TW432409B - A reactor - Google Patents

A reactor Download PDF

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Publication number
TW432409B
TW432409B TW88104659A TW88104659A TW432409B TW 432409 B TW432409 B TW 432409B TW 88104659 A TW88104659 A TW 88104659A TW 88104659 A TW88104659 A TW 88104659A TW 432409 B TW432409 B TW 432409B
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Taiwan
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reactor
patent application
scope
coil
item
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TW88104659A
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Chinese (zh)
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Hakan Kols
Thorsten Schutte
Kjell Andersson
Mats Ekberg
Kailash Srivastava
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Asea Brown Boveri
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Abstract

A reactor comprises a plurality of windings (3-5) each adapted to be connected to a phase (6-8) of a multiphase alternating voltage. The windings are configurated so that they upon connection to said voltage are influenced substantially by the same magnetic flux. At least one of said windings is at least partially formed by a cable in the form of a flexible electric conductor with an envelope able to confine the electric field created around the conductor.

Description

赝432 4 Ο 9 _案號 88104659_年月日_j|vi_ 五、發明說明(1) 發明領域及習知技術 本發明之發明領域係有關於一包含多個線圈的電抗 器*各線圈適於連接多相交變電壓中的一相。 該多相交變電壓中的各相具有至少一所連接之電抗器 的線圈,但是確定線圈的數目高於相數,二或多個線圈並 或串聯至一或多相中。 此電抗器可使用在許多不同的領域中,其中在某些情 況下,必需可影響電磁量者。 為了說明本發明及本發明所欲解決的問題(但是並非 用於限制本發明),此將於下文中加以說明當在用於傳送 或分配電力的電力裝置或網路中產生錯誤時,或者是當該 多相交變電壓發生不對稱時的一種電抗器,其具有用於保 護不同型式之電力設備之型式° 必需指出多相交變電壓之相數目可為任何大於一的數 目,但是在此將於下文中加以三相電壓的例子,此係因為 三相電壓為最常見的多相電壓。而且,必需強調的是,本 發明並不限制在特定的電壓範圍内,而是可應用在低介質 及高電壓的情況。 在上述最後說明之此類型的電抗器最好加以連接,使 得不同電壓源及電力裝置或問題中的網路之間互相串聯。 該裝置或網路被連接到具有不同電壓位準的二或多個交變 電壓,其適於將此類型的電抗器_聯在該裝置或網路及一 或多個電壓源之間。例如,此可為變壓器或傳輸線。在此 電抗器之電壓的型式可解釋為經由在特定干擾下,於不同 線圈中,由電流感測之等效電感的改變所產生,且由此,赝 432 4 Ο 9 _case number 88104659_year month_j | vi_ V. Description of the invention (1) Field of invention and known technology The field of invention of the present invention relates to a reactor including a plurality of coils. For connecting one of the phases of a multiphase alternating voltage. Each phase in the polyphase alternating voltage has at least one coil of a connected reactor, but it is determined that the number of coils is higher than the number of phases, and two or more coils are connected in series to one or more phases. This reactor can be used in many different fields, and in some cases it must be able to affect the electromagnetic quantity. In order to explain the present invention and the problems it intends to solve (but not to limit the present invention), this will be explained below when an error occurs in an electric device or network for transmitting or distributing power, or When the polyphase alternating voltage is asymmetric, it has a type for protecting different types of electrical equipment. It must be noted that the number of phases of the polyphase alternating voltage can be any number greater than one, but here it will be Examples of three-phase voltages are given below because three-phase voltages are the most common multi-phase voltage. Moreover, it must be emphasized that the present invention is not limited to a specific voltage range, but can be applied to low dielectric and high voltage situations. The reactors of the type described at the end are preferably connected so that different voltage sources and electrical installations or the network in question are connected in series. The device or network is connected to two or more alternating voltages having different voltage levels, which is suitable for connecting a reactor of this type between the device or network and one or more voltage sources. This can be, for example, a transformer or a transmission line. Here, the type of the reactor voltage can be interpreted as being caused by the change in the equivalent inductance of current sensing in different coils under specific interference, and therefore,

第5頁 Ρ4 32 4 Ο 9 ^ m ^ α 案號 88ΗΜ659_年月日__ 五、發明說明(2) 改變電抗器的等效電感。 通常有必要在提供沒有任何干擾的交變電壓時,電抗 器不必加以注意,即需要使電壓降達到最小。但是,又相 當需要當發生任何型式的干擾時,電抗器上的電壓降可相 當得高,因此可保護該設備防止高電流。在熟知之此類型 的電抗器中,無法結合這兩類型的需要,因此之間必需取 得妥協=此意指如果需要相當高的電壓降,且由此在不對 稱錯誤時,可得到有效的電抗器之電流限制性質時,在電 流操作期間,不可忽略一項事實:即必需接受某一程度的 電壓降。此大部份係由於當設計此電抗器的尺寸時,選擇 一中間尺寸的關係,因此在此兩種情況令可得到π中間結 果”。 一正常的三相電抗器中具有正及負的序列電感,其至 少必需高到如其本身的零序列電流一般。此意指如果如在 地面錯誤所導致零序列電流將實際上限制此類型的電抗器 時,甚至在對稱的交變電壓下,電壓降相當得高。在此例 子中沒有任何的零序列電流,但是當由於錯誤或其他的干 擾零序列電流產生而導致的相交變電壓中的不對稱,則必 需加以限制。此類型的電抗器試著由導入較高電感而產生 高的電壓降以完成此項限制。零序列電流相當低,且在三 個腳的電抗器中,此電流限制效應相當低。然而在轉動腳 電抗器中,零序列電流將約高到加及減序列電感般。此意 指後者必需製造得相當大,以使得零序列電流可感測到足 夠高的電感以使電抗器的電流限制效應相當良好。 發明概述Page 5 Ρ4 32 4 Ο 9 ^ m ^ α Case No. 88ΗΜ659_ 年月 日 __ V. Description of the invention (2) Change the equivalent inductance of the reactor. It is usually necessary to avoid the need for reactors to provide an alternating voltage without any interference, that is, to minimize the voltage drop. However, it is quite necessary that when any type of interference occurs, the voltage drop across the reactor can be reasonably high, thus protecting the device from high currents. In the well-known reactors of this type, it is not possible to combine the needs of the two types, so a compromise must be achieved = this means that if a relatively high voltage drop is needed, and thus an asymmetrical error, an effective reactor can be obtained In the current limiting nature of the device, during the current operation, one fact cannot be ignored: that is, a certain level of voltage drop must be accepted. Most of this is because when designing the size of this reactor, a relationship of intermediate size is selected, so in these two cases, π intermediate results can be obtained. "A normal three-phase reactor has positive and negative sequences. The inductance must be at least as high as its own zero-sequence current. This means that if the zero-sequence current, as caused by a ground error, will actually limit this type of reactor, even at a symmetrical alternating voltage, the voltage drop Quite high. In this example, there is no zero-sequence current, but when the asymmetry in the alternating voltage due to errors or other disturbing zero-sequence currents, it must be limited. This type of reactor tries This limitation is achieved by introducing a high voltage drop due to the introduction of a higher inductance. The zero-sequence current is quite low, and in a three-pin reactor, this current-limiting effect is quite low. However, in a rotating-pin reactor, the zero-sequence The current will be about as high as the plus and minus sequence inductance. This means that the latter must be made quite large so that the zero sequence current can sense a sufficiently high inductance to make The current limiting effect of the reactor is quite good.

第6頁 ^4324 0 9 _案號88104659_年月日_魅_ 五、發明說明(3) 因此,本發明的目的係提供一種定義在上述簡介中之 類型的電抗器τ此電抗器可處理上述說明的問題,及用於 熟知之電抗器的相關問題。本發明的第二目的係提供一具 有一架構的電抗器,此架構為可改進熟知之此類型的電抗 器,使製造程序簡化,提高可靠度,操作時的功率耗損 低,價格低等優點,在商用上比已知電抗器更具價值。 上述主要目的可由此類型電抗器的線圈達成,使得當 連接到該電壓時可為實際上相同的磁通量所影響。 經由配置該線圈,使得其實際上為相同的磁通量所影 響,則有可能配置連接線圈,使得在正常的情況上,磁通 量實際上為0。即,在供應對稱之多相交變電壓時,意謂 者不同的電流原則上不同導致任何的電感,且線圏的電 壓降將達到最小。但是,可依據下列方式架構電抗器:使 不同線圈的自感相當高,由一零序列電流而由電感感測出 來,由此,需要非常高的電壓降以驅動此電流,此將導致 非常強的電流限制,且維持此零序列電流在一可接受的範 圍之内。因為本發明的電抗器不會干擾正常的操作,所以 依據此方式,有可能使得0序列電感甚高於傳統電抗器所 必需者。例如傳輸網路的電裝置可依據此方式,而有效地 保護極高的地表錯誤電流或者是當如樹掉落在網路線上等 的情況下所產生的短路現象。電抗器的性能可使用在用於 第三諧波及其倍數的濾波器。電抗器可有效地濾掉這些諧 波,而不影響基本電流。因此,電流限制裝置及第三諧波 濾波器的結合可由一個相同的電抗器得到,從節省成本的 觀點看來,此方式也極令人感興趣。須特別聲明的是電抗Page 6 ^ 4324 0 9 _Case No. 88104659_Year Month Date_Character_ V. Description of the invention (3) Therefore, the object of the present invention is to provide a reactor of the type defined in the above introduction τ. This reactor can handle The problems described above, and the problems associated with well-known reactors. A second object of the present invention is to provide a reactor with a structure that can improve the well-known reactors of this type, simplify the manufacturing process, improve reliability, low power loss during operation, and low price. Commercially more valuable than known reactors. The above main purpose can be achieved by the coils of this type of reactor, so that when connected to this voltage it can be affected by virtually the same magnetic flux. By arranging the coil so that it is actually affected by the same magnetic flux, it is possible to configure the connection coil so that, under normal circumstances, the magnetic flux is actually zero. That is, when supplying symmetrical multi-phase alternating voltage, it means that different currents in principle cause any inductance, and the voltage drop of the line coil will reach the minimum. However, the reactor can be structured according to the following methods: the self-inductance of the different coils is quite high, and the zero-sequence current is sensed by the inductor. Therefore, a very high voltage drop is required to drive this current, which will cause a very strong Current limit and maintain this zero-sequence current within an acceptable range. Because the reactor of the present invention does not interfere with normal operation, according to this method, it is possible to make the 0-sequence inductance much higher than that required by the conventional reactor. For example, the electrical equipment of the transmission network can effectively protect the extremely high ground fault current or short circuit generated when a tree falls on the network line according to this method. The performance of the reactor can be used in filters for the third harmonic and its multiples. Reactors effectively filter out these harmonics without affecting the basic current. Therefore, the combination of the current limiting device and the third harmonic filter can be obtained by a same reactor, which is also very interesting from the viewpoint of cost saving. Special declaration is required for reactance

第7頁 修正 4 Ο 9 號 88104659 年 五、發明說明(4) 器被動限制電流,即自動限制零序列電流。因此,不需要 特別偵測零序列電流,然後此將執行一量測作業,此限制 了零序列電流。在許多電廠中,此方式具有相當大的優 點。但是,有時候,必需偵測從其他目的上所產生的錯誤 電流,如控制一斷路器。此完全與錯誤電流數目相關的偵 測可由一般磁通量谓測的任何型式輕易地執行。 依據本發明的較佳實施例,選擇線圈數,線圈的繞線 方向及每線圈的繞線數,使得在該線圈中流動的磁通量當 以對稱方式供應多相交變電壓予線圈時,該磁通量大致上 為0。因此,由此在供應對稱電流時,電感對這些電流的 影響相當的低。此優點可從上文中了解。 依據本發明的另一較佳實施例,相數為3 *且本發明 尤適於多相者,此係因為在此例子中可輕易地得到流過線 圈之電流,當以1 2 0度的電流相位差而供應對稱電流時, 驅動磁通量之電流,兩電流的加總大致上為0。如果線圈 繞線例如與屬於將相等之對應相的線圈之線圈繞線數目結 合的同一方向時,則驅動磁通量之電流合為0。 依據本發明的另一較佳實施例,配置屬於不同相之線 圈使彼此互相靠近。此可容易地確定線圈將受到大致上相 同之磁通量的影響,且磁漏通量將維持在一低數值下。在 空氣電抗器的例子t,往往需要此特徵,但是在具有磁性 核心的電抗器中,其重要性則未必如此,當然往往也需要 此特性。 依據本發明的另一較佳實施例,線圈均通過一封閉磁 路,且依據本發明另一較佳實施例,一電抗器包含一包圍Page 7 Amendment No. 4 〇 9 88104659 Fifth, the description of the invention (4) The device passively limits the current, that is, it automatically limits the zero-sequence current. Therefore, it is not necessary to specifically detect the zero-sequence current, and then a measurement operation is performed, which limits the zero-sequence current. This approach has considerable advantages in many power plants. However, sometimes it is necessary to detect erroneous currents for other purposes, such as controlling a circuit breaker. This detection, which is entirely related to the number of error currents, can be easily performed by any type of general magnetic flux measurement. According to a preferred embodiment of the present invention, the number of coils, the winding direction of the coils, and the number of windings per coil are selected so that when a multi-phase alternating voltage is supplied to the coils in a symmetrical manner, the magnetic flux is approximately Up is 0. Therefore, when supplying symmetrical currents, the influence of inductance on these currents is quite low. This advantage can be understood from the above. According to another preferred embodiment of the present invention, the number of phases is 3 *, and the present invention is particularly suitable for multi-phase ones. This is because in this example, the current flowing through the coil can be easily obtained. When the current phase is different and a symmetrical current is supplied, the current of the driving magnetic flux is approximately zero. If the coil windings are, for example, in the same direction as the number of coil windings belonging to the coils of equal corresponding phases, the current for driving the magnetic flux becomes zero. According to another preferred embodiment of the present invention, the coils belonging to different phases are arranged so as to be close to each other. This makes it easy to determine that the coils will be affected by approximately the same magnetic flux and that the magnetic leakage flux will be maintained at a low value. In the case of the air reactor t, this feature is often required, but in a reactor with a magnetic core, its importance is not necessarily so. Of course, this feature is also often required. According to another preferred embodiment of the present invention, the coils pass through a closed magnetic circuit, and according to another preferred embodiment of the present invention, a reactor includes a surrounding

[432409 _案號 88104659_年月曰__ 五、發明說明(5) 線圈之封閉磁路。應用此封閉磁路,應用一簡單的方式, 可使得線图將為大致上相同的磁通量所影響,且將磁通量 通過此磁路或核心,且當在供應的交變電壓中發生不對稱 時,可由對電流之不對稱的分配,而感測極高的電感。電 壓為磁性核心時,則可改進電流限制特性° 依據本發明的較佳實施例,電抗器的核心可加以磁 化,且形成實際上的封閉迴路。此可將磁通量的主要部位 維持在核心内部,且可限制磁漏通量,因此在對稱供應 時,可得到可能的最低電壓降。 依據本發明的另一較佳實施例,線圈通過完全或部份 繞著且包圍該磁路,且在空氣電抗器的例子中,如對於磁 通量不具有任何磁性核心的電抗器,最好可實際上完全的 包圍,此係因為不必使用昂貴的核心。本發明電抗器也可 以設計其尺寸以適應比封閉電抗器還要高的磁場,因此整 個架構可設計得較精緻。其缺點為在不對稱情況下,其電 流限制能力將比含空氣核心的電抗器還要低。 依據本發明另一較佳實施例,磁路包圍一圓形區域。 此設計意謂著在形成使用較少材料的電路之磁漏核心的例 子中,可以較低的成本製造電抗器。在此例子中該核心可[432409 _ case number 88104659_ year month __ V. Description of the invention (5) The closed magnetic circuit of the coil. Applying this closed magnetic circuit, applying a simple method, can make the line diagram be affected by approximately the same magnetic flux, and pass the magnetic flux through this magnetic circuit or core, and when asymmetry occurs in the supplied alternating voltage, Extremely high inductance can be sensed by the asymmetric distribution of current. When the voltage is a magnetic core, the current limiting characteristic can be improved. According to a preferred embodiment of the present invention, the core of the reactor can be magnetized and form a practically closed loop. This can maintain the main part of the magnetic flux inside the core and limit the magnetic leakage flux, so that when the supply is symmetrical, the lowest possible voltage drop can be obtained. According to another preferred embodiment of the present invention, the coil passes around the magnetic circuit completely or partially and surrounds the magnetic circuit. In the case of an air reactor, for example, a reactor that does not have any magnetic core in the magnetic flux, it is best to be practical. It is completely surrounded because it does not have to use an expensive core. The reactor of the present invention can also be designed to have a size to accommodate a higher magnetic field than a closed reactor, so the entire structure can be designed more delicately. The disadvantage is that under asymmetric conditions, its current limiting capability will be lower than that of a reactor with an air core. According to another preferred embodiment of the present invention, the magnetic circuit surrounds a circular area. This design means that in the case of forming a magnetic leakage core of a circuit using less material, a reactor can be manufactured at a lower cost. In this example the core can

年月 修正 五、發明說明(6) 形的腳。 依據本發明 因此電抗器 的另一較佳實 的電感實際上 一封閉的磁漏核心中得到 要。 的第二目的係 施例,磁路至少有一空氣間隙。 為線性者,在某些例子中,比從 較好的電流限制能力來說,此項 性能更為重 本發明 之線圈中以 含包封的韌 場。 經由可 的電場之可 產生的耗損 以不必冷卻 的方式架構 在製造及上 項使用導致 料而沒有相 此實施 心的例子中 考量到線圈 依據本 有的線圈。 化,本發明 得不同線圈 圈繞線具有 在申請專利範圍第1項之電抗器 一電纜線形成至少一線圈,該電纜線的型式為 性電導體,該包封可限制繞著導體產生的電 實際上 能性, 。減少 ,且與 冷卻裝 優於今 在一絕 關的缺 例的另 ,與傳統上使 之間的絕緣問 發明的另一較 因此有可能使 的另一實施例 可至少 屬於另 限制在絕緣體系統中,由該電導體產生 該電抗器可更具效率,即可減少其中所 耗損復導致電抗器具有較低的溫度,所 不使用此線圈之架構比較下,以更簡單 置。該電纜線可為韌性電纜線,此意指 日習知技術仍使用之硬線圈。而且,此 緣體系統中,不使用氣體及液體絕緣材 點。 為在共用線圈之電抗器的磁漏核 用的核心比較下,本發明更易於 題。 佳實施例,由固態電纜線形成所 用此電纜線的優點為達到最適 使得可經由使两此電缓線,而使 一部份互相混合,即屬於相同線圈的線 一線圈的線圈繞線,而另一相完全或部 優點Year, month, amendment 5. Description of invention (6) Shaped feet. According to the invention, another preferred practical inductance of the reactor is actually obtained in a closed magnetic leakage core. A second purpose of the embodiment is that the magnetic circuit has at least one air gap. It is linear. In some examples, this performance is more important than the better current limiting capability. The coil of the present invention includes an encapsulated tough field. The losses that can be generated through the possible electric field are structured in a way that does not need to be cooled. In the example of manufacturing and the use of the above, the material is not related. In this example, the coil is based on the existing coil. In the present invention, the coils of different coils have at least one coil formed by the reactor and a cable in the first patent application scope. The type of the cable is a sexual electrical conductor, and the encapsulation can limit the electricity generated around the conductor. Actually, Reduced, and the cooling device is better than the one that is missing in the past, and the insulation between the traditional and the traditional invention is another comparison, so it is possible to make another embodiment at least belong to the other limited to the insulator system The reactor produced by the electric conductor can be more efficient, which can reduce the losses and losses caused by the reactor to have a lower temperature. The structure of the coil that does not use it is simpler to install. The cable may be a flexible cable, which means a hard coil that is still used in conventional technology. In addition, in this edge body system, gas and liquid insulating material points are not used. The present invention is easier to solve in comparison with a core for a magnetic leakage core of a reactor of a common coil. In the preferred embodiment, the solid-state cable is used to form the cable. The advantage of this cable is to achieve the optimum so that two parts can be mixed with each other by making two electrical slow wires, that is, the coils of a coil that belong to the same coil, and Complete or partial advantage of another phase

第10頁 ^4 324 0 9 _案號 88104659_年月日_\±L·._ 五、發明說明(7) 份介於其間,因此對於一給定的不對稱電感而言,在對稱 時所感測的電感可更進一步減少。最好比對稱的電感可排 除由磁漏電感所形成。當在電抗器上使用傳統的絕緣技術 時,可確定不可能使得線圈彼此互相混合。 由下文中的說明可更進一步了解本發明之特徵及優 點,閱讀時並請參考附圖。 圖式之簡單說明 下文較佳實施例的說明係作為說明例子之用,並請參 考附圖。 圖1示本發明電抗器之一種可能的應用方式之示意 圖。 圖2 - 9示本發明較佳實施例中電抗器的截面視圖,且 圖1 0為一電纜線的透視圖,此電纜線尤其是適於於形 成本發明之電抗器的線圈,其中已去除電纜線的不同以說 明其結構。 圖號說明 電抗器 2 線圈 3-5 相 6-8 磁核心 9 電纜線 10 電導體 11 支腳 14 ' 15 空氣核心 1 7 較佳實施 例之詳細說明Page 10 ^ 4 324 0 9 _Case No. 88104659_Year Month and Day_ \ ± L · ._ V. Description of the invention (7) The copy is in between, so for a given asymmetrical inductance, when it is symmetrical The sensed inductance can be reduced even further. It is better to eliminate the formation of magnetic leakage inductance than the symmetrical inductor. When conventional insulation techniques are used on the reactor, it is determined that it is impossible to mix the coils with each other. The features and advantages of the present invention can be further understood from the following description. Please refer to the accompanying drawings when reading. Brief Description of the Drawings The following description of the preferred embodiments is for illustrative purposes, and please refer to the drawings. Fig. 1 shows a schematic diagram of a possible application of the reactor of the present invention. Figures 2-9 show cross-sectional views of a reactor in a preferred embodiment of the present invention, and Figure 10 is a perspective view of a cable, which is particularly suitable for forming a coil of a reactor of the present invention, in which it has been removed The cables are different to illustrate their structure. Description of drawing number Reactor 2 coil 3-5 phase 6-8 magnetic core 9 cable 10 electric conductor 11 leg 14 '15 air core 1 7 detailed description of preferred embodiment

第11頁 I 143240 9 _案號 88104659_年月日__ 五、發明說明(8) 圖1中的示意圖顯示本發明中的電抗器連接一用於供 應三相交變電壓予負載1的網路,該負載1如一交流馬達。 電抗器2包含3個線圈3 - 5,各線圈連接到交變電壓網路的 各相6 - 8中。線圈繞著鐵或鐵合金的共同磁化核心。從離 開與多相交變電壓的位置看過去,不同線圈的線圈繞線具 有相同的方向,且具有相同的圈數。此意謂著當以對稱方 式提供三相交變電壓時,在線圈中流動的電流,及共同流 過核心的磁通量之總合實際上為0,因此,在對應線圈中 的加及減序列電流將感覺到一極低之電感,甚至,實際上 對應線圈中的自感則相當高。在供應的交變電壓對稱時, 則沒有0序列電流。 在理想的關係下,在線圈3中感應的電壓U 3可視為將 考量之相的互感,其大小如對應相的自感,即 U3=L33 d(I3+14 + 15)/dt (1 ) 其中L 3 3為線圈3的自感,1 3,1 4及1 5為流過對應線圈的電 流。從(1 )式中可看出當在各相中的電流合為0時(正序列 電流及負序列電流),則在各相中感應的電壓為1 ,此係因 為對等的阻抗為0之故,且因此不論L3 3可能高到多少,對 於電路均不會有影響。不論在各相中的0序列組件如何?如 果假設L33相當高的話,則將電抗器中均會感覺到很高的 電壓降。此電壓降對應到高阻抗,且由該電流1限制外層 序列電流。此不對稱負載係由各相中有一相接地所產生之 短路所造成,在此例子中,電抗器將強烈地限制短路電流Page 11 I 143240 9 _ Case No. 88104659_ Year Month Day__ V. Description of the invention (8) The schematic diagram in Figure 1 shows that the reactor in the present invention is connected to a network for supplying a three-phase alternating voltage to the load 1 The load 1 is like an AC motor. Reactor 2 contains 3 coils 3-5, each coil being connected to each phase 6-8 of the alternating voltage network. The coils are wound around a common magnetized core of iron or an iron alloy. Looking from the position where the voltage is separated from the polyphase alternating voltage, the coil windings of different coils have the same direction and the same number of turns. This means that when a three-phase alternating voltage is provided in a symmetrical manner, the sum of the current flowing in the coil and the magnetic flux that commonly flows through the core is actually 0. Therefore, the addition and subtraction sequence currents in the corresponding coils will be I feel a very low inductance, and even the self-inductance in the corresponding coil is actually quite high. When the alternating voltage supplied is symmetrical, there is no zero sequence current. In an ideal relationship, the voltage U 3 induced in the coil 3 can be regarded as the mutual inductance of the phase to be considered, and its size is like the self-inductance of the corresponding phase, that is, U3 = L33 d (I3 + 14 + 15) / dt (1) Among them, L 3 3 is the self-inductance of coil 3, and 1 3, 1 4 and 15 are the currents flowing through the corresponding coils. It can be seen from the formula (1) that when the current in each phase is 0 (positive sequence current and negative sequence current), the voltage induced in each phase is 1, because the equivalent impedance is 0. Therefore, and no matter how high L3 3 may be, it will not affect the circuit. Whatever the 0-sequence component in each phase? If L33 is assumed to be quite high, a high voltage drop will be felt in all reactors. This voltage drop corresponds to a high impedance, and the outer sequence current is limited by this current1. This asymmetric load is caused by a short circuit caused by grounding in one of the phases. In this example, the reactor will strongly limit the short circuit current

第12頁 ' ^432409 _案號88104659_年月曰 修正_ 五、發明說明(9) 的大小,且係護馬達,電力網路,發電機,變壓器及其他 任何的電力設備。Page 12 '^ 432409 _ Case No. 88104659_ Year Month Amendment _ V. The size of the description of invention (9) and protects motors, power networks, generators, transformers and any other electrical equipment.

圖2中顯示本發明第一較佳實施例中的電抗器之架構 方式。而且此電抗器及此將於下文中加以說明係用於連接 三相交變電壓,且各相均包含一線圈,但是,如上文中所 說明者,本發明並不完全受到連接說明的限制。各線圈均 繞者磁核心9,該線圈為壞狀方式^在此由電缓線丨0形成 線圈3-5,該電纜線之方式為具有的電導體11,且具有包 封體或外鞘結構,係用於限制繞著導體的電場。此將於下 文中加以說明此電纜線的結構。在線圈的例子中均使用此 電纜線的優點為各相中較易絕緣D 當交變電壓對稱時,在核心9中產生的磁通量實際上 為0,此係因為不同相之間的電流將互相抵銷,且電抗器 中的漏電感相當的低,此也使得空氣的磁漏通量相當低。 因此,所有線圈中均感應的通量,在對稱的關係下,實際 上為0,且各相中實際上只感應到本身的磁漏通量,且當 不對稱時,線圈均感應到通過核心的通量= 依據圖3 所示之本發明實施例,不同線圈之間交互混 合,其方式為屬於相同線圈的繞線具有屬另一線圈的繞 線,且另一相完全或部份配置在其間。因此,有可能減少 磁漏通量,且相同電抗器的磁漏電感。之所以可具有此緊 密相鄰的繞線方式,係因為使用具有上述定義之特性的電 纜線,即其包封繞著該導體產生的電場。 圖4中所示本發明另一較佳實施例之電抗器,其中磁 化核心9包圍該線圈。此類型的電抗器通過稱為爐架型電Fig. 2 shows the structure of the reactor in the first preferred embodiment of the present invention. Moreover, this reactor and this will be described below are used to connect three-phase alternating voltage, and each phase includes a coil, but, as described above, the present invention is not completely limited by the connection description. Each coil is wound around a magnetic core 9. This coil is in a bad shape. ^ Here, coils 3-5 are formed by electrical slow wires 丨 0. The cable is in the form of an electric conductor 11 and has an encapsulation body or an outer sheath. Structures are used to limit the electric field around a conductor. The structure of this cable will be explained later. The advantage of using this cable in the example of the coil is that it is easier to insulate in each phase. D When the alternating voltage is symmetrical, the magnetic flux generated in core 9 is actually 0, because the currents between different phases will mutually Offset, and the leakage inductance in the reactor is quite low, which also makes the magnetic leakage flux of air quite low. Therefore, the flux induced in all coils is actually 0 in a symmetrical relationship, and only the magnetic flux of the magnetic flux is actually induced in each phase. When the flux is not symmetrical, the coils are induced to pass through the core. Flux = According to the embodiment of the present invention shown in FIG. 3, different coils are mixed with each other in a manner that the windings belonging to the same coil have windings belonging to another coil, and the other phase is completely or partially arranged in In the meantime. Therefore, it is possible to reduce the magnetic leakage flux and the magnetic leakage inductance of the same reactor. The reason why this close-wound winding is possible is because the cable with the characteristics defined above is used, that is, it encloses the electric field generated around the conductor. A reactor according to another preferred embodiment of the present invention is shown in Fig. 4, in which a magnet core 9 surrounds the coil. This type of reactor is

第13頁 Γ *432409 _案號 88104659_年月日__ 五、發明說明(10) 抗器°其核心形如一環形,即如一連續的環管一般,且電 抗器大致上對應繞著軸13的轉動形成對稱。實際上線圈不 完全形成轉動對稱,而是呈螺旋形° 圊5中顯示本發明中各線圈均具有共同核心9的電抗 器,其中該核心呈傳統的矩形型式,而線圈係韌性核心的 兩支腳1 4,1 5。在此例子中,空氣間隙係配置在核心t , 此有可能使得0序列電感線性化,此通過為使用者所必需 的性能。但是,此意謂著電抗器的限電流將會下降,此係 因為外層序列電感減少之故。 圖2示圖4實施例之修改形成,其中沒有空氣間隙,且 線圈互相混合以減少磁漏通量。 本發明另一較佳實施例的電抗器顯示於圖7中,此電 抗器即所謂的空氣電抗器,即具有空氣核心1 7。重要的 是,在此電抗器中,屬於不同相的空氣電抗器的線圈間形 成緊密配置,此係因為線圈將無法感應到實際上相同的磁 通量ΰ但是空氣電抗器的缺點為不可能得到相當高的電 感,且不對稱時,得到相當高的限電流效應。但是空氣電 抗器較便宜,係因為不採用鐵核心之故,且有可能設計其 尺寸,使在不對稱的關係下,具有較大的磁場,如5 Τ,而 非如具有鐵核心之電抗器的2Τ,使得所有結構可加以壓 縮。電抗器主要繞著軸1 3形成轉動對稱,雖然並非完全對 稱,係因為線圈為螺旋形之故。 圖8中顯示本發明電抗器的另一實施例,其中線圈係 繞著具有三支腳的傳統式核心的内腳。通過此電抗器稱為 ’殼形”電抗器。在此例子中,共同的通量在中間腳中導Page 13 Γ * 432409 _Case No. 88104659_Year Month and Day__ V. Description of the invention (10) The core is shaped like a ring, that is, like a continuous loop, and the reactor roughly corresponds to the axis. The rotation of 13 forms a symmetry. In fact, the coil does not completely form a rotational symmetry, but it has a spiral shape. 圊 5 shows that each coil in the present invention has a reactor with a common core 9, wherein the core is a traditional rectangular type, and the coil is a two-core flexible core. Feet 1, 4, 15. In this example, the air gap is configured at the core t, which may linearize the zero-sequence inductance, which is the performance required by the user. However, this means that the current limit of the reactor will decrease, which is because the inductance of the outer layer is reduced. Fig. 2 shows a modified form of the embodiment of Fig. 4, wherein there is no air gap, and the coils are mixed with each other to reduce magnetic leakage flux. A reactor according to another preferred embodiment of the present invention is shown in FIG. 7. This reactor is a so-called air reactor, which has an air core 17. It is important that in this reactor, the coils of air reactors belonging to different phases form a tight arrangement. This is because the coils will not be able to sense the same magnetic flux. However, the disadvantage of air reactors is that it is impossible to obtain a relatively high level. When the inductance is asymmetric, a fairly high current-limiting effect is obtained. However, air reactors are cheaper because they do not use iron cores, and it is possible to design their dimensions so that they have a larger magnetic field, such as 5T, instead of a core with iron cores in an asymmetric relationship. 2T, so that all structures can be compressed. The reactor mainly forms a rotational symmetry around the axis 13, although it is not completely symmetrical because the coil is spiral. Fig. 8 shows another embodiment of the reactor of the present invention, in which the coil is wound around the inner leg of a conventional core having three legs. This reactor is called a 'shell-shaped' reactor. In this example, the common flux is conducted in the middle leg

4 32 4 0 9 案號88104659 年月日 修正4 32 4 0 9 Case No. 88104659 Revised

第15頁 广膠4 32 4 Ο 9 _案號 88104659_年月日__ 五、發明說明(12) 例如油型式者。絕緣可由# P材料形成。而且,由聚合物材 料形成内及外層,即使是半導體者也一樣。絕緣體1 8可由 熱塑形材料製造,如低密度聚乙稀(polyethylene, LDPE),高密度聚乙烤(polyethylene,HDPE),聚丙婦 (polypropylene ,PP),聚丁歸(polybuthylene ,PB), polymethyepenten (PMP),交聯聚乙稀(polyethylene , XLPE),或者是橡勝,如乙烯丙烤(ethylene-propylene) 橡膠或矽橡膠。内層及外層的電阻率應在10-6 Ω cm到100k Qcm的範圍之内,最好是10-3 -1000Ω(:ιη,1-500Ωιη更 好。最好内層及外層的電阻,其導體/絕緣體系統之每公 尺長度範圍介於5 0 " Ώ到5 Μ Ω之間。 由於繞著絕緣體之半導體材料的内層及外層傾向於形 成大致上為等電位之表面’且在絕緣體中的電場依此方式 在整個絕緣體的厚度方向上的分配相當均勻,所以在絕緣 體系統上的電負載或應力將會降低。 絕緣材料及内及外半導體層之間的附著性在整個表面 上大致上相當均勻,使得沒有任何空缺,空洞等。此當然 在高壓應用中尤其重要,且此類型的電纜線最好為適於高 壓的絕緣系統’可適應超過1 〇 Κ V的電壓,尤其是高於3 6 Κ V 的電壓’且最好可大於72.5KV。在此高電壓處發生的電及 熱應力使得對絕緣材料產生高度的需要。須了解一般所謂 的部份放電PD在高電壓的應用中,對於絕緣材料是一項相 當重要的問題。當在絕緣層中形成中空之空間,孔洞等 時’則在可能在高電壓下發生内部電量放電,在此絕緣材 料’逐漸降級’且導致通過絕緣體的電性崩潰。此將使得Page 15 Guangjiao 4 32 4 Ο 9 _ Case No. 88104659_year month__ V. Description of the invention (12) For example, oil type. The insulation may be formed from a #P material. Moreover, the inner and outer layers are formed of a polymer material, even for semiconductors. The insulator 18 can be made of thermoplastic materials, such as low-density polyethylene (LDPE), high-density polyethylene (HDPE), polypropylene (PP), polybuthylene (PB), polymethyepenten (PMP), cross-linked polyethylene (XLPE), or rubber victory, such as ethylene-propylene rubber or silicone rubber. The resistivity of the inner and outer layers should be in the range of 10-6 Ω cm to 100k Qcm, preferably 10-3 -1000Ω (: ιη, 1-500 Ωιη is better. The resistance of the inner and outer layers, the conductor / The length of each insulator system ranges from 50 to Ώ 5 to 5 megaohms. Because the inner and outer layers of the semiconductor material surrounding the insulator tend to form a surface of approximately equal potential 'and the electric field in the insulator In this way, the distribution in the thickness direction of the entire insulator is quite uniform, so the electrical load or stress on the insulator system will be reduced. The adhesion between the insulating material and the inner and outer semiconductor layers is substantially uniform over the entire surface So that there are no vacancies, cavities, etc. This is of course especially important in high-voltage applications, and this type of cable is best an insulation system suitable for high-voltage 'can adapt to voltages greater than 100K V, especially higher than 3 6 The voltage of KV is preferably greater than 72.5KV. The electrical and thermal stresses that occur at this high voltage place a high demand on the insulating material. It is important to understand that the so-called partial discharge PD at high voltages In the application, it is a very important issue for insulating materials. When hollow spaces, holes, etc. are formed in the insulating layer, 'the internal electrical discharge may occur at high voltages, where the insulating material is' gradually degraded' and Cause electrical breakdown through the insulator. This will make

第16頁 ^ 4 32 4 U y _案號 88i04659_ 年月曰_i±L·._ 五、發明說明(13) 電抗器故障。 最好,内層、外層及固態絕緣體具有大致上相同的熱 性質,以避免產生空洞或細孔,當這些組件具有大致上相 同的熱膨脹係數時,此性能尤其重要,因此可在溫度改變 期間維持不同層之間的完全附著,而且當溫度改變時,電 纜線可均勻膨脹及收縮如單石體一般,而不會破壞或惡化 其介面。該絕緣層例如可為交聯之低密度的聚乙稀及含灰 塵或材料粒之聚乙稀之半導體層。由於溫度改變所產生的 體積型式可完全為電纜線半徑的改變,及層之熱膨脹係數 對應這些材料之彈性的相當小的差異所吸收,可由電纜線 半徑膨脹替代各層間互相間的鬆弛。 電纜線也具有某些韌性,且其韌性降到曲率半徑的倍 數,低於2 5 X電纜線的直徑,使得可能產生彎曲*但是可 確定在對應層及固態絕緣體之間可得到相當良好的附著 性。電纜線對於低於1 0 X電纜線直徑的曲率半徑具有適當 的韌性,最好是曲率半徑在5 X電纜線的直徑以下。在絕 緣系統中不同層的E模數應大致上相等,因此在不同層的 介面之間不會導致任何不必需的剪應力,因此可減少剪應 力,此應用係當電纜線受到相當彎曲時,導致在彎曲處之 外側上的張力且在彎曲處内側的壓縮應力時,在不同層之 間所產生者。 雖然文中已應較佳實施例說明本發明,但嫺熟本技術 者需了解可對上述實施例加以更改及變更,而不偏離本發 明的精神及觀點,其中本發明的基本構想係定義在所附的 申請專利範圍中。Page 16 ^ 4 32 4 U y _Case No. 88i04659_ Year and month _i ± L · ._ V. Description of the invention (13) Reactor failure. Preferably, the inner, outer, and solid insulators have approximately the same thermal properties to avoid voids or pores. This performance is especially important when these components have approximately the same coefficient of thermal expansion, so they can be maintained differently during temperature changes Complete adhesion between the layers, and when the temperature changes, the cable can expand and contract uniformly like a monolith without breaking or deteriorating its interface. The insulating layer may be, for example, a cross-linked low-density polyethylene and a polyethylene layer containing dust or material particles. Due to the change in temperature, the volume type can be completely absorbed by the change of the cable radius, and the relatively small difference in the coefficient of thermal expansion of the layers corresponding to the elasticity of these materials can be replaced by the expansion of the cable radius to replace the relaxation between the layers. The cable also has some toughness, and its toughness is reduced to a multiple of the radius of curvature, which is lower than the diameter of the 2 5 X cable, making it possible to bend * but it can be determined that a fairly good adhesion can be obtained between the corresponding layer and the solid insulator Sex. The cable has appropriate toughness for a radius of curvature of less than 10 X diameter of the cable, preferably the radius of curvature is below 5 X of the diameter of the cable. The E-modulus of different layers in the insulation system should be approximately equal, so no unnecessary shear stress will be caused between the interfaces of different layers, so the shear stress can be reduced. This application is when the cable is subjected to considerable bending, Produced between different layers when it causes tension on the outside of the bend and compressive stress on the inside of the bend. Although the present invention should be explained in terms of preferred embodiments, those skilled in the art need to understand that the above embodiments can be modified and changed without departing from the spirit and perspective of the present invention, in which the basic concept of the present invention is defined in the appended Within the scope of patent applications.

第17頁 r 顯432 4 Ο 9 _案號 88104659_年月曰__ 五、發明說明(14) 線圏的繞線方式可不為附圖中所顯示者,應用實際上 相同的磁通量時,仍可得到相當的效果,其t在某些例子 中,繞線的配置方式可更進一步分離,因此可得到所需要 的磁漏通量。 如上文中所說明者’磁性材料也包圍遠線圈D在二相 包圍一磁管的例子中對等於每線圏具有一繞線的例子。如 果具有更多的繞線,則這些繞線可在外部包圍該管子。如 果管子封閉如一圓圈,則這些繞線可完全包圍在管子内 側。後述之例子對等於如上文中所說明的外罩型電抗器。 磁性材料並非包圍該線圈”全部繞線M。在通常稱為π殼型π 的磁性材料中,該材料係在只霞蓋線圈周圍一小部份的兩 個磁返導體中,係封閉在線圈的外側。管子並非需為單 件。可由多件安裝在一起,但是也可以由繞著一磁帶或繞 著該相的線所形成。管子之透視圖可為任意圓型,矩形 等。也可以使用不同電抗器核心之空氣間隙的結合。在本 發明之理想覲念中,對於本發明之電抗器架構可進行多項 可能的變更,這些變更均在本發明的範圍之内°Page 17 r 432 4 Ο 9 _case number 88104659_year month __ V. Description of the invention (14) The winding method of the coil may not be the one shown in the drawing. When the same magnetic flux is applied, it is still A considerable effect can be obtained. In some examples, the arrangement of the windings can be further separated, so the required magnetic leakage flux can be obtained. As explained above, the magnetic material also surrounds the far coil D. In the case where the two phases surround a magnetic tube, there is an example in which there is one winding per wire. If there are more windings, these windings can surround the tube externally. If the tube is closed like a circle, these windings can completely surround the inside of the tube. The example described later is equivalent to a cover-type reactor as described above. The magnetic material does not surround the coil "is all wound M. In the magnetic material commonly called π shell type π, the material is enclosed in a small portion of two magnetic return conductors around the Xia Gai coil, and is enclosed in the coil The tube does not need to be a single piece. It can be installed in multiple pieces, but it can also be formed by a tape or a line around the phase. The perspective view of the tube can be any round shape, rectangular shape, etc. It can also be The combination of air gaps using different reactor cores. In the ideal idea of the present invention, a number of possible changes can be made to the reactor architecture of the present invention, and these changes are all within the scope of the present invention.

第18頁Page 18

Claims (1)

(醞4 32#§P逄丨〇4659 是9.¾2 2曰 修正_ 六、申請專利範圍 1,一種包含多個線圏(3_5)的電抗器,各線圈適於連 接多相交變電壓中的單相(6>8),配置該線圈使得當連接 到該電壓時’這些線圈受到相同磁通量的影響,其特徵為 該線圈(3-5)中至少一線圈中至少有一部份由一電纜線(1〇 )所形成’該電纜線之形式為具有包封(12)的韌性電導體 (1Π ’該包封(12)係用於限制繞著該導體所產生的電場。 2. 如申請專利範圍第1項之電抗器,其中相的數 目’錄圈(3 - 5 )的數目’線圈的繞線方向及每個線圈的圈 數使得當供應多相交變電壓下,線圈為對稱時,則流過該 線圈驅動共同磁通量的電流之加總實際上為〇 ^ 3. 如申請專利範圍第1項之電抗器其中該數目或相 數為3。 4·如申請專利範圍第1項之電抗器,其中配置屬於不 同相之線圈’使得彼此互相靠近。 5.如申請專利範圍第1項之電抗器,其中不同線圈 (3-5)的線圈繞線具有相同的方向,如同從連結位置向多 相交變電麼的方向中所視者。 6*如申請專利範圍第1項之電抗器,其中各線圈係繞 著共通封閉磁路(9,16)。 7,如申請專利範圍第1項之電抗器,其中包含共通之 封閉磁路’且包圍該線圏。 8_如申請專利範圍第&淨之電抗器,其中磁路(9,16) 包含一或多種材料,這些材料可能具有不同的磁性能,且 可以任意數目加以連接β(Creating 4 32 # §P 逄 丨 〇4659 is 9.¾2 2 is the amendment _ 6. Application for patent scope 1, a reactor containing multiple wires (3_5), each coil is suitable for connection in the multi-phase alternating voltage Single-phase (6> 8), the coil is configured so that when connected to the voltage 'these coils are affected by the same magnetic flux, characterized in that at least a part of at least one of the coils (3-5) consists of a cable (10) Formed 'The cable is in the form of a tough electrical conductor with an envelope (12) (1Π' The envelope (12) is used to limit the electric field generated around the conductor. 2. If a patent is applied for The reactor of item 1 of the range, in which the number of phases 'the number of recording loops (3-5)' and the winding direction of the coil and the number of turns of each coil are such that when the coil is symmetrical under the supply of a multi-phase alternating voltage, then The sum of the currents flowing through the coil to drive the common magnetic flux is actually 0. 3. For the reactor in the first scope of the patent application, the number or phase number is 3. 4. The reactor in the first scope of the patent application , In which coils belonging to different phases are arranged so that they are close to each other. The reactor of item 1 of the scope of patent application, in which the coil windings of different coils (3-5) have the same direction, as viewed from the connection position to the direction of the multi-phase alternating current. The reactor of item 1, wherein each coil is wound around a common closed magnetic circuit (9, 16). 7. The reactor of item 1 in the scope of patent application, which includes a common closed magnetic circuit 'and surrounds the coil. 8_If the scope of the patent application & net reactor, the magnetic circuit (9,16) contains one or more materials, these materials may have different magnetic properties, and can be connected in any number β !號 88104659 六、申請專利範圍! No. 88104659 6. Scope of patent application 9,如申請專利範圍第6項之電抗器 16)中至少一種材料為鐵或鐵合金。 10.如申請專利範圍第6項之電抗器 含整個鐵或鐵合金。 其中在磁路(9, 其t磁路(9)包 i 1.如申請專利範圍第6項之電抗器 中至少一種材料(9,16)為非磁性者。 12·如申請專利範圍第u項之電抗器 料(9, 16)中至少一項為空氣。 13.如申請專利範ι圍第12項之電抗器 完全包含空氣。 ™ 其t在磁路(1 6 ) 1其中非磁性材 ,其中磁路(1 7) 1 4·如申請專利範圍第6項之電抗器 少一空氣間隙(U) D 15-如申請專利範圍第6項之電抗器 16)包圍一圓形區域。 16. 如申請專利範圍第6項之電抗器 16)包圍一矩形區域。 17. 如申請專利範圍第6項之電抗器 16)包圍一三角形區域。 中清專利範圍第6項之電抗器 均只連接具有-繞線的線圈(3-5)。 形虚2、如:請專利範圍第1 8項之電抗器穴1 39 ’其比繞著該電抗器的區域還要寬 5 ) $这如宜申 '專利範圍第6項之電抗器,其中該線圈(3 ’ ^ 該磁路(9,16)的線圈繞線包圍其全部或部 其中磁路具有至 其令該磁路(9, 其中該磁路(9, 其中該磁路(9, 其中各相(9, 其中該繞線可9. The reactor according to item 6 of the patent application 16) At least one of the materials is iron or an iron alloy. 10. The reactor according to item 6 of the patent application contains the entire iron or iron alloy. Among them, the magnetic circuit (9, t magnetic circuit (9) includes i. 1. At least one material (9, 16) in the reactor of item 6 of the patent application is non-magnetic. 12 · As of patent application range u At least one of the reactor materials of item (9, 16) is air. 13. For example, the reactor of item 12 in the patent application range completely includes air. ™ t is in the magnetic circuit (1 6) 1 of which is a non-magnetic material Among them, the magnetic circuit (1 7) 1 4 · If the reactor in the scope of patent application No. 6 has one less air gap (U) D 15-like the reactor in scope of patent application No. 6) surrounds a circular area. 16. The reactor as in item 6 of the patent application 16) encloses a rectangular area. 17. The reactor as claimed in item 6 of the patent application 16) surrounds a triangular area. The reactors in item 6 of Zhongqing's patent range are only connected with -winding coils (3-5). Virtual form 2. For example, please ask for the reactor hole 1 39 of the patent scope item 18 which is wider than the area around the reactor 5) $ This Ruyi Shen's reactor scope of the patent scope item 6, where The coil of the coil (3 '^ the coil of the magnetic circuit (9, 16) surrounds all or part thereof, wherein the magnetic circuit has the magnetic circuit (9, where the magnetic circuit (9, where the magnetic circuit (9, Wherein each phase (9, where the winding can 第20頁 觼4 32 4 Ο p ---案號拈104R59 六、申請專利範圍 " ---— 份。 21. 如申請專利範圍第6項之 包圍通過該線圈繞線之磁 Λ ’其中線圈(3,5) 22. 如申請專利範圍二之1電6)抗, )包圍整個線圈或其部份。 ^ 35 其中磁路(9, 16 其中磁路(9,16 其中各線圈均配 其中所有的線圈 23如中請專利範圍第6項之電抗器, )匕圍線圈的一部份或數部份。 24. 如申請專利範圍第!項之電抗器, 置在非磁性材料的載體中。 25. 如申請專利範圍第i項之電抗器, 均由該電纜線所形成。 2 6.如申請專利範圍第24項之電抗器,其 圈(3-5)至少部份相混,即屬於相同線蘭 : " 「碉介、相丨』踝圏的繞線具有屬於 另一線圈之線圈繞線,且另一相完全或部份介於其間。 27. 如申請專利範圍第24項之電抗器,其中該包封包 含絕緣體系統,其中絕緣體系統包含由一固態絕緣材料 所开> 成的絕緣體(18)及其外側包含一外層(19),此外層的 導電率高於絕緣體的導電率,因此外層可接地,或者是對 應一低電壓,一方面,可等化電壓’且另一方面大致上包 圍由該外層之電導體(11)向内所產生的電場。 28, 如申請專利範圍第24項之電抗器,其中該包封包 含一絕緣系統,此系統具有—由‘固態絕緣材料所形成的絕 緣體(18)及一在其内部的内層(20),該至少一電導體(11) 係配置在該内層的内部,且該内層具有一電導體,此電導Page 20 觼 4 32 4 Ο p --- Case No. 拈 104R59 6. Scope of Patent Application " ----- copies. 21. If the magnetic field around the coil is covered by item 6 of the scope of the patent application, Λ ′ among which the coil (3, 5) 22. If the scope of the patent application is 2 to 6) reactance,) surrounds the entire coil or part thereof. ^ 35 where the magnetic circuit (9, 16 where the magnetic circuit (9, 16 where each coil is equipped with all the coils 23 such as the reactor in the patent claim 6), part or several of the coil 24. If the reactor under the scope of the patent application is applied, it is placed in a carrier of non-magnetic material. 25. If the reactor under the scope of the patent application, i is formed by the cable. 2 6. If the patent is applied for In the reactor of the 24th item, the coils (3-5) are at least partially mixed, that is, they belong to the same line orchid: " "碉 介 、 相 丨" ankle coil winding has a coil winding belonging to another coil And the other phase is completely or partially in between. 27. For example, the reactor of the scope of application for patent No. 24, wherein the encapsulation includes an insulator system, wherein the insulator system comprises an insulator made of a solid insulating material > (18) and its outer side includes an outer layer (19). The conductivity of the outer layer is higher than the conductivity of the insulator, so the outer layer can be grounded or correspond to a low voltage. On the one hand, it can equalize the voltage 'and on the other hand it is roughly The upper envelope is directed by the outer electrical conductor (11) The electric field generated. 28. The reactor according to item 24 of the patent application, wherein the envelope includes an insulation system having an insulator (18) formed of a 'solid insulating material and an inner layer inside it (20), the at least one electric conductor (11) is arranged inside the inner layer, and the inner layer has an electric conductor, and the electric conductivity 第21頁 a _修正 -__ 六、申請專利範圍 體的導電率低於足以使内層操作等化電位的導電率,且由 此’以等於内層外側的電場。 2 9.如申請專利範圍第27項之電抗器,其♦内層及外 層及該固態絕緣體具有大致上相等的熱性質。 30·如申請專利範圍第27項之電抗器I其中内層及/或 外層(19,20)包含一半導體材料。 31. 如申請專利範圍第27項之電抗器,其中内層及/或 外唐(19 ’2D)的電阻率介於1〇-6Ωιη-ΐ〇〇κΩ(:ιη之間,適當 的範圍為103-l〇〇〇〇cm,較佳是卜5〇〇.Ωιπ。 32. 如申請專利範圍第27項之電抗器,其中内層及/或 外層(19,20)有一電阻,此電阻在每米的導體/絕緣體系 統申為50 // Ω-5Μ Ω之間。 33. 如申請專利範圍第27項之電抗器,其令固態絕緣 體(18)及内層(20)及/或外層(19)由聚合材料所形成。 34. 如申請專利範圍第27項之電抗器,其中内層(20) 及/或外層(19)及固態絕緣體(18)大致上在整個表面上呈 剛性連結’以確定在韌性及溫度變化時,仍能具有相當良 好的附著性。 3 5·如申請專利範圍第27項之電抗器,其中由高彈性 材料形成該固態絕緣體(18)、内層(20)及/或外層(19) » 36. 如申請專利範圍第35項之電抗器,其中固態絕緣 體(18),内層(20)及/或外層<1'9)的材料大致上具有相等 的Ε模數。 37. 如申請專利範圍第27項之電抗器,其中由具有大Page 21 a _Amendment -__ VI. Scope of Patent Application The conductivity of the body is lower than the conductivity enough to equalize the inner layer operation, and therefore ′ is equal to the electric field outside the inner layer. 29. The reactor of the 27th in the scope of patent application, the inner and outer layers and the solid insulator have approximately equal thermal properties. 30. The reactor I according to item 27 of the patent application, wherein the inner layer and / or the outer layer (19, 20) contains a semiconductor material. 31. If the reactor of the 27th scope of the patent application, the resistivity of the inner layer and / or the outer Tang (19 '2D) is between 10-6Ωι-ΐ〇〇κΩ (: ιη, the appropriate range is 103 -100cm, preferably 50. Ωιπ. 32. For example, the reactor in the 27th scope of the patent application, wherein the inner layer and / or outer layer (19,20) has a resistance, this resistance is per meter The conductor / insulator system is between 50 // Ω-5M Ω. 33. If the reactor under the scope of patent application No. 27, the solid insulator (18) and the inner layer (20) and / or outer layer (19) 34. The reactor according to item 27 of the patent application, wherein the inner layer (20) and / or the outer layer (19) and the solid insulator (18) are rigidly connected substantially over the entire surface to determine the toughness It can still have fairly good adhesion when temperature changes. 3 5 · For example, the reactor under the scope of patent application No. 27, wherein the solid insulator (18), inner layer (20) and / or outer layer ( 19) »36. If the reactor of the scope of patent application No. 35, the solid insulator (18), the inner layer 20) and / or outer layer < 1'9) of a material having a substantially equal Ε modulus. 37. For the reactor in the scope of patent application No. 27, wherein 第22頁 ^B4 3 2 88104659_年月日 修正 __ 六、申請專利範圍 致上相等之熱膨脹係數的材料形成該内層(20),及/或外 層(19)及固態材料(18)。 38.如申請專利範圍第27項之電抗器,其中内層(20) 與至少一電導體(11)形成電接觸。 3 9 ·如申請專利範圍第3 8項之電抗器,其中該至少一 電導體(11)包含多條燃線,電導體中至少一燃線其至少有 一部份並未絕緣,且配置上與内層(20)形成電接觸β 40. 如申請專利範圍第27項之電抗器,其中設計導體 及其絕缘系統可承受高電壓,適於大於10KV的電塵,尤其 是大於36KV,較佳可承受大於72.5KV的電壓。 41. 如申請專利範圍第1項之電抗器,其中,該電抗器 適於經線圈連接到高電壓,適於高過10KV,尤其是高過36 κν ’較佳高過72. 5KV。Page 22 ^ B4 3 2 88104659_Year Month Day Amendment __ VI. Scope of Patent Application Materials with equal thermal expansion coefficients form the inner layer (20), and / or the outer layer (19) and solid material (18). 38. The reactor of claim 27, wherein the inner layer (20) makes electrical contact with at least one electrical conductor (11). 3 9 · If the reactor of the 38th scope of the patent application, the at least one electric conductor (11) contains a plurality of live wires, at least a part of the at least one of the electric conductors is not insulated, and is configured to be in line with The inner layer (20) forms electrical contact β 40. For example, the reactor in the 27th scope of the patent application, where the design conductor and its insulation system can withstand high voltage, suitable for electric dust greater than 10KV, especially greater than 36KV, preferably withstand Voltage greater than 72.5KV. 5KV。 41. As claimed in the scope of the patent application of the reactor, wherein the reactor is suitable for connecting to high voltage through the coil, suitable for higher than 10KV, especially higher than 36 κν ′ preferably higher than 72. 5KV. 第23頁Page 23
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI396211B (en) * 2007-12-11 2013-05-11 Hitachi Comp Peripherals Co Composite reactor and power supply device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI396211B (en) * 2007-12-11 2013-05-11 Hitachi Comp Peripherals Co Composite reactor and power supply device

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