JPS5947526B2 - Transformer protection method - Google Patents
Transformer protection methodInfo
- Publication number
- JPS5947526B2 JPS5947526B2 JP9149578A JP9149578A JPS5947526B2 JP S5947526 B2 JPS5947526 B2 JP S5947526B2 JP 9149578 A JP9149578 A JP 9149578A JP 9149578 A JP9149578 A JP 9149578A JP S5947526 B2 JPS5947526 B2 JP S5947526B2
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- Prior art keywords
- transformer
- current
- voltage
- primary
- advance
- 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.)
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Description
【発明の詳細な説明】
本発明は、電力系統の情報より、変圧器の保護を行う変
圧器の保護方式、特fこ、変圧器投入時と変圧器の内部
事故との識別をはかつてなる保護方式lこ関する。[Detailed Description of the Invention] The present invention provides a transformer protection method for protecting transformers based on power system information, which makes it easier to distinguish between transformer power-on and transformer internal accidents. Regarding the protection method.
計算機を用いた電力系統の保護装置は、各国、各メーカ
で研究が行われている。Computer-based power system protection devices are being researched by manufacturers in various countries.
第1図は、従来の変圧器保護の概念を示したものであり
、Gは電源、Lは負荷、SWI、2は遮断器を、CT1
,2は変流器を、Trは変圧器を、Rは保護装置を示す
。Figure 1 shows the concept of conventional transformer protection, where G is the power supply, L is the load, SWI, 2 is the circuit breaker, and CT1 is the
, 2 indicates a current transformer, Tr indicates a transformer, and R indicates a protection device.
保護装置Rは変流器CTL2より変圧器1次、2次の電
流を取り込み、tcrl。The protection device R takes in the transformer primary and secondary currents from the current transformer CTL2 and outputs tcrl.
2の間で生ずる事故を検出する。Detect accidents that occur between the two.
常時、負荷Lべの電力供給fこ際しては、遮断器SW1
を投入し、その後SW2を投入している。Always supply power to load L. At this time, circuit breaker SW1
, and then SW2.
この過程で、SWlの投入時lこ、大きな励磁電流が流
れ、第2調波含有罪が小さいと、第2図fこ示すような
構成の保護方式では、変圧器内部事故と誤判断し、遮断
器SW1 fこ遮断指令を発し、誤遮断することがあっ
た。In this process, when SW1 is turned on, a large excitation current flows, and if the second harmonic content is small, the protection system with the configuration shown in Figure 2 f will incorrectly judge that it is an internal fault in the transformer. The circuit breaker SW1 sometimes issued a disconnection command and caused an erroneous disconnection.
次tこ第2図の構成lこつき説明する。変流器CT15
2を介して得られる変圧器1次電流112次電流12を
取り込み、フィルタ1,2で直流分を除去し、演算部3
でフィルタ1と2の出力の差を取り、演算部3の出力l
こ基本波成分のみを通過させるフィルタ11でフィルタ
処理を施し、動作力をうる。Next, the configuration of FIG. 2 will be explained. Current transformer CT15
The transformer primary current 112 obtained through the transformer 2 is taken in, the DC component is removed by the filters 1 and 2, and the
The difference between the outputs of filters 1 and 2 is calculated, and the output l of calculation unit 3 is
Filter processing is performed using a filter 11 that allows only the fundamental wave component to pass, and the operating force is obtained.
一方、抑制力は、フィルタ1,2の出力の和を演算部4
でとり、この結果を基本波のみを通過させるフィルタ5
および第2調波のみを通過させるフィルタ6Fこ入力さ
せ、フィルタリングを行う。On the other hand, the suppressing force is calculated by calculating the sum of the outputs of filters 1 and 2.
filter 5 that passes only the fundamental wave.
Filtering is performed by inputting a filter 6F that passes only the second harmonic.
フィルタ5の出力Iこ抑制係数を乗算部7で乗じ、演算
部8で、乗算部7とフィルタ6の出力の和を求める。The output of the filter 5 is multiplied by the suppression coefficient in the multiplier 7, and the arithmetic unit 8 calculates the sum of the outputs of the multiplier 7 and the filter 6.
演算部9では、フィルタ11の出力より、演算部8の出
力を減じ、この出力を演算部10で2乗し、この出力を
一定時間加算するフィルタ12)こより、直流レベルの
動作力を得、これを一定値と比較し、一定値以上では、
事故として検出していた。In the arithmetic unit 9, the output of the arithmetic unit 8 is subtracted from the output of the filter 11, this output is squared in the arithmetic unit 10, and this output is added to the filter 12 for a certain period of time.From this, a DC level operating force is obtained, Compare this with a certain value, and above a certain value,
It was detected as an accident.
このため、前記のような問題があった。For this reason, there were problems as described above.
ifこ、ここで大きな意味を持つ第2調波の名有岸を定
める要因tこつき説明する。If this is the case, here we will explain the factors that determine the famous shore of the second harmonic, which has great significance.
第2調波の含有ヱを定める大きな要因は、変圧器の残留
磁束と電圧の投入位相である。The major factors that determine the content of the second harmonic are the residual magnetic flux of the transformer and the voltage input phase.
この関係を示したものが第3図であり、この図の横軸は
残留磁束を縦軸は、第2調波の含有ギを示す。This relationship is shown in FIG. 3, in which the horizontal axis shows the residual magnetic flux and the vertical axis shows the second harmonic content.
曲線Aは投入角0度、180度を、曲線Bは投入角90
度、270度を示す。Curve A has a loading angle of 0 degrees and 180 degrees, and curve B has a loading angle of 90 degrees.
degree, 270 degrees.
また、曲線Cは、励磁突入電流として、大きな電流の流
れる限界を示す。Further, curve C indicates a limit where a large current can flow as an excitation inrush current.
この図で直線Lv。を従来の第2調波抑制係数とすると
、直線C2Lv、および曲線A、Bで囲まれた範囲が、
励磁突入電流で誤動作する領域であった。In this figure, the straight line Lv. If is the conventional second harmonic suppression coefficient, the range surrounded by the straight line C2Lv and curves A and B is
This was the area where the magnetizing inrush current caused malfunctions.
この範囲は、最近の変圧器では、せばまっているが、皆
無トすることはできない。Although this range is narrower in modern transformers, it cannot be completely eliminated.
更tこ、最近の変圧器では、鉄心特注の向上および経済
設計等のため、基本波電流と第2調波含有ギの関係は、
第4図のようfこ表わされる。Furthermore, in recent transformers, due to improvements in custom-made iron cores and economical design, the relationship between fundamental wave current and second harmonic content is as follows.
It is expressed as f as shown in FIG.
同図で曲線りは、励磁突入時の関係を、曲線Eは、事故
時の関係を、領域Fは、第2調波抱有璋が、励磁突入時
と事故時で分離困難な領域を示す。In the figure, the curved line indicates the relationship at the time of excitation inrush, the curve E indicates the relationship at the time of an accident, and the area F indicates the area where the second harmonic wave is difficult to separate between the time of excitation inrush and the time of an accident. .
このようlこ、第2調波含有ギのみでは、事故時と励磁
突入時を完全lこ分離することはできない。In this way, it is not possible to completely separate the accident event and the excitation inrush event using only the second harmonic-containing signal.
このため、本発明は、この欠点を解消して、変圧器内部
事故と電源投入時との識別を行い得るようtこした変圧
器の保護方式を提供することtこある。Therefore, it is an object of the present invention to provide a protection method for a transformer that overcomes this drawback and makes it possible to distinguish between an internal transformer fault and a power-on fault.
本発明は、励磁突入時fこは、変圧器の巻線抵抗、もれ
リアクタンス等の電気的係数は変化せず、内部事故時l
こは、抵抗、もれリアクタンス等の電気的係数が変化す
ることfこ着目したものである。In the present invention, electrical coefficients such as winding resistance and leakage reactance of the transformer do not change during excitation inrush, and l
This focuses on the fact that electrical coefficients such as resistance and leakage reactance change.
次1こ本願の原理を説明する。Next, the principle of the present application will be explained.
第5図は、変圧器の等何回路を示したもので、’I j
r2は1次および3欠の巻線抵抗、L3.L2は1次
および2欠のもれインダクタンスを、vl、v2は1次
および2欠の端子電圧を、+1212は1次および2次
の電流を、Φは磁束を、nl)n2は1次および2欠の
巻数を示す。Figure 5 shows the equal circuit of a transformer, 'I j
r2 is the primary and triple winding resistance, L3. L2 is the primary and double leakage inductance, vl and v2 are the primary and double terminal voltages, +1212 is the primary and secondary current, Φ is the magnetic flux, nl)n2 is the primary and Indicates the number of volumes with two missing parts.
尚、rl 、r22 L12 L25 nl ) n2
は変圧器の電気的係数である。In addition, rl, r22 L12 L25 nl) n2
is the electrical coefficient of the transformer.
この図より、 と表わせる。From this figure, It can be expressed as
この式より、を消去すると、 これを書き換えて、 と表わせる。From this formula, if we eliminate Rewrite this, It can be expressed as
ここで、n12 n22 rl、r22 L) 2L2
は、変圧器が定まれば決まるものであり、この他、電圧
、電流の瞬時値Vl)V2) 11> 12が求まれば
、変圧器の健全時、励磁突入時は、(4)式が成立する
。Here, n12 n22 rl, r22 L) 2L2
is determined once the transformer is determined, and in addition, if the instantaneous values of voltage and current Vl) V2) 11>12 are found, then when the transformer is healthy and during excitation inrush, equation (4) can be obtained. To establish.
上記(4)式で左側のカッコ内は巻線数を考慮しない1
次側全体電圧、右側のカッコ内は巻線数を考慮しない2
次側全体電圧と称する。In the above equation (4), the number in parentheses on the left does not take into account the number of windings.
Next-side overall voltage, the number in parentheses on the right does not take into account the number of turns2
It is called the next-side overall voltage.
従って(4)式は巻線数を考慮した1次側、2次側の全
体電圧と云うことができる。Therefore, equation (4) can be said to be the overall voltage on the primary and secondary sides taking into account the number of windings.
これlこ対し、変圧器の内部事故時tこは、n、。On the other hand, in the event of an internal fault in the transformer, n.
n2 t r 1.r 22 L+ 、L2があらかじ
め求めであるものと異なるため、
となる。n2 tr 1. Since r 22 L+ and L2 are different from those determined in advance, the following is obtained.
ここで、■1′、v2′、11′、12′は、事故時の
電圧、電流を示す。Here, ■1', v2', 11', and 12' indicate the voltage and current at the time of the accident.
このようfこ、健全時と事故時では、電圧、電流、イン
ピーダンス関係の異なることlこ着目して、事故を検出
しようとするものである。In this way, an attempt is made to detect an accident by focusing on the fact that the relationship between voltage, current, and impedance is different between a normal state and an accident state.
第6図(ここの時の各種状態lこおける電圧、電流およ
び(5)式の出力の関係を示す。FIG. 6 shows the relationship between voltage, current, and the output of equation (5) under various conditions.
このようlこ、(5)式の出力は、内部事故以外では、
発生しない。In this way, the output of equation (5) is, except for an internal accident,
Does not occur.
このことより、内部事故を明確fこ検出できる。From this, internal accidents can be clearly detected.
次lこ、具体的な処理方法につき説明する。Next, a specific processing method will be explained.
第1図Eこ示すようlこ、変圧器1次、2次電流の他、
変圧器1次、2次電圧を電圧変成器PTI。As shown in Figure 1E, in addition to the primary and secondary currents of the transformer,
Transformer primary and secondary voltage is converted to voltage transformer PTI.
PT2を介し、電流情報と同様AD変換器A/Dでディ
ジタル情報rこ変換し、保護装置Rで(3)又は(4)
式が成り立つか否かの判断を行い、事故を検出した場合
lこは、遮断器5W1Fこ遮断指令を発する。Through PT2, the digital information is converted by the AD converter A/D in the same way as the current information, and the protection device R converts it into (3) or (4).
It is determined whether the formula holds true or not, and if an accident is detected, a command to shut off circuit breaker 5W1F is issued.
次lこ処理フローfこつき第8図1こより説明する。Next, the processing flow will be explained with reference to FIG. 8.
フ0−100で、時刻t1こおける変圧器2入電圧v1
.i次電流11.2入電圧v2.2次電流12を取り込
み、フロー101で、あらかじめ記憶しである変圧器1
次巻線抵抗「1と1次電流11との積を求め、フ0−1
02で、変圧器1次電流の現時点の値より、−サンプル
前の値の差をとり、ヅンブリング間隔で除する。At time t1, input voltage v1 of transformer 2 is 0-100.
.. The i-order current 11.2 input voltage v2.The secondary current 12 is taken in, and in flow 101, the transformer 1 which is stored in advance
Find the product of the secondary winding resistance '1 and the primary current 11, and
At step 02, the difference between the current value of the transformer primary current and the previous value of the -sample is taken and divided by the sizing interval.
フ0−103で、フロー102の結果lこあらかじめ記
憶しである変圧器1次もれインダクタンスL1を乗する
。In step 0-103, the result of step 102 is multiplied by the transformer primary leakage inductance L1, which is stored in advance.
フロー104で変圧器1次電圧v1よりフ0−101お
よびフo−1oaの結果を減じ、フロー105でフロー
104の結果lこあらかじめ記憶しである変圧器2次巻
数n2を乗する。In flow 104, the results of F0-101 and F0-1oa are subtracted from the transformer primary voltage v1, and in flow 105, the result of flow 104 is multiplied by the pre-stored transformer secondary winding number n2.
フ0−106であらかじめ記憶しである変圧器2次巻線
抵抗「2と2次電流12との債を求め、フロー101で
、変圧器2次電流の現時点の値より、−サンプル前の値
の差をとりサンプリング間隔で除する。Step 0-106 calculates the relationship between the transformer secondary winding resistance 2 and the secondary current 12, which are stored in advance, and step 101 calculates the current value of the transformer secondary current - the value before the sample. Take the difference between and divide by the sampling interval.
フロー108で、フロー107の結果lこあらかじめ記
憶しである変圧器2次もれインダクタンスL2を乗する
。In flow 108, the result of flow 107 is multiplied by the transformer secondary leakage inductance L2, which is stored in advance.
フロー109で変圧器2次電圧v2よりフ0−106お
よびフロー108の結果を減じ、フ0−110でフロー
109の結果fこあらかじめ記憶しである変圧器1次巻
数n1を乗する。In flow 109, the results of steps 0-106 and 108 are subtracted from the transformer secondary voltage v2, and in steps 0-110, the result of step 109 is multiplied by the pre-stored transformer primary winding number n1.
フ0−111で70−105の結果よりフロー110の
結果を減じ、この値が一定値以内では正常であるとして
、フロー112で1次の処理を始める時間まで待つ。At step 0-111, the result of flow 110 is subtracted from the result of step 70-105, and assuming that this value is normal within a certain value, the flow waits until the time to start the primary processing at step 112.
フロー111の結果が一定値以上では、変圧器内部の事
故として、検出し、該当する遮断器lこ遮断指令を発す
る。If the result of flow 111 is above a certain value, it is detected as an accident inside the transformer, and a command to shut off the corresponding circuit breaker is issued.
このようlこすることlこより、比較的簡単な処理で、
変圧器の内部事故を検出でき、経済的効果は非常fこ大
きい。This kind of rubbing is a relatively simple process,
Internal faults in the transformer can be detected, and the economic effect is very large.
また、事故の検出時間がはやいため、電力系統の安定度
向上fこ及ぼす効果は大きい3これまでの説明は、一度
でも(4)式の結果が一定値以上lこなった場合lこ検
出する方式Eこついて説明したが、検出信頼度をあげる
1こは、第6図の111のあとlこ、回数をかぞえる処
理を追加すればよい3又、これまでの説明は、ディジタ
ルで処理する例1こついて行ったが、アナログで処理で
きることも当然考えられる。In addition, since the detection time of an accident is quick, it has a large effect on improving the stability of the power system.3 The explanation so far has been that if the result of equation (4) exceeds a certain value even once, it will be detected. Method E has been explained in detail, but one way to increase the detection reliability is to add a process to count the number of times after 111 in Fig. 6.Also, the explanation so far is an example of digital processing. I ran into one problem, but it is of course possible that it could be processed using analog.
以上述べたようFこ本発明fこよれば、変圧器の1次側
、2次側の各電圧V1.V2、電流11.■2を取り込
み、変圧器の正常時の1次側、2次側の巻線抵抗r、
、 r2 、もれインダクタンスLH、L2、及び巻数
nI2 n2がら
を演算し、その結果Cが一定幅内tこあるときfこ変圧
器の正常及び投入時と判定できるので、処理が比較的簡
単であると共lこ、変圧器投入時と内部事故との識別を
正確fこ行うことができ、かつ事故検出時間がはやいと
いう効果がある。As described above, according to the present invention, each voltage V1 on the primary side and secondary side of the transformer. V2, current 11. ■ Take in 2, and the winding resistance r of the primary and secondary sides of the transformer when it is normal,
, r2, leakage inductance LH, L2, and number of turns nI2 (n2) are calculated, and when C is within a certain range, it can be determined that the transformer is normal and turned on, so the process is relatively simple. In addition, it is possible to accurately distinguish between the time when the transformer is turned on and an internal fault, and the fault detection time is quick.
第1図は従来の全体図、第2図は従来の具体的構成図、
第3図は説明図、第4図は従来例の欠点を説明する図、
第5図は変圧器の等価回路図、第6図はタイムチャート
、第7図は本発明の全体図、第8図は処理フロー図であ
る。
T「・・・・・・トランス、PT’l、PT2・・・・
・・変成器、CTI、CT2・・・・・・変流器、R・
・・・・・保護装置。Figure 1 is an overall diagram of the conventional system, Figure 2 is a specific configuration diagram of the conventional system,
Figure 3 is an explanatory diagram, Figure 4 is a diagram explaining the drawbacks of the conventional example,
FIG. 5 is an equivalent circuit diagram of the transformer, FIG. 6 is a time chart, FIG. 7 is an overall diagram of the present invention, and FIG. 8 is a processing flow diagram. T ``...Trance, PT'l, PT2...
...Transformer, CTI, CT2...Current transformer, R.
...Protective device.
Claims (1)
2次側電圧v2、電流12を取り込み、あらかじめ与え
られてなる変圧器の正常時の1次側、2次側の巻線抵抗
rl 2 r2、もれインダクタンスL12 L2 s
及び巻数nI)n2をもとlこ、の演算をし、この演算
結果Cが一定幅内のときlこは正常及び変圧器投入時、
前記演算結果Cが一定幅を超えているときlこは変圧器
内部事故との識別を行い、この識別結果lこ応じて変圧
器の保護を行なわせるようlこした変圧器保護方式。 2、特許請求の範囲第1項lこおいて、上記変圧器0)
l i[t Vl、電流■2.2次電圧v2、電流■
2の取り込みはサンプリングtこよって行い、その取り
込み後の上記各処理はディジタル的lこ行わせるようl
こした変圧器保護方式。[Claims] 1 The primary side of the transformer during normal operation, which is obtained in advance by taking in the primary side voltage 1 and current 11 of the transformer, and the secondary side voltage v2 and current 12 of the transformer, which are given in advance. Secondary winding resistance rl 2 r2, leakage inductance L12 L2 s
and the number of turns nI)n2, calculate 1, and when the calculation result C is within a certain range, 1 is normal and the transformer is turned on,
A transformer protection system in which when the calculation result C exceeds a certain range, it is identified as an internal fault in the transformer, and the transformer is protected in accordance with this identification result. 2.Claim 1, l, wherein the transformer 0)
l i[t Vl, current ■2. Secondary voltage v2, current ■
2 is taken in by sampling, and each of the above-mentioned processes after the acquisition is performed digitally.
This is a transformer protection method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9149578A JPS5947526B2 (en) | 1978-07-28 | 1978-07-28 | Transformer protection method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9149578A JPS5947526B2 (en) | 1978-07-28 | 1978-07-28 | Transformer protection method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5518856A JPS5518856A (en) | 1980-02-09 |
| JPS5947526B2 true JPS5947526B2 (en) | 1984-11-20 |
Family
ID=14027984
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9149578A Expired JPS5947526B2 (en) | 1978-07-28 | 1978-07-28 | Transformer protection method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5947526B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5999925A (en) * | 1982-11-30 | 1984-06-08 | 株式会社東芝 | Exciting rush detecting method for transformer |
-
1978
- 1978-07-28 JP JP9149578A patent/JPS5947526B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5518856A (en) | 1980-02-09 |
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