WO2005101626A1 - ノイズ抑制回路 - Google Patents
ノイズ抑制回路 Download PDFInfo
- Publication number
- WO2005101626A1 WO2005101626A1 PCT/JP2005/001364 JP2005001364W WO2005101626A1 WO 2005101626 A1 WO2005101626 A1 WO 2005101626A1 JP 2005001364 W JP2005001364 W JP 2005001364W WO 2005101626 A1 WO2005101626 A1 WO 2005101626A1
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- Prior art keywords
- inductor
- inductance
- inductors
- noise
- noise suppression
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Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H7/00—Multiple-port networks comprising only passive electrical elements as network components
- H03H7/01—Frequency selective two-port networks
- H03H7/09—Filters comprising mutual inductance
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02H—EMERGENCY PROTECTIVE CIRCUIT ARRANGEMENTS
- H02H9/00—Emergency protective circuit arrangements for limiting excess current or voltage without disconnection
- H02H9/005—Emergency protective circuit arrangements for limiting excess current or voltage without disconnection avoiding undesired transient conditions
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02M—APPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER; CONTROL OR REGULATION THEREOF
- H02M1/00—Details of apparatus for conversion
- H02M1/12—Arrangements for reducing harmonics from ac input or output
- H02M1/126—Arrangements for reducing harmonics from ac input or output using passive filters
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H7/00—Multiple-port networks comprising only passive electrical elements as network components
- H03H7/01—Frequency selective two-port networks
- H03H7/17—Structural details of sub-circuits of frequency selective networks
- H03H7/1741—Comprising typical LC combinations, irrespective of presence and location of additional resistors
- H03H7/1758—Series LC in shunt or branch path
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B2203/00—Indexing scheme relating to line transmission systems
- H04B2203/54—Aspects of powerline communications not already covered by H04B3/54 and its subgroups
- H04B2203/5462—Systems for power line communications
- H04B2203/5491—Systems for power line communications using filtering and bypassing
Definitions
- the present invention relates to a noise suppression circuit for suppressing noise propagating on a conductive line.
- Power electronics devices such as switching power supplies, inverters, and lighting circuits for lighting devices have power conversion circuits that convert power.
- the power conversion circuit has a switching circuit that converts a direct current into a rectangular wave alternating current. Therefore, the power conversion circuit generates a ripple voltage having a frequency equal to the switching frequency of the switching circuit and noise accompanying the switching operation of the switching circuit. This ripple voltage and noise adversely affect other devices. Therefore, it is necessary to provide a means for reducing ripple voltage and noise between the power conversion circuit and other devices or lines.
- LC filters include T-type filters and ⁇ -type filters in addition to those having one inductance element and one capacitor.
- a common noise filter for electromagnetic interference ( ⁇ ) is also a kind of LC filter.
- a typical ⁇ filter is configured by combining discrete elements such as a common mode choke coil, a normal mode choke coil, an X capacitor, and a ⁇ capacitor.
- power line communication has been regarded as promising as a communication technology used when constructing a communication network in a home, and its development is being promoted.
- Power line communication is performed by superimposing a high-frequency signal on a power line.
- noise is generated on the power line due to the operation of various electric and electronic devices connected to the power line, and this causes a decrease in communication quality such as an increase in an error rate. Therefore, means for reducing noise on power lines is required.
- power line communication it is necessary to prevent communication signals on indoor power lines from leaking to outdoor power lines.
- a C filter is used!
- noise propagating through two conductive lines includes a normal mode (differential mode) noise that causes a potential difference between the two conductive lines, and a noise transmitted through the two conductive lines in the same phase.
- Common mode noise common mode noise.
- Japanese Patent Application Laid-Open No. 9-102723 describes a line filter using a transformer.
- This line filter includes a transformer and a filter circuit.
- the secondary winding of the transformer is inserted into one of the two conductive wires that carry the power supplied to the load from the AC power supply.
- Two input terminals of the filter circuit are connected to both ends of the AC power supply, and two output terminals of the filter circuit are connected to both ends of the primary winding of the transformer.
- a power supply voltage power noise component is extracted by a filter circuit, and this noise component is supplied to a primary winding of a transformer. From the noise component.
- This line filter reduces normal mode noise.
- Japanese Patent Application Laid-Open No. 5-121988 (FIG. 1) describes a low-pass filter composed of three impedance elements.
- This low-pass filter has two high-impedance elements inserted in series into one of the two conductive lines, one end connected between the two high-impedance elements, and the other end connected between the two conductive lines. And a low-impedance element connected to the other end.
- Each of the two high impedance elements is configured by a parallel connection circuit of a coil and a resistor, and the low impedance element is configured by a capacitor.
- This low-pass filter reduces normal mode noise.
- Japanese Patent No. 2784783 (FIG. 6) describes a normal mode noise filter circuit for reducing normal mode noise and a common mode noise filter circuit for reducing common mode noise.
- the normal mode noise filter circuit is composed of two coils inserted into each of the two conductive wires, and a capacitor connecting midway between the windings of each coil.
- the common mode noise filter circuit is composed of two coils inserted into each of the two conductive wires, and two capacitors provided between the winding of each coil and the ground. .
- a filter inserted into a conductive wire for power transport is required to obtain desired characteristics while a current for power transport is flowing, and to take measures against temperature rise. Therefore, a ferrite core with a gap is usually used as a magnetic core in an inductance element in a filter for a power conversion circuit.
- an inductance element has a problem in that its characteristics approach those of an air-core inductance element, and the inductance element becomes large in size to achieve desired characteristics.
- the low-pass filter described in Japanese Patent Application Laid-Open No. 5-121988 (FIG. 1) and the filter circuit described in Japanese Patent No. 2784783 (FIG. 6) use the conventional noise reduction principle. Because it is the same as the LC filter, it has the same problems as the conventional LC filter! /
- the present invention has been made in view of the difficult problems, and an object of the present invention is to provide a noise suppression circuit that can suppress noise over a wide frequency range and that can be downsized.
- a noise suppressing circuit is a circuit that suppresses normal mode noise transmitted by first and second conductive lines and causing a potential difference between these conductive lines.
- the first and second inductors inserted in series with the first conductive line and magnetically coupled to each other, a third inductor and a first capacitor connected in series, Is connected between the first inductor and the second inductor, and the other end is connected to the second conductive line. Then, provided that the coupling coefficient k of the first and second inductors is smaller than 1 and the inductance coefficient coupling coefficient k of the third inductor is smaller than 1, a desired noise attenuation characteristic is obtained. Is set to an appropriate value.
- the first and second inductors are electromagnetically coupled to each other.
- the first and second inductors may each be formed by separate windings, or may be formed by a single winding.
- a connection point is provided in the middle of the single winding, and the first inductor and the other end of the winding are connected from one end of the winding to the connection point.
- the point up to the force connection point may be used as the second inductor.
- One end of the series circuit is connected to this connection point.
- the inductances of the first and second inductors may have the same value. When the first and second inductors are formed by a single winding, the inductances can be made equal by providing the connection point at the midpoint of the single winding, for example.
- one end of the series circuit is connected to a connection portion connected to the first and second inductors.
- the other end connected to the second conductive line is called a second end.
- An end of the first inductor opposite to the first end is called one end of the first inductor, and an end of the first inductor on the first end side is referred to as an end of the first inductor. Is called the other end of the first inductor.
- an end of the second inductor on the first end side is referred to as one end of a second inductor, and an end of the second inductor opposite to the first end is referred to as a first end. Called the other end of inductor 2.
- a normal mode voltage is applied between one end of the first inductor and the second end of the second conductive wire. Then, this voltage is divided by the first inductor and the series circuit, and predetermined voltages having the same direction are generated between both ends of the first inductor and between both ends of the series circuit. Since the first inductor and the second inductor are electromagnetically coupled to each other, a predetermined voltage is generated between both ends of the second inductor according to a voltage generated between both ends of the first inductor. .
- the direction of the voltage generated between both ends of the second inductor is The directions of the generated voltages are opposite to each other, and the voltages cancel each other.
- the voltage between the other end of the second inductor and the second end is applied between one end of the first inductor and the second end. Voltage lower than the applied voltage.
- a normal mode voltage is applied between the other end of the second inductor and the second end of the second conductive wire.
- the voltage between one end of the first inductor and the second end is equal to the voltage between the other end of the second inductor and the second end. It is smaller than the voltage applied between the head and the part.
- a desired noise attenuation characteristic can be obtained on condition that the inductance of the third inductor is smaller than 1 in the coupling coefficient k.
- LI and L2 are the same Value LO and L3 is the same value LO.
- the noise suppression circuit in particular, when the inductance L3 of the third inductor satisfies the following condition, the noise attenuating frequency characteristic is Almost the same characteristics as in the ideal state can be obtained.
- a noise suppression circuit is a circuit for suppressing normal mode noise transmitted by first and second conductive lines and causing a potential difference between these conductive lines. And a first and second inductors inserted in series with the first conductive line and magnetically coupled to each other, and a series circuit composed of a third inductor and a first capacitor connected in series. And fourth and fifth inductors inserted in series with the second conductive line and magnetically coupled to each other, and one end of the series circuit is connected to the first inductor. It is connected between the second inductor and the other end is connected between the fourth inductor and the fifth inductor.
- the coupling coefficient kl of the first and second inductors and the coupling coefficient k2 of the fourth and fifth inductors are smaller than 1, and the inductance coefficient kl, k2 of the third inductor is smaller than 1.
- the value is set so as to obtain a desired noise attenuation characteristic.
- the first and second inductors are electromagnetically coupled to each other as in the noise suppression circuit according to the first aspect.
- the fourth and fifth inductors can be similarly configured.
- a connection point is provided in the middle of a single winding, and the force at one end of the winding is also adjusted to the connection point by the fourth inductor.
- the fifth inductor may be from the other end of the winding to the connection point. The other end of the series circuit is connected to this connection point.
- the inductances of the fourth and fifth inductors may have the same value.
- the inductances can be made equal by providing the connection point at the midpoint of the single winding, for example.
- a connection portion at which one end of the series circuit is connected to the first and second inductors is referred to as a first end portion, and a connection portion at the other end connected to the fourth and fifth inductors. Is called the second end.
- An end of the first inductor opposite to the first end is called one end of the first inductor, and an end of the first inductor on the first end side is referred to as an end of the first inductor. Called the other end of the first inductor.
- the end of the second inductor on the first end side is referred to as one end of a second inductor, and the end of the second inductor opposite to the first end is referred to as a first end. Called the other end of inductor 2.
- An end of the fourth inductor opposite to the second end is called one end of a fourth inductor, and an end of the fourth inductor on the second end side is referred to as an end of the fourth inductor. Is called the other end of the fourth inductor.
- the end of the fifth inductor on the side of the second end is referred to as one end of a fifth inductor, and the end of the fifth inductor on the side opposite to the second end is referred to as one end of the fifth inductor. Called the other end of the fifth inductor.
- the noise suppression circuit when a normal mode voltage is applied between one end of the first inductor and one end of the fourth inductor, This voltage is divided by the first inductor, the series circuit, and the fourth inductor, and a predetermined voltage is applied between both ends of the first inductor, both ends of the series circuit, and both ends of the fourth inductor. Pressure develops. Since the first inductor and the second inductor are electromagnetically coupled to each other, a predetermined voltage is generated between both ends of the second inductor according to the voltage generated between both ends of the first inductor.
- the fourth and fifth inductors are electromagnetically coupled to each other, a predetermined voltage is applied across the fifth inductor according to the voltage generated across the fourth inductor. Occurs.
- one end of the series circuit is connected between the first inductor and the second inductor, and the other end is connected between the fourth inductor and the fifth inductor.
- the direction of the voltage generated between both ends of the inductor 2 and the direction of the voltage generated between the ends of the fifth inductor are opposite to the direction of the voltage generated between both ends of the series circuit. Offset each other.
- the voltage between the other end of the second inductor and the other end of the fifth inductor is equal to one end of the first inductor and one end of the fourth inductor. It becomes smaller than the voltage applied during.
- the noise suppression circuit when a normal mode voltage is applied between the other end of the second inductor and the other end of the fifth inductor, Similarly to the above description, the voltage between one end of the first inductor and one end of the fourth inductor is equal to the other end of the second inductor and the other end of the fifth inductor. Is smaller than the voltage applied between the first and second ends.
- a desired noise attenuation characteristic is obtained on condition that the inductance of the third inductor has a coupling coefficient kl, k2 smaller than 1. Since the value is set to a value that can be obtained, the frequency characteristics of the noise attenuation, for example, characteristics that are almost the same as the ideal state, characteristics that have a similar tendency, or characteristics that are partially better than the ideal state can get.
- L1 and L2 and L4 and L5 have the same value LO, and L3 has a value twice as large as LO.
- L3 has a value twice as large as LO.
- L1 inductance of the first inductor
- L2 inductance of the second inductor
- L4 inductance of the fourth inductor
- L5 inductance of the fifth inductor
- the noise suppressing circuit suppresses normal mode noise transmitted by the first and second conductive lines and causing a potential difference between these conductive lines.
- a circuit wherein the first and second inductors are inserted in series with the first conductive line and are magnetically coupled to each other, and the third inductor, the first capacitor, and the power connected in series.
- a fourth and a fifth inductor inserted in series with the second conductive line and magnetically coupled to each other with the first and second inductors. Are connected between the first inductor and the second inductor, and the other end is connected between the fourth inductor and the fifth inductor.
- the coupling coefficient kl of the first and second inductors, the coupling coefficient k2 of the fourth and fifth inductors, the coupling coefficient k3 of the first and fourth inductors, and the second and fifth inductors are all smaller than 1 and the inductance coefficient of the third inductor.
- the values are set to obtain desired noise attenuation characteristics.
- the first and second inductors on the first conductive line and the fourth and fifth inductors on the second conductive line are mutually magnetic.
- the basic operation of noise suppression is the same as that of the noise suppression circuit according to the above-described second aspect, although being different from the noise suppression circuit according to the second embodiment.
- the inductance-coupling coefficients kl, k2, k3, k4, k5, and k6 of the third inductor are all set to be / J, which is smaller than 1 by a factor of 1.
- the noise attenuation is set to a value that provides the desired noise attenuation characteristics
- the frequency characteristics of the noise attenuation are, for example, approximately the same as those in the ideal state, characteristics that have a similar tendency, or partial characteristics. In this case, characteristics superior to those in the ideal state can be obtained.
- LI, L2 and L4, L5 have the same value LO, and L3 has a value four times the LO.
- examples of the first conductive line and the second conductive line are as follows.
- each conductive line in a single-phase two-wire power line there are two of the three single-phase three-wire power lines that are currently used for power supply.
- noise suppression circuit According to the noise suppression circuit according to each aspect of the present invention, noise can be suppressed over a wide frequency range, and the size can be reduced.
- the inductance L3 in the series circuit is set to an appropriate value on condition that the coupling coefficient is smaller than 1, the frequency characteristic of the noise attenuation is, for example, almost the same as the ideal state, or Characteristics with a similar tendency or partially better than ideal conditions can be obtained.
- FIG. 1A is a circuit diagram showing a first configuration example of a noise suppression circuit according to a first embodiment of the present invention.
- FIG. 1B is a circuit diagram showing a second configuration example of the noise suppression circuit according to the first embodiment of the present invention.
- FIG. 2 is a diagram showing an example of an actual configuration of first and second inductors.
- FIG. 3 is a diagram showing a circuit configuration used in a first simulation for obtaining characteristics of the noise suppression circuit according to the first embodiment of the present invention.
- FIG. 4 is a characteristic diagram showing a first simulation result.
- FIG. 5 is a diagram showing a circuit configuration used in a second simulation for obtaining characteristics of the noise suppression circuit according to the first embodiment of the present invention.
- FIG. 6 is a characteristic diagram showing a result of a second simulation.
- FIG. 7 is a diagram showing a circuit configuration used in a third simulation for obtaining characteristics of the noise suppression circuit according to the first embodiment of the present invention.
- FIG. 8 is a characteristic diagram showing a third simulation result.
- FIG. 9A is a circuit diagram showing a first configuration example of a noise suppression circuit according to a second embodiment of the present invention.
- FIG. 9B is a circuit diagram showing a second configuration example of the noise suppression circuit according to the second embodiment of the present invention.
- FIG. 10 is a diagram showing an example of an actual configuration of first and second inductors and fifth and sixth inductors.
- FIG. 11A is a circuit diagram showing a first modification of the noise suppression circuit according to the second embodiment of the present invention.
- FIG. 11B is a circuit diagram showing a second modification of the noise suppression circuit according to the second embodiment of the present invention.
- FIG. 12 is a diagram showing a circuit configuration used in a simulation for obtaining characteristics of a noise suppression circuit according to a second embodiment of the present invention.
- FIG. 13 is a characteristic diagram showing a simulation result of an attenuation characteristic in the noise suppression circuit according to the second embodiment of the present invention.
- FIG. 14 is an explanatory diagram of a method of measuring a coupling coefficient.
- FIG. 15A is a circuit diagram showing a first configuration example of a noise suppression circuit according to a third embodiment of the present invention.
- FIG. 15B is a circuit diagram showing a second example of the configuration of the noise suppression circuit according to the third embodiment of the present invention.
- FIG. 16 is an explanatory diagram of a coupling coefficient between inductors in a noise suppression circuit according to a third embodiment of the present invention.
- FIG. 17 is a characteristic diagram showing a simulation result of an attenuation characteristic in the noise suppression circuit according to the third embodiment of the present invention.
- FIG. 18 is a circuit diagram showing an equivalent circuit of the noise suppression circuit used in the simulation of FIG.
- the noise suppression circuit according to the present embodiment is a circuit that suppresses normal mode (differential mode) noise transmitted by two conductive wires and causing a potential difference between these conductive wires.
- FIGS. 1A and 1B show first and second configuration examples of the noise suppression circuit according to the present embodiment.
- This noise suppression circuit includes a pair of terminals la and lb, another pair of terminals 2a and 2b, A first conductive line 3 connects between the terminals la and 2a, and a second conductive line 4 connects between the terminals lb and 2b.
- the noise suppression circuit further includes first and second inductors 51 and 52 inserted in series with the first conductive line 3.
- the noise suppression circuit also includes a series circuit 15 including a third inductor 53 and a first capacitor 14 connected in series. One end of the series circuit 15 is connected between the first inductor 51 and the second inductor 52, and the other end is connected to the second conductive line 4.
- connection portion where one end of the series circuit 15 is connected to the first and second inductors 51 and 52 is referred to as a first end P 1 and is connected to the second conductive line 4.
- the connection portion at the other end is referred to as a second end P2.
- an end of the first inductor 51 opposite to the first end P1 is called one end of the first inductor 51, and the first end P1 side of the first inductor 51 is referred to as a first end. Called the other end of one inductor 51.
- the first end P1 side of the second inductor 52 is called one end of the second inductor 52, and the end of the second inductor 52 opposite to the first end P1 is the first end. Called the other end of the second inductor 52.
- the third inductor 53 has a winding 13a wound around the magnetic core 13b.
- the first capacitor 14 functions as a high-pass filter that passes a normal mode signal having a frequency equal to or higher than a predetermined value.
- FIG. 1A shows that, of the third inductor 53 and the first capacitor 14, the third inductor 53 is located closer to the first end P1, and the first capacitor 14 is the second capacitor.
- FIG.1B conversely, the first capacitor 14 is arranged at a position closer to the first end P1, and the third inductor 53 is arranged at a position closer to the second end P2.
- FIG.1B conversely, the first capacitor 14 is arranged at a position closer to the first end P1, and the third inductor 53 is arranged at a position closer to the second end P2.
- the first and second inductors 51 and 52 are electromagnetically coupled to each other.
- the first inductor 51 has a winding 11a wound around the magnetic core 12a.
- the second inductor 52 has a winding l ib wound around the magnetic core 12b.
- the black circles on each winding indicate the polarity and direction of winding.
- the polarities of the first and second inductors 51 and 52 are in the same direction as illustrated.
- the first and second inductors 51, 52 are thus separated by separate windings 11a, lib, respectively. It may be formed, but it is also possible to form it with a single winding 11 as shown in FIG. The winding 11 is wound around the magnetic core 12. In FIG. 2, circuits other than the first and second inductors 51 and 52 are not shown.
- connection point (the first end P1) may be provided, and the one end force of the winding 11 may be the winding 11a up to the connection point and used as the first inductor 51.
- the second inductor 52 may be formed with a winding 1 lb up to the other end force connection point of the winding 11.
- One end of the series circuit 15 is connected to this connection point.
- the inductances of the first and second inductors 51 and 52 have the same value.
- the inductances can be made equal.
- the first and second inductors 51 and 52 are electromagnetically coupled to each other, and their coupling coefficient k is ideally 1.
- the coupling coefficient is 1, and even when the coupling state is relatively good, the coupling coefficient becomes a value such as 0.998.
- the coupling coefficient is affected by the core material, the number of windings, the winding method, and the like.
- the coupling coefficient is reduced to about 0.4.
- the smaller the number of turns the smaller the coupling coefficient tends to be.
- the magnetic permeability of the magnetic core the smaller the coupling coefficient tends to be. In this case, if the value of each circuit element is determined by regarding the coupling coefficient as 1, a problem arises that the originally expected amount of attenuation cannot be obtained.
- the value of each circuit element be determined according to the actual value of the coupling coefficient.
- the inductance L3 of the third inductor 53 is particularly large. Is set to a value corresponding to the actual value of the coupling coefficient k so that desired noise attenuation characteristics can be obtained, provided that the coupling coefficient k is smaller than 1.
- the first inductor 51 and the second inductor 52 are electromagnetically coupled to each other, a predetermined voltage is applied across the second inductor 52 according to the voltage generated across the first inductor 51. Voltage is generated.
- the direction of the voltage generated between both ends of the second inductor 52 is The direction of the voltage generated across both ends is opposite to the direction of the voltage generated, and these voltages cancel each other.
- the voltage between the other end of the second inductor 52 and the second end P2 that is, the voltage Vo between the terminals 2a and 2b, is equal to the voltage between one end of the first inductor 51 and the second end.
- the voltage VU applied between the end P2 and the end P2 also decreases.
- the inductances LI and L2 of the first and second inductors 51 and 52 are both set to the same value L0, and the inductance L3 of the third inductor 53 is also set to the same value L0.
- the impedance of capacitor 14 is zero.
- the inductances LI and L2 of the first and second inductors 51 and 52 are considered. This can be achieved, for example, by making the windings 11a and 1 lb of the first and second inductors 51 and 52 and the winding 13a of the third inductor 53 equal.
- the inductance of the winding is proportional to the square of the number of turns, the inductance of the entire winding 11 including the windings 11a and l ib is four times the inductance L3 of the third inductor 53. .
- the inductance L3 of the third inductor 53 is / 4 of the inductance of the winding 11.
- the third inductor 53 only needs to have a small inductance.
- FIG. 3 shows an equivalent circuit of the noise suppression circuit used in the first simulation.
- Ra and Rb are set as input and output impedances.
- Ra corresponds to the input / output impedance of the power system
- Rb corresponds to the input / output impedance of the device.
- the Rb side is set as the measurement device side.
- the element values of each circuit element used in the simulation are shown near each circuit symbol.
- the inductances LI and L2 of the first and second inductors 51 and 52 and the inductance L3 of the third inductor 53 were both set to the same value (1 ⁇ ).
- the attenuation characteristic was calculated when the value of the coupling coefficient k of the first and second inductors 51 and 52 was sequentially reduced from the ideal value of 1 to 0.8.
- FIG. 4 shows the result of the simulation. This is a graph showing the frequency characteristic of the attenuation amount of the normal mode noise in the noise suppression circuit.
- the horizontal axis represents frequency (Hz)
- the vertical axis represents gain (dB). The smaller the gain, that is, the greater the absolute value of the gain in the negative direction, the greater the amount of noise attenuation.
- the line indicated by reference numeral 64 indicates the simulation result when the coupling coefficient k is 0.9
- the noise suppression circuit even if the coupling coefficient k is smaller than 1, the value of the inductance L3 of the third inductor 53 is adjusted according to the value of the coupling coefficient k.
- the damping characteristics it is possible to obtain characteristics that are almost the same as those in the ideal state, or characteristics that have a similar tendency. Alternatively, by making a resonance point at an arbitrary frequency, characteristics that are partially superior to the ideal state can be obtained.
- FIG. 5 shows an equivalent circuit of the noise suppression circuit used in the second simulation.
- the values of the other circuit elements are the same as in the circuit of FIG.
- the line denoted by reference numeral 70 is in the ideal state
- the line indicated by reference numeral 79 0.
- the simulation results for the case of .08H are shown.
- the maximum value of the inductance L3 is determined based on the condition that the resonance frequency fO obtained by the above equation is desirably equal to or higher than the cutoff frequency in an ideal state.
- the minimum value of the inductance L3 is calculated from the simulation as L3 ⁇ 0.9k (Ll-L2) 12 & (3a)
- FIG. 7 shows an equivalent circuit of the noise suppression circuit used in this simulation.
- the coupling coefficient k was set to 0.8.
- the maximum value of the inductance L3 obtained from the above equation (2a) is
- Equation (3a) force The minimum value of the required inductance L3 is
- FIG. 8 shows the result of the simulation.
- the line denoted by reference numeral 81 is in the ideal state
- C indicates the capacitance of the first capacitor 14 of the series circuit 15. In this case as well, in a frequency band higher than the cutoff frequency and at a frequency up to the characteristic of the ideal state, a region where the attenuation characteristic is better than the characteristic of the ideal state occurs.
- the maximum value of the inductance L3 is determined based on the condition that the resonance frequency fO obtained by the above equation is desirably equal to or higher than the cutoff frequency in an ideal state.
- the characteristics show almost the same characteristics as the ideal state up to a certain state, and the attenuation characteristics deteriorate from a certain frequency or higher.
- the minimum value of the inductance L3 is calculated from the simulation as follows:
- the inductance L3 is set according to the value of the coupling coefficient k. Therefore, it is necessary to measure the value of the coupling coefficient k in advance in order to determine the value of the inductance L3. Next, a method of measuring the coupling coefficient k will be described.
- the coupling coefficient k can be obtained.
- FIG. 14 shows an example of a method of measuring the mutual inductance M.
- La and Lb are measured for the case where two coils are connected in series and the case where anti-phase is connected in series.
- the mutual inductance M can be obtained by the following equation. Note that La and Lb represent the inductance between the terminals.
- the normal mode noise can be effectively reduced over a wide frequency range without using a coil having a large force and a relatively simple configuration. Can be suppressed.
- the inductance L3 in the series circuit 15 is set to an appropriate value according to the value of the coupling coefficient k, the frequency characteristic of the noise attenuation is almost the same as the ideal state or similar to the ideal state. Trend characteristics or characteristics that are partially better than ideal can be obtained.
- the noise suppression circuit according to the first embodiment is an unbalanced circuit in which an inductor is inserted only into the first conductive line 3 of the two conductive lines 3 and 4.
- the noise suppression circuit according to the above is a balanced circuit by inserting inductors into both of the two conductive wires 3 and 4.
- FIGS. 9A and 9B show the first and second examples of the noise suppression circuit according to the second embodiment of the present invention. Is shown.
- the noise suppression circuits of FIGS. 9A and 9B are obtained by adding fourth and fifth inductors 54 and 55 to the configuration of the noise suppression circuit of FIGS. 1A and 1B. , 1B.
- the fourth and fifth inductors 54 and 55 are inserted in series with the second conductive line 4.
- a connection part where one end of series circuit 15 is connected to first and second inductors 51 and 52 is referred to as a first end P1
- the connection portion at the other end connected to the fourth and fifth inductors 54 and 55 is called a second end P2.
- an end of the first inductor 51 opposite to the first end P1 is called one end of the first inductor 51
- the first end P1 of the first inductor 51 is referred to as one end. Is called the other end of the first inductor 51.
- first end P1 side of the second inductor 52 is referred to as one end of the second inductor 52, and the end of the second inductor 52 opposite to the first end P1 is referred to as one end. Called the other end of the second inductor 52.
- the end of the fourth inductor 54 opposite to the second end P2 is called one end of the fourth inductor 54, and the fourth end of the fourth inductor 54 on the side of the second end P2.
- the end is referred to as the other end of the fourth inductor 54.
- the end of the fifth inductor 55 on the second end P2 side is called one end of the fifth inductor 55, and the end of the fifth inductor 55 on the opposite side to the second end P2.
- the end is referred to as the other end of the fifth inductor 55.
- FIG. 9A shows that, of the third inductor 53 and the first capacitor 14, the third inductor 53 is located closer to the first end P1, and the first capacitor 14 is the second capacitor.
- FIG. 9B shows that, of the third inductor 53 is located closer to the first end P1, and the third inductor 53 is closer to the second end P2. It is an example of the configuration provided.
- the fourth and fifth inductors 54 and 55 are electromagnetically coupled to each other.
- the fourth inductor 54 has a winding 21a wound around a magnetic core 22a.
- the fifth inductor 55 has a winding 2 lb wound around the magnetic core 22b.
- the black circles marked on each winding are the polarity and winding direction of the winding. Represents.
- the polarities of the first and second inductors 51 and 52 and the fourth and fifth inductors 54 and 55 may be opposite to those shown in the figure as long as the relationship between the windings is maintained. good.
- the fourth and fifth inductors 54 and 55 may be formed of separate windings 22a and 22b, like the first and second inductors 51 and 52, but as shown in FIG. It can also be formed by winding 21. The winding 21 is wound around the magnetic core 22. In FIG. 10, circuits other than the first and second inductors 51 and 52 and the fourth and fifth inductors 54 and 55 are not shown.
- connection point (the second end P2 )
- the one end force of the winding 21 is also used as the fourth inductor 54 with the winding 21a extending to the connection point.
- the other end force of the winding 21 may be set to the fifth inductor 55 with the winding 21b up to the connection point.
- the other end of the series circuit 15 is connected to this connection point.
- the inductances of the fourth and fifth inductors 54 and 55 are preferably the same as the inductances of the first and second inductors 51 and 52. More preferably, all the inductances of the first and second inductors 51 and 52 and the fourth and fifth inductors 54 and 55 should be the same.
- the fourth and fifth inductors 54 and 55 are formed by a single winding 21, for example, by providing the connection point at the middle point of the single winding 21, the fourth and fifth inductors 54 and 55 are formed. Each of the 55 inductances can be made equal.
- first and second inductors 51 and 52 are electromagnetically coupled to each other, and their coupling coefficient kl is ideally 1.
- the coupling coefficient k2 of the fourth and fifth inductors 54 and 55 is also ideally 1.
- a coupling coefficient of 1 cannot be realized in practice.
- the values of coupling coefficient kl of first and second inductors 51 and 52 and coupling coefficient k2 of fourth and fifth inductors 54 and 55 are actually different.
- the inductance L3 of the third inductor 53 is smaller than 1
- the actual noise attenuation characteristics can be obtained so that the desired noise attenuation characteristics can be obtained, provided that the inductance L3 of the third inductor 53 is smaller than 1. It is set to a value corresponding to the value of the coupling coefficient kl, k2.
- the method of determining the value of the distance L3 will be described later in detail.
- the first inductor 51 and the second inductor 52 are electromagnetically coupled to each other, the first inductor 51 and the second inductor 52 are connected across the second inductor 52 in accordance with the voltage generated across the first inductor 51. A predetermined voltage is generated.
- the fourth inductor 54 and the fifth inductor 55 are electromagnetically coupled to each other, the fourth inductor 54 and the fifth inductor 55 are connected to each other in accordance with the voltage generated across the fourth inductor 54. , A predetermined voltage is generated.
- one end of the series circuit 15 is connected between the first inductor 51 and the second inductor 52, and the other end is connected between the fourth inductor 54 and the fifth inductor 55.
- the direction of the voltage generated between both ends of the second inductor 52 and the direction of the voltage generated between both ends of the fifth inductor 55 are the same as the direction of the voltage generated between both ends of the series circuit 15. Are in opposite directions and their voltages cancel each other. As a result, the voltage between the other end of the second inductor 52 and the other end of the fifth inductor 55, that is, the voltage Vo between the terminals 2a and 2b, is increased by one end of the first inductor 51.
- the voltage VU applied between the second inductor 54 and one end of the fourth inductor 54 also becomes smaller.
- the noise suppression circuit according to the present embodiment even when a normal mode voltage is applied between terminals 2a and 2b, the voltage between terminals la and lb is changed between terminals 2a and 2b in the same manner as described above. It becomes smaller than the voltage applied to.
- the noise suppression circuit according to the present embodiment when the normal mode noise is applied to the terminals la and lb and when the normal mode noise is applied to the terminals 2a and 2b, In addition, normal mode noise can be suppressed.
- the voltage Vo between the terminals 2a and 2b becomes the voltage lZ4Vi between both ends of the second inductor 52, the voltage lZ4Vi between both ends of the fifth inductor 55, and the voltage between both ends of the third inductor 53. Since the voltage lZ2Vi cancels out, it becomes zero in principle. Also, when a normal mode voltage Vi is applied between the terminals 2a and 2b, the voltage between the terminals la and lb is basically zero as described above.
- the noise suppression circuit according to the present embodiment has the third inductor even if the coupling coefficients kl and k2 are smaller than 1.
- FIGS. 11A and 11B show modifications of the balanced noise suppression circuit shown in FIGS. 9A and 9B. More specifically, the degree of balance can be further increased compared to the noise suppression circuits in Figs. 9A and 9B. This is a modified example. Note that the noise suppression circuits of FIGS. 11A and 11B are different from the noise suppression circuits of FIGS. 9A and 9B only in the part of the series circuit 15 and are not shown because other circuit parts are the same. In particular, the noise suppression circuit of FIG.11A has twice the capacity of the first capacitor 14 with respect to the series circuit 15 which is also powerful with the third inductor 53 and the first capacitor 14 shown in FIGS.9A and 9B.
- the configuration is such that the third inductor 53 is sandwiched between the two capacitors 14a and 14b.
- the inductance L3 of the third inductor 53 in the circuit of FIG. 11A is the same as the third inductor 53 shown in FIGS. 9A and 9B.
- the noise suppression circuit of FIG. 11B is different from the series circuit 15 shown in FIGS. 9A and 9B in that the first capacitor 14 is used as it is and the first capacitor 14 is connected to the third inductor.
- the configuration is such that it is sandwiched between two inductors 53a and 53b having half the inductance of 53.
- FIG. 12 shows an equivalent circuit of the noise suppression circuit used in this simulation.
- Ra and Rb are set as input and output impedances.
- the attenuation characteristics when the value of the inductance L3 is variously changed were calculated.
- the line denoted by reference numeral 91 is in the ideal state
- the maximum value of the inductance L3 is determined based on the condition that the resonance frequency fO obtained by the above equation is desirably equal to or higher than the cutoff frequency in an ideal state.
- the lines indicated by reference numerals 96 and 97 correspond to (L3 16 ⁇ m).
- the attenuation characteristics shown in Fig. 13 characteristics similar to those in the ideal state are obtained.In particular, the characteristics are almost the same as those in the ideal state until a certain state, and the attenuation starts at a certain frequency. The characteristics deteriorate. For this reason, there is an advantage in setting L3 to this condition value if used in a frequency range substantially the same as the ideal state.
- the inductor is inserted into each of first and second conductive lines 3 and 4, and first and second conductive lines 3 and 4 are inserted. , 4 are configured to be balanced, so that the degree of balance between lines can be increased.
- the inductance L3 in the series circuit 15 is set to an appropriate value according to the values of the coupling coefficients kl and k2, the frequency characteristics of the noise attenuation are substantially the same as or similar to the ideal state. It is possible to obtain the characteristics of the tendency, or the characteristics partially better than the ideal state.
- Other configurations, operations, and effects of the present embodiment are the same as those of the first embodiment.
- FIGS. 15A and 15B show first and second configuration examples of the noise suppression circuit according to the third embodiment of the present invention.
- the noise suppression circuits of FIGS. 15A and 15B are different from the configuration of the noise suppression circuits of FIGS. 9A and 9B according to the second embodiment in the first and second inductors 51 and 52 and the fourth and fifth inductors, respectively.
- the fifth inductors 54 and 55 are magnetically coupled to each other. Except for the difference in the connection relationship, the basic configuration and the operation of noise suppression are the same as those of the noise suppression circuits in FIGS. 9A and 9B.
- the first and second inductors 51 and 52 and the fourth and fifth inductors 54 and 55 are connected to each other, for example, by winding the respective windings around the same magnetic core 12. Magnetically coupled. However, the magnetic core 12 may be a split core. In FIGS. 15A and 15B, the black circles marked on each winding indicate the polarity of the winding and the direction of winding. First and The polarities of the second inductors 51 and 52 and the fourth and fifth inductors 54 and 55 may be reversed from the illustrated ones if the relationship between the windings is maintained, .
- the coupling coefficient between first and second inductors 51 and 52 is kl
- the fourth and fifth inductors are The coupling coefficient between 54 and 55 is k2
- the coupling coefficient between first and fourth inductors 51 and 54 is k3
- the coupling coefficient between second and fifth inductors 52 and 55 is k4
- the first and fourth inductors are k4.
- the coupling coefficient between the five inductors 51 and 55 is defined as k5
- the coupling coefficient between the second and fourth inductors 52 and 54 is defined as k6.
- the first and second inductors 51 and 52 and the fourth and fifth inductors 54 and 55 are all magnetically coupled to each other, and the value of each coupling coefficient kl-k6 is Ideally it will be 1. However, it is impossible to realize that the coupling coefficient is actually 1
- the inductance of the third inductor 53 is particularly considered.
- L3 is set to a value corresponding to the actual value of the coupling coefficient kl-1 k6 so that a desired noise attenuation characteristic is obtained, provided that the coupling coefficient kl-1 k6 is smaller than 1.
- the inductances LI and L2 of the first and second inductors 51 and 52 and the inductances L4 and L5 of the fourth and fifth inductors 54 and 55 are both set to the same value LO, and the third inductor 53
- the state in which the inductance L3 is four times the value of LO is defined as an ideal state.
- the value of the inductance L3 of the third inductor 53 is changed to the value of the coupling coefficient kl-1 k6 even if it is smaller than the coupling coefficient kl-1 k6 force Si.
- Figure 18 shows the noise suppression used in this simulation.
- 2 shows an equivalent circuit of the circuit.
- Ra and Rb are set as input and output impedances.
- FIG. 17 shows the result of the simulation. This is a graph showing the frequency characteristics of the attenuation of the normal mode noise, as in FIG.
- the line indicated by reference numeral 105 15.9 ⁇
- the simulation results for 4 ⁇ m are shown.
- the line indicated by reference numerals 101 to 103 corresponds to ( ⁇ ⁇ 3> 16 / ⁇ ). In this case, a strong resonance point appears in an ideal state. And the resonance frequency
- the number fo is
- f indicates taking the square root of the whole C (L3—Ml—M2—M5—M6).
- C indicates the capacitance of the first capacitor 14 of the series circuit 15. Therefore, in this case, the resonance frequency can be moved to an arbitrary frequency by changing the value of L3.
- a region where the attenuation characteristic is better than that in the ideal state partially occurs in a frequency region higher than the cutoff frequency. That is, as shown in FIG. 17, in a frequency band higher than the cutoff frequency and until the characteristic coincides with the characteristic in the ideal state, there is a region where the attenuation characteristic is better than the characteristic in the ideal state.
- the maximum value of the inductance L3 is determined based on the condition that the resonance frequency fO obtained by the above equation is desirably equal to or higher than the cutoff frequency in an ideal state.
- the noise suppression circuit includes a ripple voltage generated by the power conversion circuit.
- a ripple voltage generated by the power conversion circuit.
- It can be used as a means to reduce noise on power lines and to prevent communication signals on indoor power lines from leaking to outdoor power lines.
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Filters And Equalizers (AREA)
- Power Conversion In General (AREA)
Abstract
Description
Claims
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US10/594,460 US7459995B2 (en) | 2004-03-31 | 2005-01-31 | Noise suppression circuit |
JP2006512266A JP4483863B2 (ja) | 2004-03-31 | 2005-01-31 | ノイズ抑制回路 |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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JP2004106098 | 2004-03-31 | ||
JP2004-106098 | 2004-03-31 |
Publications (1)
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WO2005101626A1 true WO2005101626A1 (ja) | 2005-10-27 |
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PCT/JP2005/001364 WO2005101626A1 (ja) | 2004-03-31 | 2005-01-31 | ノイズ抑制回路 |
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US (1) | US7459995B2 (ja) |
JP (1) | JP4483863B2 (ja) |
CN (1) | CN1938925A (ja) |
WO (1) | WO2005101626A1 (ja) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
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WO2017208919A1 (ja) * | 2016-06-01 | 2017-12-07 | 株式会社村田製作所 | フィルタ回路およびコネクタ |
US11309859B2 (en) | 2018-07-17 | 2022-04-19 | Kabushiki Kaisha Toyota Chuo Kenkyusho | Noise filter |
Families Citing this family (19)
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JP4231825B2 (ja) * | 2004-08-20 | 2009-03-04 | Tdk株式会社 | ノイズ抑制回路 |
US7423490B2 (en) * | 2006-03-31 | 2008-09-09 | Rockwell Scientific Licensing, Llc | Wideband high frequency chokes |
US7623001B2 (en) * | 2008-01-16 | 2009-11-24 | Universal Scientific Industrial Co., Ltd. | Electromagnetic interference eliminating apparatus |
US8115571B2 (en) * | 2008-11-28 | 2012-02-14 | Schaffner Emv Ag | Harmonic filter |
CA2689029C (en) * | 2008-12-24 | 2016-08-16 | Synergy Energy Inc. | Device for filtering harmonics |
US8670250B2 (en) * | 2010-09-13 | 2014-03-11 | Futurewei Technologies, Inc. | Common mode noise reduction apparatus and method |
JP5120434B2 (ja) * | 2010-09-30 | 2013-01-16 | 株式会社デンソー | 帯域阻止フィルタ |
DE102011007833A1 (de) * | 2011-04-21 | 2012-10-25 | Robert Bosch Gmbh | Auslöschung parasitärer Induktivitäten in zu elektrischen Wandlern parallel geschalteten Filterkondensatoren in einem Bordnetz für ein Fahrzeug |
WO2013136415A1 (ja) * | 2012-03-12 | 2013-09-19 | 三菱電機株式会社 | 電力変換装置 |
JP6108690B2 (ja) * | 2012-06-06 | 2017-04-05 | キヤノン株式会社 | 差動伝送回路及び電子機器 |
US9257894B2 (en) * | 2013-10-01 | 2016-02-09 | Tci, Llc | Reconfigurable passive filter |
US20160285360A1 (en) * | 2015-03-24 | 2016-09-29 | Ford Global Technologies, Llc | Method and apparatus for electromagnetic interference reduction |
CN106067778A (zh) * | 2015-04-23 | 2016-11-02 | 松下知识产权经营株式会社 | 磁气部件及电气电路 |
WO2017005863A1 (en) * | 2015-07-09 | 2017-01-12 | Constructions Electroniques + Telecommunications | High power density inverter (i) |
US10491181B2 (en) * | 2016-10-07 | 2019-11-26 | Murata Manufacturing Co., Ltd. | High-frequency filter and high-frequency module |
JP6812911B2 (ja) * | 2017-06-22 | 2021-01-13 | Tdk株式会社 | 電力変換装置 |
US10608313B2 (en) | 2018-01-08 | 2020-03-31 | Linear Technology Holding Llc | Wilkinson combiner with coupled inductors |
US11005442B2 (en) | 2019-05-23 | 2021-05-11 | Analog Devices International Unlimited Company | Artificial transmission line using t-coil sections |
TWI718029B (zh) * | 2020-03-17 | 2021-02-01 | 宏碁股份有限公司 | 加速放電裝置 |
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- 2005-01-31 CN CNA2005800100564A patent/CN1938925A/zh active Pending
- 2005-01-31 US US10/594,460 patent/US7459995B2/en not_active Expired - Fee Related
- 2005-01-31 JP JP2006512266A patent/JP4483863B2/ja not_active Expired - Fee Related
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JPS5364446A (en) * | 1976-11-22 | 1978-06-08 | Matsushita Electric Works Ltd | Filter electric wire |
JPS562632U (ja) * | 1979-06-15 | 1981-01-10 | ||
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US11309859B2 (en) | 2018-07-17 | 2022-04-19 | Kabushiki Kaisha Toyota Chuo Kenkyusho | Noise filter |
Also Published As
Publication number | Publication date |
---|---|
JPWO2005101626A1 (ja) | 2008-03-06 |
US7459995B2 (en) | 2008-12-02 |
CN1938925A (zh) | 2007-03-28 |
US20070241838A1 (en) | 2007-10-18 |
JP4483863B2 (ja) | 2010-06-16 |
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