This invention relates to an arrester structure that is installed in a low-voltage AC power circuit and adapted for bypassing and discharging a lightning current to the ground in order to protect an electronic device sensitive to overvoltage when lightning strike occurs.
After the Franklin lightning conductor was invented in the late 1700s, lightning conductors and conductor wires were exclusively used as devices for protecting buildings from lightning for about 200 years (external protection from lightning). This is because damage could be minimized by receiving a lightning stroke current by these conductors and discharging it to the ground at the shortest distance via a grounding electrode. As distribution lines and telephone lines began to spread in the early 1900s, many accidents occurred in which insulating parts of electric and communication devices are broken by a lightning current that flowed into a building via these electric wires or a lightning current that flowed into the grounding on the outside of the building via these electric wires when lightning struck the building. Particularly recently, since the degree of spreading of electronic devices is increased and they serve as the central parts of economy, transportation, electric power, communications and production management, preventive measures against system down due to lightning strike is an important technical problem.
As a method for preventing an accident due to a lightning current flowing into a building or a lightning current flowing out of a building, it is proposed as best to electrically connect the principal metal parts (for example, steel frames, steel rods and the like) of the basic structure of the building to form basic grounding, provide a single or plural grounding buses within the building, connect the grounding buses to the basic grounding at the shortest distance, and electrically connect all the metal pipes (for example, water pipe, gas pipe and the like) and electric wires (distribution lines, telephone lines, antenna lines and the like) led in from outside, to a bonding bar near the entrance (equipotential bonding). This was standardized in Germany in 1987 (non-patent reference 1). This standard was employed as an international standard, with its contents substantially unchanged (non-patent reference 2). Also in Japan, a new standard in conformity to the above-mentioned IEC standard was established (non-patent reference 3).
With respect to lightning current at the time of lightning strike, the international standard (non-patent reference 4) presents the current values, waveforms and quantities of electric charges shown in Table 1.
1)Since the majority of the entire charges Qs is included in the first lightning stroke, the entire discharging charges coincide with the presented values.
2)Since the majority of the intrinsic energy W/R is included in the first lightning stroke, the intrinsic energy of all the discharges coincides with the presented values.
3)The protection level is decided by the frequency of lightning strike and the importance of the building to be protected (level I > II > III > IV).
The crest value I of lightning current of 100 to 200 kA and the duration of wave tail T2 of 350 μs were values largely exceeding the conventionally expected values. The change of the reference waveform clarifies on one hand that the conventional arrester burns and explodes relatively easily at the time of lightning strike and does not serve as intended as the arrester, and suggests on the other hand that large increase in the amount of impulse current resistance of the lightning current arrester is necessary.
The arrester that has been conventionally used most often in order to limit the overvoltage generated in distribution lines is a device including varistor device made of zinc oxide, as a principal element. The current and voltage waveforms when an impulse current flows through the zinc oxide varistor are shown in
However, as shown in
Table 2 shows the relation between the threshold load value of the varistor (it can be loaded once without being broken) with respect to an impulse current of 10/350 μs and the diameter of the varistor.
It can be understood that only an amount of resistance that is ¼ required amount of impulse current resistance of 20 kA is acquired even if a large varistor with a diameter of 80 mm is used.
An arrester including a spark gap as a principal element has an overvoltage switching characteristic by nature (see
However, in order to realize practical use of the spark gap as a lightning current arrester, there are two technical problems to be solved.
1) After a lightning impulse current vanishes, a follow current flows from the power circuit through the ionized air path. If this follow current is intercepted by an external protection circuit, inconvenience occurs such as the loss of the protective function against overvoltage due to shutdown of power supply to the load circuit or shutdown of the spark gap arrester from the power line.
2) When a large lightning impulse current flows, the air on the periphery of the aerial arc discharge path is heated and ionized and thus explosively expands and erupts, thereby affecting the peripheral wiring and equipment.
The problem 2) is solved by the technique of patent reference 1.
It cannot be said that the foregoing problem 1) is completely solved by the above-described structure of patent reference 1. It is because an arc voltage is dependent on an arc current and the following equation generally holds under the condition of constant pressure.
UB=(UA+UK)+RB*IB
Here, UB is arc voltage, UA+UK is anode voltage drop plus cathode voltage drop, RB is arc resistance, and IB is arc current.
When the power circuit impedance and/or the arc resistance RB is relatively large, the current waveform of follow current 1 appears. Since the power restriking voltage at the current-zero point is 60 V or less, the follow current vanishes at this point. However, when the power circuit impedance and the arc resistance are small, the current waveform of follow current 2 appears. Since the power restriking voltage at the current-zero point is 60 V or more, the arc restrikes and the follow current continues.
Patent Reference 1: Specification of Laid-Open European Patent Application No. 78434
Non-Patent Reference 1: DIN VDE 0185, Part 100, “Prescriptions and general principles with respect to protection of buildings against lightning”
Non-Patent Reference 2: IEC 61024-1 (1990), “Protection of structures against lightning, Part 1”
Non-Patent Reference 3: JIS A 4201-2003, “Protection of architectures against lightning”
Non-Patent Reference 4: IEC 61312-1 (1995), “Protection against lightning electromagnetic impulse, Part 1, General principles”
Problems that the Invention is to Solve
Thus, an object of this invention is to realize a spark gap arrester of a sealed structure in which restrike after passage of a lightening current is prevented, generating no follow current.
Means for Solving the Problems
A voltage drop independent of an arc current is provided by inserting a metal plate into an arc discharge path to split the arc and then generating anode and cathode voltage drops on both sides of the metal plate. Since the voltage drop acquired by a pair of anode and cathode electrodes is about 60 V, if a power-supply voltage of 200 V is assumed, at least four metal plates must be added in order to acquire a voltage drop of 300 V.
When a conductor is arranged near a magnetic material plate and a current is flowed through the conductor, an attraction force acts between the magnetic material plate and the conductor. This is because magnetic fluxes generated by the current are usually concentric about the conductor, whereas if there is a magnetic material having high permeability near the conductor, the majority of the magnetic fluxes are concentrated within the magnetic material and the magnetic flux density of the magnetic material-side part of the conductor is lowered. This attraction force becomes zero if the conductor shifts to the center of the magnetic material plate. In this invention, this principle is applied and an arc generated between the two discharge electrodes at the time of lightning strike is shifted into a grid structure of arc-suppressing plates, thus suppressing the arc.
Moreover, as auxiliary means for shifting the arc discharge path, it is effective to arrange an arc-suppressing insulating material (polyacetal, polypropylene or the like) and utilize arc-suppressing gas that erupts because of thermal decomposition of the above-mentioned insulating material when an arc is generated.
Advantage of the Invention
According to the structure of this invention, excellent advantages as follows can be provided.
10 building structure, 11 bonding bar, 12 arrester, 20 distribution transformer, 21 secondary winding as described above, 31 lightning strike point, 32-36 lightning current path, R1, R2 grounding resistance, 100 spark gap, 101a, 101b electrode copper-tungsten chip, 102a, 102b electrode copper member, 103a, 103b flange, 104a, 104b terminal screw, 105a, 105b air duct, 106 arc chamber, 201-209 arc-suppressing plate, 301 insulator, 302 insulating pipe, 303a, 303b insulating ring, 304a, 304b insulating cap, 305a, 305b insulating plate, 306 metal pipe, 311 spacer ring, 312 air gap
Hereinafter, the structure and function of an arrester for a low-voltage AC power circuit according to this invention will be described in detail with reference to
On the outer side of the insulator 301, an insulating pipe 302 made of an organic arc-suppressing insulating material, for example, polyacetal, polypropylene or the like, is arranged. The pipe 302 decomposes by the heat when arc discharge (arc a) is generated in the spark gap, and erupts arc-suppressing gas, thus shifting an arc leg point to the conical surfaces of the electrodes 101a, 101b on the outer side of the gap (arc b).
In the above-described arc chamber 106, n metal magnetic material arc-suppressing plates, in this embodiment, nine metal magnetic material arc-suppressing plates 201 to 209 are arranged which are concentric with the circular cross sections of the conical electrodes 101a, 102a and 101b, 102b. The metal magnetic material may be, for example, wrought iron. Since the arc-suppressing plate 205 at the center is arranged at the nearest position to the gap, the arc discharge path shifts outward because of the above-described attraction force that acts between the arc discharge path and the inner edge of the ring, and first, the arc-suppressing plate 205 enters the arc discharge path. On both sides thereof, the cathode and anode of arc discharge are formed (arc c).
Thus, an arc voltage of (UA+UK) equal to approximately 60 V is applied. Next, all the arc-suppressing plates 201 to 204 and 206 to 209 on both sides of the arc-suppressing plate 205 similarly and sequentially enter the arc discharge path. Ultimately, an arc d across all the arc-suppressing plates is formed and an arc voltage of n×(UA+UK) (V) is applied.
Insulating rings 303a, 303b, made of an arc-suppressing insulating material and covering the lateral sides of the two discharge electrodes 101a, 102a and 101b, 102b, prevent an arc leg point from being generated there and have an effect of promoting the extension of the arc discharge path.
The arc discharge path is maintained even when the impulse current exceeds the peak value and enters the attenuation process. However, when the current value becomes substantially zero, if the instantaneous power-supply voltage value V1 is smaller than the arc voltage, no follow current is generated from the power supply and the arc vanishes.
When the lightning impulse current value is relatively small, the impulse current may vanish at the stage of arc a or b. In this case, since the arc voltage does not increase sufficiently, a follow current from the power supply can be generated. Also the arc due to the follow current, like the arc due to the impulse current, is shifted outward of the gap by arc-suppressing gas erupting from an insulating pipe 302 made of an organic arc-suppressing insulating material, and to the conical surfaces of the discharge electrodes 101a, 101b, causing creeping discharge (arc b). Moreover, the arc is shifted to arc c and d by the attraction force from the arc-suppressing plates.
Because of the cooling effect due to the contact of the arc with the arc-suppressing plate, and the cathode and anode voltages generated on both sides of the metal ring, the follow current is quickly reduced and vanishes near the AC voltage zero point. Since the arc resistance is sufficiently large, even if the power-supply impedance is sufficiently small, the follow current has the waveform of follow current 1 in
Since all of the discharge electrodes, the arc-suppressing insulating members and the arc-suppressing magnetic material rings are arranged in the rotationally symmetrical structure, wherever the first spark discharge occurs in the main electrode, the self-arc-suppressing function is the same.
To fix the positions of the metal magnetic material rings 201 to 209 and to maintain insulation from the metal pipe 306, a spacer ring 311 having a step-like cross section is used. To cool the arc and to prevent the arc from transferring to the metal pipe, using an organic arc-suppressing insulating material for the spacer ring 311 is effective.
To reduce the residual magnetism of the magnetic material metal rings 201 to 209 used as arc-suppressing plates, a part of the metal rings is cut out to provide an air gap 312 in the magnetic path, as shown in
Number | Date | Country | Kind |
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2004-025367 | Feb 2004 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP05/00991 | 1/26/2005 | WO | 9/7/2006 |