JPH03285180A - Light ct for complex conductors - Google Patents
Light ct for complex conductorsInfo
- Publication number
- JPH03285180A JPH03285180A JP2086868A JP8686890A JPH03285180A JP H03285180 A JPH03285180 A JP H03285180A JP 2086868 A JP2086868 A JP 2086868A JP 8686890 A JP8686890 A JP 8686890A JP H03285180 A JPH03285180 A JP H03285180A
- Authority
- JP
- Japan
- Prior art keywords
- case
- conductor
- conductors
- coils
- series
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 239000004020 conductor Substances 0.000 title claims abstract description 67
- 230000003287 optical effect Effects 0.000 claims description 12
- 238000001514 detection method Methods 0.000 abstract description 3
- 238000010586 diagram Methods 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 230000005540 biological transmission Effects 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 238000009434 installation Methods 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000017525 heat dissipation Effects 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 239000013307 optical fiber Substances 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
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- Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は変電所や送電線等の複導体母線に流れる大電流
を精度よく検出することができる複導体用光CTに関す
るものである。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an optical CT for double conductors that can accurately detect large currents flowing in double conductor buses such as substations and power transmission lines.
(従来の技術)
一般に変電所や送電線で使用される母線は送電電流が多
くなってくると単導体よりも複導体が使用される割合が
多くなり、2〜8本の導体が使用される場合がある。(Conventional technology) Generally, as the transmission current increases, busbars used in substations and power transmission lines use more double conductors than single conductors, and 2 to 8 conductors are used. There are cases.
このような複導体母線に流れる数百A〜数+KAO大電
流を検出する従来法としては、■?I導体を1本に絞り
、大型巻線鉄心を持つCTに貫通し全電流を計測する方
法、■複導体のうちの1導体の電流を同様のCTにより
計測する方法が知られている。Conventional methods for detecting large currents ranging from several hundred amperes to several +KAO flowing through such multi-conductor busbars include ■? Two methods are known: one in which the number of I conductors is reduced to one, the I conductor is passed through a CT having a large winding core, and the total current is measured; and (2) the current in one conductor of a multiple conductor is measured by a similar CT.
ところがこれらの方法はいずれも大型のCTを使用する
ためにそれを支持する大型の碍管をCTの下部に設置し
なければならず、十分な用地が確保できる場所にしか取
付けられないという問題があった。また■の方法は既設
の導体を一旦切断したうえで−導体化してCTを入れ込
む必要があり、施工期間が長く経済的にも問題があった
。更に■の方法は測定誤差が大きく、またCTが取付け
られていない他の導体で事故が起こっても検出できない
等の問題があった。However, all of these methods have the problem that in order to use a large CT, a large insulator tube must be installed below the CT to support it, and it can only be installed in locations where sufficient land can be secured. Ta. In addition, method (2) requires that the existing conductor be cut once and then converted into a negative conductor before the CT is inserted, resulting in a long construction period and an economical problem. Furthermore, method (2) has problems such as large measurement errors and failure to detect even if an accident occurs on another conductor to which the CT is not attached.
(発明が解決しようとする課a)
本発明は上記したような従来の問題点を解決して、狭い
場所にも取付けが可能であり、また既設の導体を切断す
ることなく容易に取付けができ、しかも全導体を流れる
電流を精度よく検出することができる複導体用光CTを
提供するために完成されたものである。(Problem to be solved by the invention a) The present invention solves the above-mentioned conventional problems, and can be installed even in narrow spaces, and can be easily installed without cutting existing conductors. Moreover, it was completed in order to provide an optical CT for double conductors that can accurately detect the current flowing through all the conductors.
(課題を解決するための手段)
上記の課題を解決するためになされた第1の発明は、複
数本の各導体のまわりに導体クランプを備えた開閉式の
ケースを設け、各ケースの内部に往路、復路ともにその
ヒンジ部を通過するように巻き戻した一連のトロイダル
コイルを取り付けるとともに、その二次側のソレノイド
に全電流に比例した磁界を検出するファラディ素子を取
り付けたことを特徴とするものである。(Means for Solving the Problem) A first invention made to solve the above problem is to provide an openable case equipped with a conductor clamp around each of a plurality of conductors, and to A series of unwound toroidal coils are attached so as to pass through the hinge portion on both the outward and return trips, and a Faraday element that detects a magnetic field proportional to the total current is attached to the solenoid on the secondary side. It is.
また同一の課題を解決するためになされた第2の発明は
、複数本の各導体のまわりに導体クランプを備えた開閉
式のケースを設け、各ケースの内部に往路、復路ともに
そのヒンジ部を通過するように巻き戻した一連のトロイ
ダルコイルを取り付けるとともに、その二次側に負担抵
抗とその両端の発生電圧を検出するポッケルス素子とを
取り付けたことを特徴とするものである。A second invention made to solve the same problem is to provide a retractable case equipped with a conductor clamp around each of the plurality of conductors, and to install the hinge portion inside each case for both the outward and return paths. It is characterized by a series of toroidal coils that are unwound so as to pass through the coil, and a burden resistor and a Pockels element that detects the voltage generated at both ends of the coil are attached to the secondary side of the coil.
(実施例)
以下にこれらの発明を図示の実施例によって詳細に説明
する。(Examples) These inventions will be described in detail below using illustrated examples.
第1図および第2図は第1の発明の複導体用光CTを2
導体母線に取り付けた実施例を示すもので、(1)は2
本の導体、(2)は各導体(1)のまわりに取付けられ
た開閉式のケースである。このケース(2)は例えばア
ルミニウムのような金属からなる気密構造のもので、ヒ
ンジ部(3)を中心として開閉し導体(1)のまわりに
閉じることができる構造となっている。ケース(2)の
内部にはケース(2)の先端に達する一連のトロイダル
コイル(4)が設けられている。Figures 1 and 2 show two optical CT for double conductor according to the first invention.
This shows an example in which it is attached to a conductor bus bar, and (1) is 2
The book conductor (2) is a retractable case attached around each conductor (1). This case (2) has an airtight structure made of metal such as aluminum, and has a structure that can be opened and closed around a hinge part (3) and can be closed around the conductor (1). Inside the case (2) there is a series of toroidal coils (4) that reach the tip of the case (2).
このトロイダルコイル(4)はケース(2)の各半部毎
に往路、復路ともヒンジ部(3)を通過するように巻き
戻されたものであり、ヒンジ部(3)を中心としてケー
ス(2)を自由に開閉することができ、しかもケース(
2)を導体(1)のまわりに閉じたときに導体(1)の
ほぼ全周を囲むトロイダル状となるように構成されてい
る。なお第3図の回路図に示すように、各導体(1)の
トロイダルコイル(4)は直列に結合されている。This toroidal coil (4) is unwound in each half of the case (2) so as to pass through the hinge part (3) on both the outward and return journeys, and the toroidal coil (4) is wound around the hinge part (3) in the case (2). ) can be opened and closed freely, and the case (
2) is constructed so that when it is closed around the conductor (1), it becomes a toroidal shape that surrounds almost the entire circumference of the conductor (1). As shown in the circuit diagram of FIG. 3, the toroidal coils (4) of each conductor (1) are coupled in series.
またケース(2)はその片側に熱伝導性の悪い材料から
なる導体クランプ(5)を備えている。この導体クラン
プ(5)はケース(2)を閉じたときに導体(1)をク
ランプすることにより、導体(1)を正確にトロイダル
コイル(4)の中心に位置させ、出力の変動を防止する
ためのものである。更に各ケース(2)は導体クランプ
(5)の外側に放熱フィン(6)を備えている。これに
より導体(1)の温度上昇による熱を逃がして次に述べ
るセンサ部(力が高温になることを防止している。The case (2) is also provided with a conductor clamp (5) made of a material with poor thermal conductivity on one side. This conductor clamp (5) clamps the conductor (1) when the case (2) is closed, thereby positioning the conductor (1) accurately at the center of the toroidal coil (4) and preventing fluctuations in the output. It is for. Furthermore, each case (2) is provided with a heat dissipation fin (6) on the outside of the conductor clamp (5). This allows the heat due to the rise in temperature of the conductor (1) to escape and prevents the sensor section (to be described below) from becoming high temperature.
センサ部(7)は図示のように各ケース(2)とパイプ
(8)により気密に接続されており、その内部にトロイ
ダルコイル(4)の二次側のソレノイド(9)が設けら
れている。そしてこのソレノイド(9)の中心に全電流
に比例した磁界を検出し、光信号に変換するファラディ
素子00)が取付けられている。なおセンサ部(7)の
全体はシールドケースで覆われて検出精度を高めている
。As shown in the figure, the sensor part (7) is airtightly connected to each case (2) by a pipe (8), and a solenoid (9) on the secondary side of the toroidal coil (4) is provided inside the sensor part (7). . A Faraday element 00) is attached to the center of this solenoid (9) for detecting a magnetic field proportional to the total current and converting it into an optical signal. Note that the entire sensor section (7) is covered with a shield case to improve detection accuracy.
上記のトロイダルコイル(4)は磁心が空心で断面積が
10〜20cd、巻数は1500〜3000ター :/
、ソレノイド(9)は磁心が空心で直径が20〜50n
+o+、巻数は4゜OO〜8000ターンが適当である
。これはファラディ素子00)に要求される50KAで
750エルステ・7ド以上の磁場が得られることという
条件を満足するために決定される値である。即ち、第4
図に示す縦軸にソレノイドコイルの必要巻数、横軸にト
ロイダルコイルの必要巻数を取ったグラフ上で考えた場
合、ソレノイドコイルに流せる電流限界を巻線径より5
Aとすると、下側の直線よりも上方の領域であることが
要求される。またトロイダルコイル(4)の最大限界寸
法上から断面積が20d以下とすると、上側の直線より
も下方の領域であることが要求される。さらにトロイダ
ルコイル(4)の断面積を20c+11以下とすると3
000ターンが限界であり、右側の垂直線より左側の領
域であることが要求される。これらを総合するとハンチ
ングを付した好ましい領域が決定され、前記した値を得
ることができる。The above toroidal coil (4) has an air core, a cross-sectional area of 10 to 20 cd, and a number of turns of 1500 to 3000 ter.
, the solenoid (9) has an air core and a diameter of 20 to 50 nm.
+o+, the appropriate number of turns is 4°OO to 8000 turns. This value is determined to satisfy the condition required for the Faraday element 00) that a magnetic field of 750 oerste.7 de or more can be obtained at 50 KA. That is, the fourth
When considering the graph shown in the figure, where the vertical axis is the required number of turns of the solenoid coil and the horizontal axis is the required number of turns of the toroidal coil, the current limit that can be passed through the solenoid coil is 5
If A, the area is required to be above the lower straight line. Further, if the cross-sectional area is 20 d or less from the maximum limit dimension of the toroidal coil (4), it is required that the area is below the upper straight line. Furthermore, if the cross-sectional area of the toroidal coil (4) is 20c+11 or less, 3
The limit is 000 turns, and the area is required to be on the left side of the right vertical line. By combining these, a preferable region with hunting can be determined, and the above-mentioned value can be obtained.
このように構成された第1の発明の複導体用光CTは、
複数本の導体(1)を流れる大電流をトロイダルコイル
(4)によって合成したうえで、その二次側のソレノイ
ド(9)のファラディ素子0ωにより光信号として検出
することができるものであり、次の通りの利点を持つ。The optical CT for double conductor of the first invention configured in this way is as follows:
A large current flowing through multiple conductors (1) is synthesized by a toroidal coil (4) and then detected as an optical signal by a Faraday element 0ω of a solenoid (9) on the secondary side. With the advantages of street.
第1に、各導体(1)の電流を合成して検出できるので
、高い測定精度を確保することができる。First, since the currents of each conductor (1) can be combined and detected, high measurement accuracy can be ensured.
第2に、導体(1)のまわりにケース(2)を閉じるこ
とにより既設の導体(1)を切断することなく取付けが
可能である。Second, by closing the case (2) around the conductor (1), installation is possible without cutting the existing conductor (1).
第3に、ケース(2)に導体クランプ(5)を設けたの
で導体(1)を常に正しくトロイダルコイル(4)の中
心に位置させることができ、測定誤差を小さくすること
ができる。Thirdly, since the conductor clamp (5) is provided on the case (2), the conductor (1) can always be correctly positioned at the center of the toroidal coil (4), and measurement errors can be reduced.
第4に、従来の大型巻線鉄心を持つCTに比較して小型
化、軽量化を図ることができ、架線に余分な荷重を掛け
ることがなく、狭い場所にも、既設の設備にも容易に取
付けが可能である。Fourth, it can be made smaller and lighter than conventional CTs with large wire-wound cores, and there is no need to put extra load on overhead wires, making it easy to install in narrow spaces or with existing equipment. It can be installed on.
第5に、ファラディ素子0ωにより電流を光信号に変換
して取り出すので、信号をセンサから光ファイバーによ
って母線上を自由に引き回して取り出すことができ、設
置位置が限定されることがない。Fifth, since the current is converted into an optical signal and extracted by the Faraday element 0ω, the signal can be freely routed from the sensor on the bus bar using the optical fiber and extracted, and the installation position is not limited.
第5図以下は第2の発明の実施例を示すものであり、第
6図の回路図に示すようにセンサ部(7)のみが相違す
るものである。即ち、第2の発明ではトロイダルコイル
(4)の二次側に負担抵抗θDを取り付けるとともに、
その両端の発生電圧を検出するためのポッケルス素子α
2が取り付けられている。FIG. 5 and subsequent figures show an embodiment of the second invention, which differs only in the sensor section (7) as shown in the circuit diagram of FIG. 6. That is, in the second invention, the burden resistance θD is attached to the secondary side of the toroidal coil (4), and
Pockels element α for detecting the voltage generated across it
2 is installed.
また本実施例では負担抵抗00と並列にサージ吸収用素
子OJを接続し、ポッケルス素子(12+の破損を防止
している。なお上記した第5図と第6図は2導体用のも
のを示すが、第7図は3導体用、第8図は4導体用のも
のを示している。In addition, in this embodiment, a surge absorbing element OJ is connected in parallel with the burden resistance 00 to prevent damage to the Pockels element (12+).The above-mentioned Figures 5 and 6 show the one for two conductors. However, FIG. 7 shows one for three conductors, and FIG. 8 shows one for four conductors.
第2の発明における負担抵抗(11)の大きさはIKΩ
以上とすることが好ましい。これはポッケルス素子qり
の特性上負担抵抗(II)に要求される、6KAの定格
電流時の発生電圧が100V以下、低電流時(0,2K
A)の発生電圧がIV以上、短絡電流時(50KA)の
発生電圧が500V以下との条件を満足するためである
。第9図に示される縦軸に出力電圧、横軸に通電電流を
取ったグラフからこれらの各条件を満足できる負担抵抗
値を求めると、負担抵抗値が上記したIKΩ〜100
KΩの範囲内にあることが好ましいことが分かる。The size of the burden resistance (11) in the second invention is IKΩ
It is preferable to set it as above. This is because the generated voltage at the rated current of 6 KA is 100 V or less and at low current (0.2 K), which is required for the burden resistance (II) due to the characteristics of the Pockels element.
This is to satisfy the conditions of A) that the generated voltage is IV or more and the generated voltage at the time of short circuit current (50 KA) is 500 V or less. The burden resistance value that satisfies each of these conditions is determined from the graph shown in FIG. 9, in which the vertical axis is the output voltage and the horizontal axis is the conduction current.
It can be seen that it is preferable to be within the range of KΩ.
このように構成された第2の発明の複導体用光CTも、
複数本の導体(1)を流れる大電流をトロイダルコイル
(4)によって合成したうえで、ポッケルス素子021
により光信号として検出することができるものであり、
検出部の構成が異なるだけで第1の発明について述べた
と同様の利点を有するものである。The optical CT for a double conductor of the second invention configured in this manner also includes:
The large current flowing through the plurality of conductors (1) is combined by the toroidal coil (4), and then the Pockels element 021
can be detected as an optical signal by
This invention has the same advantages as described for the first invention, except that the configuration of the detection section is different.
なお以上の第1の発明及び第2の発明の実施例では、ト
ロイダルコイル(4)、ソレノイド(9)ともに空心の
ものとされているが、これらのうちの一方または双方に
鉄心を設けることもできる。In the above embodiments of the first invention and the second invention, both the toroidal coil (4) and the solenoid (9) are air-core, but one or both of them may be provided with an iron core. can.
(発明の効果)
以上に説明したとおり、これらの発明の複導体用光CT
は、狭い場所にも取付けが可能であり、また既設の導体
を切断することなく容易に取付けができ、しかも全導体
を流れる電流を精度よく検出することができる利点を有
するものである。(Effect of the invention) As explained above, the optical CT for double conductor of these inventions
This has the advantage that it can be installed even in narrow spaces, can be easily installed without cutting existing conductors, and can accurately detect the current flowing through all conductors.
よって本発明は従来の問題点を解決したものとして、産
業の発展に寄与するところは極めて大である。Therefore, the present invention can greatly contribute to the development of industry as a solution to the conventional problems.
第1図は第1の発明の実施例を示す平面図、第2図はそ
の正面図、第3図はその回路図、第4図はトロイダルコ
イルの巻数とソレノイドコイルの巻数との関係を示すグ
ラフ、第5図は第2の発明の実施例を示す平面図、第6
図はその回路図、第7図は第2の発明を3導体母線に適
用した実施例を示す正面図、第8図は同じく4導体母線
に適用した実施例を示す正面図、第9図は負担抵抗の通
電電流と出力電圧との関係を示すグラフである。
(1):導体、(2)二ケース、(3):ヒンジ部、(
4) : I−ロイダルコイル、(5):導体クランプ
、(9):ソレノイド、0ω:ファラディ素子、00:
負担抵抗、021:ポッケルス素子。Fig. 1 is a plan view showing an embodiment of the first invention, Fig. 2 is a front view thereof, Fig. 3 is a circuit diagram thereof, and Fig. 4 shows the relationship between the number of turns of the toroidal coil and the number of turns of the solenoid coil. Graph, Fig. 5 is a plan view showing the embodiment of the second invention, Fig. 6 is a plan view showing the embodiment of the second invention.
The figure is a circuit diagram, FIG. 7 is a front view showing an embodiment in which the second invention is applied to a three-conductor bus, FIG. 8 is a front view showing an embodiment in which the second invention is applied to a four-conductor bus, and FIG. It is a graph showing the relationship between the current flowing through the burden resistor and the output voltage. (1): Conductor, (2) Two cases, (3): Hinge, (
4): I-loidal coil, (5): Conductor clamp, (9): Solenoid, 0ω: Faraday element, 00:
Burden resistance, 021: Pockels element.
Claims (1)
)を備えた開閉式のケース(2)を設け、各ケース(2
)の内部に往路、復路ともにそのヒンジ部(3)を通過
するように巻き戻した一連のトロイダルコイル(4)を
取り付けるとともに、その二次側のソレノイド(9)に
全電流に比例した磁界を検出するファラディ素子(10
)を取り付けたことを特徴とする複導体用光CT。 2、複数本の各導体(1)のまわりに導体クランプ(5
)を備えた開閉式のケース(2)を設け、各ケース(2
)の内部に往路、復路ともにそのヒンジ部(3)を通過
するように巻き戻した一連のトロイダルコイル(4)を
取り付けるとともに、その二次側に負担抵抗(11)と
その両端の発生電圧を検出するポッケルス素子(12)
とを取り付けたことを特徴とする複導体用光CT。[Claims] 1. Conductor clamps (5
), each case (2) is equipped with a retractable case (2).
) is equipped with a series of unwound toroidal coils (4) that pass through the hinge part (3) on both the forward and return trips, and a magnetic field proportional to the total current is applied to the solenoid (9) on the secondary side. Faraday element to detect (10
) is attached to an optical CT for double conductors. 2. Place conductor clamps (5) around each of the multiple conductors (1).
), each case (2) is equipped with a retractable case (2).
) is equipped with a series of toroidal coils (4) which are unwound so as to pass through the hinge part (3) on both the forward and return trips, and a load resistor (11) on the secondary side and the voltage generated at both ends thereof. Pockels element to detect (12)
An optical CT for a double conductor, characterized in that it is equipped with.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2086868A JP2879927B2 (en) | 1990-03-30 | 1990-03-30 | Optical CT for multiple conductors |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2086868A JP2879927B2 (en) | 1990-03-30 | 1990-03-30 | Optical CT for multiple conductors |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH03285180A true JPH03285180A (en) | 1991-12-16 |
JP2879927B2 JP2879927B2 (en) | 1999-04-05 |
Family
ID=13898801
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2086868A Expired - Lifetime JP2879927B2 (en) | 1990-03-30 | 1990-03-30 | Optical CT for multiple conductors |
Country Status (1)
Country | Link |
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JP (1) | JP2879927B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006098378A (en) * | 2004-09-29 | 2006-04-13 | Seratekku Kk | High precision voltage/current sensor for power transmission and distribution system |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5357983U (en) * | 1976-10-19 | 1978-05-17 | ||
JPS6157873U (en) * | 1984-09-21 | 1986-04-18 | ||
JPS63198879A (en) * | 1986-11-14 | 1988-08-17 | ナイアガラ モーホーク パワー コーポレーシヨン | Magnetic shunt device for power feeder for transmission line sensor module |
JPH01120674U (en) * | 1988-02-04 | 1989-08-16 | ||
JPH01162671U (en) * | 1988-04-28 | 1989-11-13 |
-
1990
- 1990-03-30 JP JP2086868A patent/JP2879927B2/en not_active Expired - Lifetime
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5357983U (en) * | 1976-10-19 | 1978-05-17 | ||
JPS6157873U (en) * | 1984-09-21 | 1986-04-18 | ||
JPS63198879A (en) * | 1986-11-14 | 1988-08-17 | ナイアガラ モーホーク パワー コーポレーシヨン | Magnetic shunt device for power feeder for transmission line sensor module |
JPH01120674U (en) * | 1988-02-04 | 1989-08-16 | ||
JPH01162671U (en) * | 1988-04-28 | 1989-11-13 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006098378A (en) * | 2004-09-29 | 2006-04-13 | Seratekku Kk | High precision voltage/current sensor for power transmission and distribution system |
Also Published As
Publication number | Publication date |
---|---|
JP2879927B2 (en) | 1999-04-05 |
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