1 kHz or less and 100 kHz or more), the phase difference between the current waveform and the voltage waveform is measured in advance by measuring with a pure resistance as a load, etc. By grasping this, this phase difference can be corrected, and the current waveform can be acquired in synchronization with the voltage.

  As described above, in the current waveform measuring device of the present invention, the current value and the information of the phase difference with respect to the voltage of the current can be measured at the same time, and the current waveform in a form synchronized with the voltage is contactless. It can be measured.

  FIG. 2 shows an example of a current waveform measured using current measuring means. In general, the waveform of the current consumed by an electrical device or the like is a periodic waveform synchronized with the waveform of the supply voltage (approximately a sine wave in the case of a commercial AC power supply) as shown in FIG. As shown in FIG. 2A, if the current waveform can be measured in a form synchronized with the voltage, the power consumption value of the load is accurately calculated by time-integrating the product of the voltage and the current. be able to. On the other hand, as shown in FIG. 2B, when a phase difference occurs between the measured value of the current waveform and the measured value of the voltage due to the phase characteristics of the measuring system, the power consumption calculation result is An error based on this phase difference occurs.

  FIGS. 3A and 3B show current waveforms and voltage waveforms when the electric devices A and B operate independently, and FIG. 3C shows a combined current waveform and voltage when the electric devices A and B operate simultaneously. Waveform is shown. In general, as shown in FIGS. 3A and 3B, the current waveform varies depending on the type and operating state of the electrical device. On the other hand, in the above-described electric device identification technology, the combined current waveform on the distribution board is the sum of these respective waveforms as shown in FIG. Therefore, by comparing and contrasting the current waveform obtained when each electrical device obtained in advance is operating alone and these combined current waveforms, the type and operating state of the electrical device used in the home can be determined. It can also be identified on the board. However, even in such a case, the phase difference of the current waveform with respect to the voltage needs to be kept constant in order to accurately identify and estimate the device.

  As described above, in these applications, when measuring a current waveform such as a power supply line, not only the measurement value related to the current but also information on the phase difference of the current waveform with respect to the voltage is required. Alternatively, at least timing information such as zero cross points appearing at regular intervals in the periodic waveform needs to be acquired.

  FIG. 4 shows a basic configuration of the current waveform measuring apparatus according to the first embodiment of the present invention. In FIG. 4, the input capacitance Cp and the input resistance Rp between the input terminals of the voltage measuring device 105 are shown. Moreover, the electrostatic capacitance between the electric wire L1 and the electrode 101 is shown as C1, and the electrostatic capacitance between the electric wire L2 and the electrode 102 is shown as C2. In FIG. 4, the current flowing through the electric wire L1 is measured by the current measuring transformer 103 and the current measuring device 104, and the voltage between the electric wires L1 and L2 is measured by the voltage measuring device 105. Note that the electric wire L2 may be grounded in the case of a neutral wire of a power supply line or the like.

  FIG. 5 shows an equivalent circuit of the current waveform measuring apparatus according to the first embodiment of the present invention. The line voltage Vo to be measured is applied to a circuit in which C1, the input impedance (Cp and Rp) of the voltage measuring device 105, and C2 are connected in series. The measurement voltage V is obtained as a result of dividing the line voltage Vo by these impedances.

It is expressed. Here, C12 is the combined capacity when C1 and C2 are connected in series.
C12 = C1C2 / (C1 + C2)
Ω represents an angular frequency. (J is an imaginary unit)
From the equation (1), when the input impedance of the voltage measuring device is sufficiently high, that is, when Cp is small and Rp is large, the value of the denominator approaches C12, and the measurement result V becomes almost equal to the line voltage Vo. .

  In the region where the frequency of the voltage to be measured is high (when ω ≧ 1 / (Rp (C12 + Cp))), the equation (1) is

In the high frequency region, the voltage conversion sensitivity becomes a constant value that does not depend on the frequency.

  In FIG. 6, the voltage waveform measuring apparatus 105 in the first embodiment is manufactured, the frequency characteristics thereof are measured, and the calculation results based on the equation (1) when the parameters C1, C2, Cp, and Rp are fitted. Indicates. The amplitude characteristic shown in FIG. 6 is the ratio between the line voltage Vo and the detection voltage V and corresponds to the voltage conversion sensitivity. As shown above, the amplitude characteristic is flat in the high frequency region exceeding 10 kHz. The amplitude frequency characteristic is shown.

  As described above, the voltage V measured by the voltage measuring device 105 is substantially equal to the line voltage Vo when the input impedance of the voltage measuring device 105 is sufficiently high, and the electric wire L1 and the electrode 101, and the electric wire L2 and the electrode. It is possible to measure the line voltage Vo regardless of the values of the capacitances C1 and C2 between 102. Even when the input impedance of the voltage measuring device 105 cannot obtain a sufficiently high value as described above, if the frequency is in a sufficiently high range, the sensitivity of the voltage is almost constant regardless of the frequency. Therefore, it is possible to measure a voltage waveform without distortion.

  Note that, even in a low frequency region (50/60 Hz) such as a general commercial power supply, although the voltage conversion sensitivity is lower than that in the high frequency region, the voltage waveform and phase information are set as the output voltage V corresponding to the equation (1). It can be measured.

  In the measurement system having a high input impedance of the voltage measuring apparatus 105 as described above, it is easy to pick up high-frequency noise generated outside, and the measurement result may be affected in a place with a lot of noise. In the current waveform measuring apparatus 104 of the present invention, concentric cylindrical shield electrodes are provided outside the electrodes 101 and 102, and the connection of the shield electrodes and the design of the capacitances C1 and C2 between the electrodes are specified. By performing under the conditions, it is possible to suppress the influence of noise induced from the outside, and it is possible to measure a voltage waveform with high accuracy.

  Moreover, in voltage measurement in a low frequency region (50/60 Hz) like a general commercial power supply, the phase frequency characteristics are reduced by connecting a capacitor having an appropriate capacitance between electrodes for measuring voltage. The frequency can be flattened, and the voltage waveform and phase information can be accurately measured regardless of the input impedance of the voltage measuring device 105.

  In addition, by integrating the voltage measuring electrode 101 and the current measuring transformer 103 and attaching them to an existing electric wire in a clamp type, a small and easy-to-install measuring device can be realized.

(Embodiment 2)
FIG. 7 shows a configuration of a current waveform measuring apparatus according to Embodiment 2 of the present invention. FIG. 7 shows a configuration example when the current waveform measuring device is applied to a single-phase three-wire power supply system of a general household as an example, and between the electric wires L1 and L2 and the electric wire E that is a neutral wire. A voltage of AC 100V having a reverse phase is applied to each of the two.

  In the present embodiment, the current measuring transformer 203 and the current measuring device 205 are installed outside the electric wire L1 and the electrode 201, and the current measuring transformer 204 and the current measuring device 206 are arranged outside the electric wire L2 and the electrode 202. It is the feature that installed. In such an embodiment, the current I1 flowing through the load Load1 such as an electric device connected between the electric wire L1 and the electric wire E is measured using the current measuring transformer 203 and the current measuring device 205, and the electric wire L2 and the electric wire are measured. The current I2 flowing through the load Load2 connected to E is measured individually using the current measuring transformer 204 and the current measuring device 206. By such measurement, it is possible to individually measure the currents flowing through the loads Load1 and Load2 connected to the two power supply systems (the electric wires L1 to E and the electric wires L2 to E).

  On the other hand, with respect to the power supply voltage, the voltage measuring device 207 measures the voltage between the cylindrical electrode 201 and the electrode 202 installed so as to surround the electric wire L1 and the electric wire L2, respectively. At this time, the voltage between the electric wires L1 and L2 is AC200V, but the phase of the voltages of the two power supply systems (the electric wires L1 to E and the electric wires L2 to E) are reversed. By measuring Vo, phase information of both power supply systems can be obtained simultaneously.

(Embodiment 3)
FIG. 8 shows a basic configuration of a current waveform measuring apparatus according to Embodiment 3 of the present invention. FIG. 9 shows an equivalent circuit of the current waveform measuring apparatus according to the third embodiment.

  In this embodiment, in addition to the embodiment shown in FIG. 4, a cylindrical shield electrode 304 is provided outside the electrode 301 and the current measurement transformer 303 so that the central axis coincides with the electrode 301 and the current measurement transformer 303. The shield electrode 304 is not in electrical contact with the electric wire L1 or the electrode 301, but is in electrical contact with the electrode 302 by the electric wire 305 or the like. In addition, since it is desirable to fix the positional relationship between the electric wire L1 and the electrode 301, it may be physically fixed by providing a spacer or the like in the gap. Note that the capacitance between the electrode 301 and the shield electrode 304 was αC1 using the capacitance C1 and the coefficient α.

  When measuring the voltage of a commercial power supply (single-phase three-wire) for general households, one side (cold side) of AC100V is grounded as a neutral point. In such a case, it is desirable to use the cold side as the electric wire L2. In addition, even when the wire to be measured is a communication line or the like, when the single line is connected to a circuit ground or the like, it is desirable to use the ground side as the electric wire L2. This is because the shield electrode 304 is installed to prevent the influence of external noise, particularly common mode noise, and since it is connected to the electrode 302, the lower the impedance of the electrode 302 with respect to the ground, the noise removal. This is because the effect becomes high.

  Note that one side of the voltage measuring device 307 may be connected to either the shield electrode 304 or the electrode 302.

FIG. 8 shows a conductor N in which a common mode noise voltage V _N is generated as a noise source. Noise source N leads to noise by electrostatic induction, but shows the coupling capacitance between the affects it in Figure conductor N and the shield electrode 304 as C _N.

Noise voltage V _N of the common mode, when the common mode impedance to earth wire L1 and line L2 is high, because the common-mode impedance of the electrode 301 and the shield electrode 304 can be regarded as substantially equal, the noise voltage V _N is the electrode 301 and the shield The influence on the measurement voltage V, which is the voltage between the electrodes 304, is small.

On the other hand, since one of the commercial power lines is grounded as described above (in this case, the electric wire L2), the common mode impedance of the electrode 302 is low, and the shield electrode 304 connected thereto is the same. Since the noise current due to the noise voltage V _N flows from C _N to the ground via C 2, the influence of the noise voltage V _N on the measurement voltage V should be reduced if the capacitance C 2 is sufficiently large compared to C _N. I can do it. If possible, ideal noise shielding is possible if the electrode 302 is grounded or the electrode 302 and the grounded electric wire L2 can be directly connected.

(Embodiment 4)
FIG. 10 shows a basic configuration of a current waveform measuring apparatus according to Embodiment 4 of the present invention. FIG. 11 shows an equivalent circuit of the current waveform measuring apparatus according to the fourth embodiment.

  In FIG. 10, a cylindrical shield electrode 406 is provided outside the cylindrical electrode 402 and the current measuring transformer 404 so that the central axis coincides therewith. The shield electrode 406 is not in electrical contact with the wire L2 or the electrode 402, but is in electrical contact with the shield electrode 405 with the wire 407 or the like. Note that the capacitance between the electrode 401 and the shield electrode 405 is α1C1 using the coefficient α1 and the capacitance C1, and the capacitance between the electrode 402 and the shield electrode 406 is α2C2 using the coefficient α2 and the capacitance C2. .

FIG. 10 shows how the common mode noise voltage V _N of the noise source N affects via the coupling capacitor C _N , as in the third embodiment shown in FIG. In this embodiment, the shield electrode 405 and the shield electrode 406 are electrically connected, and an equivalent circuit thereof is as shown in FIG.

FIG. 12 shows a simplified equivalent circuit in which Rp, Cp, and the voltage source Vo are omitted in order to examine only the influence of the noise voltage _VN on the measurement voltage V in the current waveform measurement apparatus according to the fourth embodiment. FIG 12, the voltage to ground that occurs in the electrode 401 and the electrode 402 by the noise voltage _{V N,} are respectively V1, V2 and. At this time,

Therefore, the measurement voltage V is

It becomes. When α1 = α2, (3) equation V = 0, and the measured voltage V is not affected by the noise voltage _{V N.} From the above, the external noise can be canceled by designing the structure and positional relationship of the electrode and the shield electrode so that α1 = α2.

  In other words, in other words, α1 = α2, the capacitance between the wire L1 and the electrode 401 is C10, the capacitance between the electrode 401 and the shield electrode 405 is C11, and between the wire L2 and the electrode 402. When the electrostatic capacity of C20 and the electrostatic capacity between the electrode 402 and the shield electrode 406 are C21, respectively,

It is the same as having the relationship.

  When the design is made so that the equation (4) holds, voltage measurement that is not easily affected by external noise as described above becomes possible, measurement accuracy with respect to phase information is improved, and current waveform measurement with higher accuracy is possible. It becomes possible.

(Embodiment 5)
FIG. 13 shows a basic configuration of a current waveform measuring apparatus according to Embodiment 5 of the present invention. FIG. 14 shows an equivalent circuit of the current waveform measuring apparatus according to the fifth embodiment.

In FIG. 13, the electrode and the shield electrode are the same as those in the fourth embodiment shown in FIG. 10, but two voltage measurement devices 510 and 511 are provided, and the voltage measurement device 510 uses the voltage between the electrode 501 and the shield electrode 505. The voltage is measured, and the voltage between the electrode 502 and the shield electrode 506 is measured by the voltage measuring device 511. When the measurement results of each voltage are Vp1 and Vp2, the difference V = Vp1−Vp2 (5)
Is the measurement result.

  By dividing the voltage measuring device for each electric wire, it is sufficient to measure the voltage between the adjacent electrode and the shield electrode even when the distance between the two electric wires is long. By routing an impedance measurement cable, the problem of easily picking up external noise is eliminated, and sensitivity can be measured and the measurement is less susceptible to noise.

  If the shield electrodes 505 and 506 can be grounded as shown by a chain line a in FIGS. 13 and 14, an ideal shielding effect can be expected in the entire apparatus.

  FIG. 15 shows a configuration example of a current waveform measuring apparatus in which the shielding effect of the entire system is enhanced using a shielded cable in the fifth embodiment. In this example, the shield electrodes 505 and 506 are brought into electrical contact with an electric wire 507 via a shield cable 513. The measurement results Vp1 and Vp2 measured by the voltage measuring devices 510 and 511 are sent to the difference calculating device 512, and the measured voltage V is calculated from the difference as shown in equation (5).

  FIG. 16 shows another configuration example of the current waveform measuring apparatus according to the fifth embodiment. In FIG. 16, voltage measuring devices 510 and 511 include an amplifier circuit or a buffer circuit that measures a voltage with a high input impedance and outputs the result with a low output impedance. Further, the pressure measuring devices 510 and 511 are directly connected to the electrodes 501 and 502 and the shield electrodes 505 and 506 to measure the voltage.

  In this configuration, the high-impedance portion where external noise is easily picked up can be shortened as much as possible, so that it is less susceptible to noise. Further, since the output impedance is low, even when an inexpensive cable without a shield such as a pair cable is used, it is less affected by noise.

(Embodiment 6)
FIG. 17 shows a basic configuration of a current waveform measuring apparatus according to Embodiment 6 of the present invention. In the sixth embodiment, a capacitor having a capacitance C3 is connected between the electrodes 601 and 602 in contrast to the configuration of the first embodiment. The electrostatic capacity C3 is sufficiently larger than the electrostatic capacity C1 between the electric wire L1 and the electrode 1 and the electrostatic capacity C2 between the electric wire L2 and the electrode 2.

  FIG. 18 shows an equivalent circuit of the current waveform measuring apparatus according to the sixth embodiment. As shown in FIG. 18, the line voltage Vo to be measured is added to a circuit in which C1, a parallel circuit of C3, an input impedance (Cp and Rp) of the voltage measuring device, and C2 are connected in series. The measured voltage V is obtained by dividing Vo by these impedances.

It is expressed. Here, C12 is a combined capacity when C1 and C2 are connected in series. C12 = C1C2 / (C1 + C2)
Ω represents an angular frequency. (J is an imaginary unit)
From the equation (6), in the region where the resistance component Rp of the input impedance of the voltage measuring device is sufficiently large and the frequency of the voltage to be measured is high (ω ≧ 1 / (Rp (C12 + C3 + Cp))), the equation (7) Is

In the high frequency region, the voltage conversion sensitivity becomes a constant value that does not depend on the frequency. On the other hand, the phase θ in equation (6) is

However,

From equation (8), θ = 0 when ω is sufficiently larger than ωo, and θ = 2 / π when ω is sufficiently smaller than ωo. From this, it can be seen that when ω is sufficiently larger than ωo, there is no phase difference between the input voltage and the output voltage.

  FIG. 19 shows the calculation results of the frequency characteristics of the amplitude and phase of the detection voltage expressed by the equations (7) and (8). As shown in FIG. 19, in the absence of C3, the amplitude characteristics are almost flat in a frequency region higher than fo = ωo / 2π = 9.5 kHz, and the phase difference between the actual voltage and the detected voltage is almost 0 °. Become. As described above, when the current waveform measuring apparatus of the present invention is used for measurement in a frequency region higher than fo, it can perform measurement with good sensitivity and good phase characteristics.

  On the other hand, in the frequency range lower than fo, the phase characteristics change up to 90 °, so that it is necessary to correct the phase difference after measuring the phase characteristics. At this time, the phase difference between the actual voltage and the detected voltage is established by connecting C3 having a sufficiently large capacitance and setting fo sufficiently lower than the frequency of the signal to be measured. Can be suppressed to a sufficiently small value. In FIG. 19, when measuring a commercial power supply as an example, the value of C3 is set to 0.01 μF (C1 = C2 = 1 pF), thereby suppressing the phase difference in the frequency range of 50 Hz to 60 Hz to a sufficiently small value. It shows that you can. As a result, the measurement accuracy of the voltage phase information is improved, and as a result, the current waveform can be measured with higher accuracy.

  As can be seen from the equation (7) and FIG. 19, when the value of C3 is increased, the voltage sensitivity decreases accordingly. Therefore, an appropriate value of C3 should be selected in consideration of the phase difference and the voltage sensitivity. Is desirable.

(Embodiment 7)
FIG. 20 shows a basic configuration of a current waveform measuring apparatus according to Embodiment 7 of the present invention. In particular, when measuring a low frequency voltage waveform such as an AC power supply voltage, the voltage sensitivity in the high frequency region is higher than that in the low frequency region as shown in FIG. . Even if the line voltage waveform Vo to be measured has a shape close to a sine wave, noise and distortion may occur in the waveform after measurement. In such a case, the influence of high frequency noise and distortion is suppressed by passing through a low-pass filter having a function of removing a frequency component higher than a desired frequency band, and the original voltage as shown in the graph of FIG. A waveform close to the waveform can be reproduced.

  In the current waveform measuring apparatus described above, the sensor portion including the electrode and the current measuring transformer may be configured as a clamp type. 21A to 21C show the configuration of a clamp-type probe provided with electrodes and a current measuring transformer. The current measuring transformer can efficiently measure current by adopting a configuration in which the wire to be measured is surrounded by the magnetic core 801. In addition, the electrode portion includes electrodes 804 on both sides of the clamp as shown in FIG. 21 (c), and is in electrical contact when the clamp is closed so that accurate voltage detection is possible. Is possible. By integrating the current measuring transformer 802 and the electrode 804 as shown in FIG. 21C, the current measuring transformer 802 and the electrode 804 are compact and can be easily attached in a non-contact manner without any modification to existing wires. A current waveform measuring device that can be realized is realizable.

(Embodiment 8)
22 and 23 show configuration examples of the current waveform measuring apparatus according to the eighth embodiment of the present invention. In these figures, the current measuring transformers 903, 1003, and 1004 and the voltage measuring electrodes 901, 902, 1001, and 1002 are configured to be shifted in position with respect to the longitudinal direction of the wires to be measured L1 and L2.

  In the current waveform measuring apparatus of the present invention, the detected current value depends on the mutual induction coefficient between the current measuring transformers 903, 1003, and 1004 and the wires, and the detected voltage value is the voltage measuring electrodes 901 and 902. , 1001, 1002 and the capacitance between the wires. At this time, since the current measuring transformer and the voltage measuring electrode have an electromagnetic influence on each other, the mutual induction coefficient and the capacitance described above change in a complex manner depending on their positional relationship, and the current and voltage Design values relating to performance such as detection sensitivity and values actually produced in the apparatus do not always coincide with each other with high accuracy.

  At this time, as shown in FIGS. 22 and 23, by shifting the positions of the current measurement transformers 903, 1003, and 1004 and the voltage measurement electrodes 901, 902, 1001, and 1002, the mutual electromagnetic influence is minimized. It is easy to obtain the performance as designed in advance.

  FIG. 24 shows a configuration example of a clamp type probe in which the positions of the current measuring transformer and the voltage measuring electrode are shifted in this way. In FIG. 24, half of the clamp-type sensor is a current measurement portion on which a current measurement transformer 1102 is mounted, and the other half is a voltage measurement portion on which a voltage measurement electrode 1101 is mounted. By adopting such a configuration, it is possible to realize a small current waveform measuring apparatus that can be attached to an existing electric wire and that can easily achieve the designed performance.

  Finally, with reference to FIGS. 25 and 26, the effect of improving the power measurement accuracy by simultaneously measuring current and voltage when measuring AC power consumption with the current waveform measuring apparatus of the present invention will be described.

  FIG. 25 shows an example of a power supply voltage waveform of a power supply line of a home appliance (refrigerator) and a current waveform flowing through the power supply line. A current waveform indicated by a thick solid line in FIG. 25 indicates an actual measurement value obtained by measuring a current with a measurement system having no phase difference between the voltage and the current. The voltage waveform at this time is indicated by a thin dotted line in FIG. FIG. 25 shows a waveform obtained by delaying the phase difference between the voltage and current by 1/10 period and a waveform obtained by advancing by 1/10 period (both calculated values) based on the measured value of the current waveform. ing.

  The power consumed by the home appliance shown in FIG. 25 can be obtained as a value obtained by integrating the product of current and voltage over one period. When a phase difference occurs in the voltage and current measurement results during actual measurement, a waveform shifted on the time axis as shown in the figure is measured. If the power calculation is originally performed, an error occurs in the power calculation result.

  FIG. 26 shows the relationship between the relative value of the power value calculated for the current waveform of FIG. 25 with respect to the true power value, and the phase difference between the voltage and current. Here, the power value when there is no phase difference is set as the true power value, and the relative value is displayed as 100%. As described above, the calculated power value greatly fluctuates due to the phase difference between the voltage and the current, and an error of nearly 50% occurs when the phase difference is 45 degrees.

  For this reason, it is important to make the phase difference between the measured values of the current and voltage as small as possible in order to increase the measurement accuracy of the power value and active power, reactive power, and power factor. In the current waveform measuring apparatus of the present invention, by measuring the voltage in addition to the current waveform, it is possible to measure the current waveform synchronized with the voltage cycle, and it is possible to measure the power accurately.

  As described above, by using the current waveform measuring device of the present invention, the current waveform flowing through the power supply line, the communication line, etc. can be measured including the phase relationship with the voltage. At this time, for voltage measurement, it has been necessary to directly contact these electric wires in the past, and there is a problem of risk of electric shock or affecting communication function. Since the voltage measurement can be performed in a non-contact manner, these problems do not occur, and a safe measurement can be performed with little influence on the existing system to be measured.

  In addition, the current waveform measuring apparatus of the present invention can obtain an effect of shielding or canceling external noise, is not easily affected by external noise, and enables highly accurate voltage measurement.

  In particular, even in a low frequency (50/60 Hz) region such as a commercial power supply, measurement with a small phase difference between voltage and current can be performed, and this is used for accurate power consumption measurement and device power estimation technology. The current waveform synchronized with the voltage can be measured.

L1, L2 Electric wires 101, 102, 201, 202, 301, 302, 401, 402, 501, 502, 601, 602, 701, 702, 804, 901, 902, 1001, 1002, 1101 Electrode 103, 203, 204, 303, 403, 404, 503, 504, 603, 703, 704, 802, 903, 1003, 1004, 1102 Current measuring transformer 104, 205, 206, 306, 408, 409, 508, 509, 604, 708709, 803, 904, 1005, 1006, 1104 Current measuring device 105, 207, 307, 410, 510, 511, 605, 710, 805, 905, 1005, 1006, 1105 Voltage measuring device 305, 407, 507, 707 Electric wire 800 Clamp type probe 801 1103 magnetic core Load load

Claims (6)

A current waveform measuring device for measuring a current waveform flowing through a load connected between two electric wires to which an AC voltage is applied,
A first electrode that is not electrically connected to the first electric wire of the two electric wires and is disposed so as to surround the first electric wire with a certain distance from the first electric wire;
A second electrode that is not electrically connected to the second electric wire of the two electric wires, and is disposed so as to surround the second electric wire with a certain distance from the second electric wire;
A voltage measuring unit that measures a first AC voltage generated between the first electrode and the second electrode by electrostatic induction from the AC voltage;
A first current measuring transformer for generating an induced current from a change in magnetic field caused by a current flowing through the first electric wire;
A first current measuring unit that measures a first alternating current from a variation in an induced current generated in the first current measuring transformer;
A first shield which is not electrically connected to the first electric wire and is disposed so as to surround the first electric wire and the first current measuring transformer with a certain distance from the first electric wire. Electrodes,
Means for electrically connecting the first shield electrode and the second electrode;
With
Measuring a phase difference with respect to the from the measurement values of said first alternating current of the first AC voltage, the first AC voltage time waveform and the first alternating current of the first alternating current A current waveform measuring device. A current waveform measuring device for measuring a current waveform flowing through a load connected between two electric wires to which an AC voltage is applied,
A first electrode that is not electrically connected to the first electric wire of the two electric wires and is disposed so as to surround the first electric wire with a certain distance from the first electric wire;
A second electrode that is not electrically connected to the second electric wire of the two electric wires, and is disposed so as to surround the second electric wire with a certain distance from the second electric wire;
A voltage measuring unit that measures a first AC voltage generated between the first electrode and the second electrode by electrostatic induction from the AC voltage;
A first current measuring transformer for generating an induced current from a change in magnetic field caused by a current flowing through the first electric wire;
A first current measuring unit that measures a first alternating current from a variation in an induced current generated in the first current measuring transformer;
A second current measuring transformer for generating an induced current from a fluctuation of a magnetic field generated by a current flowing through the second electric wire;
A second current measuring unit for measuring a second alternating current from a variation in induced current generated in the second current measuring transformer;
A first shield which is not electrically connected to the first electric wire and is disposed so as to surround the first electric wire and the first current measuring transformer with a certain distance from the first electric wire. Electrodes,
A second shield that is not electrically connected to the second electric wire and is disposed so as to surround the second electric wire and the second current measuring transformer with a certain distance from the second electric wire. Electrodes,
Means for electrically connecting the first shield electrode and the second shield electrode;
With
Measured value of the first AC voltage, the measured value or these measured values and the second alternating current of the first alternating current, the time waveform of the first alternating current, the time of the second alternating current waveform and a current waveform measuring apparatus according to claim 1, characterized in that the phase difference is measured for those of said first AC voltage. A capacitance C10 between the first electric wire and the first electrode;
A capacitance C11 between the first electrode and the first shield electrode;
A capacitance C20 between the second electric wire and the second electrode;
A capacitance C21 between the second electrode and the second shield electrode;
The first electrode and the first shield electrode are arranged with respect to the first electric wire so that the relationship between the first electric wire and C10 / C11 = C20 / C21, and the second electric wire The current waveform measuring apparatus according to claim 2, wherein the second electrode and the second shield electrode are arranged. A current waveform measuring device for measuring a waveform of a current flowing through a load connected between two electric wires to which an AC voltage is applied,
A first electrode that is not electrically connected to the first electric wire of the two electric wires and is disposed so as to surround the first electric wire with a certain distance from the first electric wire;
A second electrode that is not electrically connected to the second electric wire of the two electric wires, and is disposed so as to surround the second electric wire with a certain distance from the second electric wire;
A first current measuring transformer for generating an induced current from a change in magnetic field caused by a current flowing through the first electric wire;
A first current measuring unit that measures a first alternating current from a variation in an induced current generated in the first current measuring transformer;
A second current measuring transformer for generating an induced current from a fluctuation of a magnetic field generated by a current flowing through the second electric wire;
A second current measuring unit for measuring a second alternating current from a variation in induced current generated in the second current measuring transformer;
A first shield which is not electrically connected to the first electric wire and is disposed so as to surround the first electric wire and the first current measuring transformer with a certain distance from the first electric wire. Electrodes,
A second shield that is not electrically connected to the second electric wire and is disposed so as to surround the second electric wire and the second current measuring transformer with a certain distance from the second electric wire. Electrodes,
And means for electrically connecting the said first shield electrodes second shield electrodes,
A first voltage measuring unit for measuring a first AC voltage of the first electrode with respect to the first shield electrode;
A second voltage measuring unit that measures a second AC voltage of the second electrode with respect to the second shield electrode;
With
A measurement value of a third AC voltage between the first electric wire and the second electric wire calculated as a difference between the measurement value of the first AC voltage and the measurement value of the second AC voltage; From the measured value of the first alternating current and the measured value of the second alternating current, the time waveform of the first alternating current, the time waveform of the second alternating current, and the phase with respect to the third alternating voltage A current waveform measuring apparatus for measuring information. Capacitance C10 between the first wire and the first electrode and the second wire and the second electrode connected between the first electrode and the second electrode. 5. The current waveform measuring apparatus according to claim 1, further comprising a capacitor having a capacitance larger than any of the capacitances C <b> 20 between the first and second capacitors.   The first electrode and the first current measuring transformer are disposed so as to be shifted in a longitudinal direction of the first electric wire so as not to overlap with the first electric wire. Item 6. The current waveform measuring device according to any one of Items 1 to 5.

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