JPS609331A - Tide calculating system - Google Patents

Tide calculating system

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Publication number
JPS609331A
JPS609331A JP58117510A JP11751083A JPS609331A JP S609331 A JPS609331 A JP S609331A JP 58117510 A JP58117510 A JP 58117510A JP 11751083 A JP11751083 A JP 11751083A JP S609331 A JPS609331 A JP S609331A
Authority
JP
Japan
Prior art keywords
power
bus
load
power flow
processing block
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.)
Pending
Application number
JP58117510A
Other languages
Japanese (ja)
Inventor
深谷 満
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP58117510A priority Critical patent/JPS609331A/en
Publication of JPS609331A publication Critical patent/JPS609331A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 この発明は、電力系統に過負荷を発生させることなく、
特定の複数母線ビ経由して着目母線より新たに供給し得
る電力量ケ算出する潮流算出方式%式% この種の方式としては、第1図のフローチャートに示す
ようなコンピュータ処理が提案されている。第1図にお
いて、処理ブロック1は着目母線にのみ単位負荷ン設定
し、その他の全ての発電量及び負荷量を零に設定する。
[Detailed Description of the Invention] This invention enables
A power flow calculation method that calculates the amount of power that can be newly supplied from the target bus via a specific plurality of bus lines % Formula % As this type of method, computer processing as shown in the flowchart in Figure 1 has been proposed. . In FIG. 1, processing block 1 sets a unit load only to the bus of interest, and sets all other power generation amounts and load amounts to zero.

続いて処理ブロック2ば、処理ブロック1で設定された
発電量及び負荷量に基づき、電力系統の潮流、即ち単位
負荷潮流を計算する。一方処理ブロック6は着目母線の
発電量及び負荷量につき変化する前の1.力系統の潮流
値χ計測計算推定又は予」りによりめろ。処理ブロック
4は、処理プロツク2及び6でめた潮流値を用い、各電
力設備に過負荷を発生させることな(、新たに着目母線
より供給し得る電力量乞算出する。
Subsequently, processing block 2 calculates the power flow of the power system, that is, the unit load power flow, based on the power generation amount and load amount set in processing block 1. On the other hand, processing block 6 performs 1. Use the power system power flow value χ measurement calculation estimation or preliminary calculation. Processing block 4 uses the power flow values determined in processing blocks 2 and 6 to calculate the amount of power that can be newly supplied from the target bus without overloading each power facility.

このような従来の潮流算出方式では、着目母線が1母線
の時のみ電力量の範囲ン求めることができ、複数の母線
に着目した場合の電力量ン求めることが出来ないという
大きな欠点があった。
This conventional power flow calculation method has a major drawback in that it is only possible to determine the range of power consumption when the target bus is one bus, and it is not possible to determine the range of power consumption when multiple buses are focused. .

この発明は、上記のような従来の潮流算出方式の欠点ン
除去するためになされたもので、着目母線が複数存在し
その複数の着目母線から電力が同時に供給さ几る場合に
、順次着目母線に単位負荷ン設定し、他の発電量及び負
荷量を零とした電力系統ン想定する。続いてこのTE電
力系統対して直流フロー法による潮流計算7行い、各電
力設備に対する潮流(単位負荷潮流)と、各着目母線の
位相角(単位負荷位相角)ン求めろ。さらに着目母線と
、その着目母線より環カン供給される母線とを結ぶ宙、
力設備のインピーダンス、単位負荷潮流及び7N 6r
負負荷相角ン用いて所定の一次方程式ン解くことにより
、着目母線と供給される母線と乞継いだ場合の潮流状朝
ン求め、また同様な一次方程式χ解くことにより、供給
さ几る母線に単位負荷を設定した時の潮流状態をめる。
This invention was made to eliminate the drawbacks of the conventional power flow calculation method as described above, and when there are multiple buses of interest and power is supplied from the plurality of buses of interest at the same time, Assume a power system with a unit load set at , and other power generation and load amounts set to zero. Next, perform power flow calculation 7 using the DC flow method for this TE power system, and find the power flow (unit load flow) for each power facility and the phase angle (unit load phase angle) of each bus of interest. Furthermore, the space connecting the bus of interest and the bus that is supplied from the bus of interest to the ring ring,
Power equipment impedance, unit load current and 7N 6r
By solving a predetermined linear equation using the negative load phase angle, we can find the tidal flow rate when the target bus line and the supplied bus line intersect, and by solving a similar linear equation, we can find the supplied bus line. Determine the power flow state when the unit load is set to .

これらの潮流状態と電力系統の各設備の潮流値とから、
複数の着目母線より新たに供給できる電力量ン算出する
潮流算出方式ン提供することを目的とする。
From these power flow conditions and the power flow values of each equipment in the power system,
The purpose of this invention is to provide a power flow calculation method for calculating the amount of power that can be newly supplied from a plurality of focused buses.

以下、この発明の一実施例χ第2図について説明する。Hereinafter, one embodiment of the present invention will be described with reference to FIG. 2.

第2図において、処理ブロック1は特定の系統に対して
電力を供給することができろ複数の特定の母線に着目し
、この着目母線の1つづつについて順次単位負荷を設定
すると共に他σ)発電量及び負荷瞼乞零に設定し電力系
統の単位負荷潮流及び単6r負荷位相角を計算jる。次
に処理ブロック2は着目母線とその着目母線から電カケ
供給される母線とン結ぶ電力設備のみの潮流計算7行い
In FIG. 2, processing block 1 focuses on a plurality of specific buses that can supply power to a specific system, and sequentially sets a unit load for each of the buses of interest, and also sets a unit load for each of the buses of interest. The power generation amount and load are set to zero, and the unit load flow and single load phase angle of the power system are calculated. Next, processing block 2 performs power flow calculation 7 only for the bus of interest and the power equipment connected to the bus to which electricity is supplied from the bus of interest.

供給さ几る母線の直前の位置までの潮流値と直前σ’)
 (X’L i#での位相角と欠求める。処理ブロック
6は処理ブロック2でめた位相角と、着目母線から電力
乞供給される切線までの電力設備のインピーダンスとか
ら1位相角に関する連立方程式χ作成−する。処理ブロ
ック4は続いて処+)Uブロック6で作成した連立方程
式を解き、複数の着目母線から環カン供給される母線ま
での電力設備のそ几ぞtしに流オ′シるj副流1直と、
その時の′軽力を供給さ2する1σ線での位相角と欠計
算する。処理ブロック5は先の処理ブロック6で作成し
た連立方程式において、処理ブロック2でめた位相角を
零とし、環カン供給さ几る母線に単位負荷を設定した状
態で】!b立方程式を解き、着目母線の単位負荷位相角
と、着目母線と環カン供給される母線と乞結ぶ電力設備
の単位負荷潮流乞計算する。処理ブロック6は着目母線
が接続する電力系統の潮流値ン計測、計算。
Power flow value up to the position immediately before the supplied bus line and immediately before σ')
(The phase angle at The equation χ is created.Processing block 4 then solves the simultaneous equations created in block 6 and calculates the flow power for each of the power equipment from the plurality of target buses to the bus that is supplied to the ring. 'Siru j side stream 1st shift,
At that time, we calculate the phase angle at the 1σ line that supplies the light force. In processing block 5, in the simultaneous equations created in processing block 6, the phase angle obtained in processing block 2 is set to zero, and a unit load is set on the bus line fed by the ring can]! b Solve the equation and calculate the unit load phase angle of the bus of interest and the unit load power flow of the power equipment connected to the bus of interest and the bus that is supplied from the ring. Processing block 6 measures and calculates the power flow value of the power system to which the target bus is connected.

推定又は予測によりめる。処理ブロック7は先に述べた
処理ブロック4でめた電力を供給される母線へ流入する
潮流、及び処理ブロック1でめた単位負荷潮流を用いて
、処理ブロック6でめた潮流値の修正を行う。処理ブロ
ック8は、処理ブロック5でめた単位負荷潮流により、
処理ブロック1でめた単位負荷潮流を修正する。続いて
処理ブロック9では、処理ブロック7でめた潮流値及び
処理ブロック8で修正した単位負荷潮流!用い、各電力
設備に過負荷乞発生させずに、複数の着目母線より新た
に供給できる電力計を算出する。
Based on estimation or prediction. Processing block 7 corrects the power flow value determined in processing block 6 by using the power flow flowing into the bus to which power is supplied, determined in processing block 4, and the unit load power flow determined in processing block 1. conduct. Processing block 8 uses the unit load flow determined by processing block 5 to
Modify the unit load flow determined in processing block 1. Next, in processing block 9, the power flow value determined in processing block 7 and the unit load power flow corrected in processing block 8 are calculated. Using this method, we calculate the wattmeter that can be newly supplied from a plurality of target buses without overloading each power facility.

着目母線が2母線の場合について、第2図の潮流算出動
作を説明する。第3図は、着目母線とそれらの母線より
電カケ供給される母線とで構成さ几る系統構成図になっ
ている系統例により説明する。第3図において、着目母
線111及び着目母線212は、貝何世線13に送電線
114及び送電線215を経て接続している。この時開
閉器16゜19は閉状態、開閉器17.18は開状態と
なっている。
The power flow calculation operation shown in FIG. 2 will be explained in the case where there are two buses of interest. FIG. 3 will be explained using an example of a system that is a system configuration diagram consisting of a bus of interest and buses to which electric power is supplied from these buses. In FIG. 3, the bus of interest 111 and the bus of interest 212 are connected to the Kaisei line 13 via a power transmission line 114 and a power transmission line 215. At this time, the switches 16 and 19 are in the closed state, and the switches 17 and 18 are in the open state.

処理ブロック1では、まず着目母線111に単位負荷を
設定し、他の発電量及び負荷量を零にして単位負荷潮流
及び単位負荷位相角ン求め1着目母線1110単位負荷
位相角乞θ11、着目母線2120単位負荷位相角ンθ
1.とする。次に1着目母線212に対しても同様の処
理7行い、着目母線111の単位負荷位相角乞θ781
着目母線2120単位負荷位相角ンθ2.とする。
In processing block 1, first, a unit load is set on the focused bus 111, and the other power generation amounts and load amounts are set to zero, and the unit load power flow and unit load phase angle are determined. 2120 units load phase angle θ
1. shall be. Next, the same process 7 is performed for the first bus 212 of interest, and the unit load phase angle θ781 of the bus 111 of interest is
Observed bus line 2120 unit load phase angle θ2. shall be.

次に処理ブロック2では、送電線114のみの潮流計算
を行い、送電線】14の負荷母線16の直前の位相角ン
求めてこれをφ1とする。同様に送電線215に対して
も潮流計算ケ行い、ハγ相角をめてこれゲφ、とする。
Next, in processing block 2, a power flow calculation is performed only for the power transmission line 114, and the phase angle n immediately before the load bus 16 of the power transmission line 14 is determined, and this is set as φ1. Similarly, a power flow calculation is performed for the power transmission line 215, and the γ phase angle is calculated to be φ.

第4図は、この処理ブロック2の処理の様子ン示す系統
構成図である。
FIG. 4 is a system configuration diagram showing the processing of this processing block 2.

更に処理ブロック6では、第5図に示す系統構成因のよ
うに開閉器16.17を論理上1閉1として送電線11
4と送fii1M215と7流れる潮流χそれぞれp、
 、 13.とするとき、次の式が導出される。1.f
lち、 φ++ O++ ” P++θ、7・Pt−X、・P、
=θo ””” (+)φ、十〇2.・p、十〇6.・
p、−x、・P2−θ。・・・・−・ (2)ここで、
X、、X、はそれぞれ送Tn4線114.送亀線215
のインピーダンス、またθ。は負荷母線16のr)’l
l負角ある。また、送電線14.15の潮流Pl、P、
は次の関係がある。
Furthermore, in processing block 6, the power transmission line 11 is connected with the switches 16 and 17 logically set as 1 closed 1, as shown in the system configuration factor shown in FIG.
4 and sending fii1M215 and 7 flowing current χ p, respectively.
, 13. Then, the following formula is derived. 1. f
lchi, φ++ O++ ” P++θ, 7・Pt−X,・P,
=θo ””” (+)φ, 102.・p, 106.・
p, -x, ·P2-θ.・・・・・・−・ (2) Here,
X, ,X, are respectively the transmission Tn4 wires 114. Okuki Line 215
impedance, also θ. is r)'l of the load bus 16
l There is a negative angle. In addition, the power flows Pl, P of the power transmission line 14.15,
has the following relationship.

P、+ 1’、= o −・・・・・・・・・・・・・
・・・・(3)そこで(11、+21 、 (31式よ
り次0式が導出される。
P, + 1', = o -・・・・・・・・・・・・・
...(3) Then, (11, +21, (31), the following 0 formula is derived.

次に、負荷母/1113に対し、第6図に示した系統ソ
、′り成因のように更に単位負荷4与えた場合の送′1
F1線114、送電線215のそ1.ぞ几の潮流の変化
(it ’&ΔP、、JP、とし更に負荷母線16の位
相角の変化敬ンΔθ0とすると、次の式が導出される。
Next, for the load mother/1113, the transmission '1' when an additional unit load of 4 is given as shown in Fig. 6 as shown in Figure 6.
Part 1 of F1 line 114 and power transmission line 215. Assuming that the change in the power flow (it'& ΔP, JP) and the change in the phase angle of the load bus 16 Δθ0, the following equation is derived.

θ11・ΔP、十〇8.・ΔP2−X、・Δp、=Δθ
。 ・・・・・・ (5)θ7.・ΔP、+02.・Δ
P、−X、・Δp、=Δθ。 ・・・・・・ (6)Δ
P、+ΔP、=1.0 ・・・・・・・・・・・・ (
7)上記(51、(6) 、 (7)式より次式が導出
されろ。
θ11・ΔP, 108.・ΔP2−X, ・Δp, = Δθ
. ...... (5) θ7.・ΔP, +02.・Δ
P, -X, · Δp, = Δθ.・・・・・・(6)Δ
P, +ΔP, = 1.0 ・・・・・・・・・・・・ (
7) Derive the following equation from equations (51, (6), and (7) above).

処理ブロック4では、(4)式に於る潮流P、 、 P
2、位卯角θ。は次式Z解くことにより得ろ。
In processing block 4, the currents P, , P in equation (4) are
2. Orientation angle θ. Obtain by solving the following equation Z.

処理ブロック5では(8)式に於る潮流θ)変化計ii
 l’+ 。
In processing block 5, the power flow θ) change meter ii in equation (8)
l'+.

ΔP、Pt角の変化量Δθ0は次式ン解くことにより得
る。
The amount of change Δθ0 in the ΔP and Pt angles can be obtained by solving the following equation.

更に処理ブロック7では、処理ブロック4において(9
)式で与えら几た潮流P、、P、及び処理プロン1でめ
た中(s’L *荷潮流により、処理ブロック6でまる
1111力系統の潮流値ヶ4+’s iF、する。電力
系統の潮流の修正は、層目母線111に151シてまっ
ている中位負荷潮流にPlに乗じ、こf’Lχ処理ブロ
ック6でまっている電力系統の潮流値に加える。
Furthermore, in processing block 7, in processing block 4 (9
) The power flow P, , P given by the formula, and the load flow determined by processing block 1 (s'L *load flow), the power flow value of the 1111 power system in processing block 6 is 4+'s iF.Electric power To correct the power flow of the power system, the medium load power flow stored in the layer bus 111 is multiplied by Pl, and this is added to the power flow value of the power system stored in the f'Lχ processing block 6.

同様に、着目f)ガが212 tc関してもまっている
単f)r負荷潮流に11.χ乗じ、こオ]、タ電力系統
の潮流値に加えることにより行う。
Similarly, focus on the single f) r load current that f) is 212 tc. This is done by adding the power flow value of the electric power system.

次に処311!ブロック8では、処IJIブロック5に
オdいて(1(P式でめられた潮流変化数Δ1゛1.Δ
P2ケ用い、処理ブロック1でめた着目母線111、着
目母線212に対するそれぞれの中位負荷潮流χ修正し
、負荷母線131C対する中位負荷潮流ン求める。中位
負荷潮流の修正は、着目母線111に関してまっている
潮流の感度係数全てに対しΔP1乞乗じ、また着目1t
i:線212に関してはΔP2χ乗じることにより行う
Next place 311! In block 8, the processing IJI block 5 is added (1 (number of tidal current changes Δ1゛1.Δ
Using P2, the medium load power flow χ for the bus of interest 111 and the bus of interest 212 determined in processing block 1 is corrected, and the medium load power flow for the load bus 131C is determined. The correction of the medium load power flow is performed by multiplying all the sensitivity coefficients of the power flow for the target bus 111 by ΔP1, and by multiplying the target bus 111 by ΔP1.
i: Regarding the line 212, it is performed by multiplying by ΔP2χ.

処理ブロック9では、処理ブロック7でめた潮流及び処
理ブロック8でめた単6γ負荷潮流を用いて、着目母(
’1111、着目母線212より新たに供給し得る電力
最′JX:算出する。その際のOL電力量算出の方式は
以下の通りである。
In processing block 9, the mother of interest (
'1111, the maximum electric power that can be newly supplied from the target bus 212 'JX: Calculate. The method for calculating the OL power amount at that time is as follows.

電力系統において、各電力設備4流れる潮流(・i5着
目母線より新たに供給する電力用に比例し、第7図に示
すような相関関係がある。第7図中、Pは着目母線から
新たに供給する電力量χ、fmは甫。
In the power system, the power flow flowing through each power facility 4 (i5 is proportional to the power newly supplied from the bus of interest, and there is a correlation as shown in Figure 7. In Figure 7, P is the power flow newly supplied from the bus of interest. The amount of electric power χ and fm to be supplied is 甫.

力設備mヶ流れる潮流乞、flmは電力設備mの即位負
荷潮流ン、f m oは着目母線より新たに電カン供給
する前の電流設備mの潮流とする。この関係χ利用し、
健全な電力系統に過角荷乞発生させずに着目母線より負
荷系統に供給し得ろ重力計の最大値phr^X及び最小
値PMTNは次式によりめることができる。
It is assumed that the current flowing through the power equipment m, flm is the current load current of the power equipment m, and f m o is the power flow of the current equipment m before the electric power is newly supplied from the target bus. Using this relationship χ,
The maximum value phr^X and minimum value PMTN of the gravimeter that can be supplied to the load system from the target bus without causing excessive overload in a healthy power system can be determined by the following equation.

fl。〉0の時には、 f zm < 00時には、 PMAX = M I N (PMAX7X )PMI
N ” MAX (pH<sNm )η1 ここで、PMAXmは電力設備mが過負荷とならずに着
目fB線より新たに供給できる最大電力を−PMTNm
は電力設備だが過負荷とならずに着目母線より新たに供
給できる最小電力、またMAX G−・)はmvcつい
ての最大値、MIN(・−・)はmについての最小値、
さらにFmは電力設備mの設備容縫である。
fl. 〉0, f zm < 00, PMAX = M I N (PMAX7X) PMI
N ” MAX (pH<sNm) η1 Here, PMAXm is the maximum power that can be newly supplied from the focused fB line without overloading the power equipment m, -PMTNm
is the minimum power that can be newly supplied from the target bus without overloading the power equipment, and MAX G-・) is the maximum value for mvc, MIN(・-・) is the minimum value for m,
Furthermore, Fm is the equipment capacity of power equipment m.

上記処理を着目母線のそれぞれに対して行い、求められ
た最大電力の内で最小の値乞着目母線から供給できる最
大電力と、また1役小電力の内で最大の値ゲ供給できる
竜小雷1力とする。
The above process is performed for each of the target bus lines, and the maximum power that can be supplied from the target bus line is the lowest value among the maximum power obtained, and the highest value can be supplied among the small power units. 1 power.

上述の実施例では着目母線が2母線の場合ン説明したが
、着目母線が3母線以上であっても、同様の処理ン行う
事により、着目母線より新たに供給jろことかできろ電
力前ン求めることができる。
In the above embodiment, the case where there are two buses of interest is explained, but even if there are three or more buses of interest, by performing the same process, it is possible to newly supply power from the bus of interest. You can ask for it.

以上のように、この発明のr>Jll流出出方式よれば
、a2数の母線から新たに供給できる電力量の算出に関
して多(σ)演算前ン必要とする潮流計算は、“f!■
カン供給する母線が新た[漸目さILだ場合に行うだけ
でよく、また亀カン供給される母線が、電力を供給する
母線とつながった場合には、電カン供給する系統の潮流
値を、簡単な計算により修1F可能であるため、新たな
潮流計算は不要となる。
As described above, according to the r>Jll outflow method of the present invention, the power flow calculation that requires multiple (σ) calculations to calculate the amount of power that can be newly supplied from the bus of the a2 number is “f!■
This only needs to be done when the bus that supplies power is new [IL], and if the bus that is supplied with power is connected to the bus that supplies power, the power flow value of the system that supplies power is Since it can be repaired by simple calculations, new power flow calculations are not required.

上記のように潮流計算ン行う回数は応援系統にある着目
母線の数でよく、少ない潮流計算回数で電力系統に過負
荷を発生させずに、新たに供給できる電力量χ算出でき
、しかもどのような系統の形態であろうと算出可能であ
るという効果がある。
As mentioned above, the number of power flow calculations can be determined by the number of buses of interest in the support system, and with a small number of power flow calculations, it is possible to calculate the amount of new power χ that can be supplied without overloading the power system. This has the advantage that calculations can be made regardless of the form of the lineage.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は従来提案されている潮流算出方式χ示す処理ブ
ロック図、@2図はこの発明の一実施例による潮流算出
方式2示す処理ブロック図、第3図、第4図、第5図及
び第6図はいずれも第2図実施例の動作説明用に例示的
に示した電力系統の系統構成、第7図及び第8図は該電
力系統の特性図である。 1〜9・・・処理ブロック、11・・・着目母線1%1
2・・・着目母線2,16・・・負荷母線、14・・・
送電線l。 15・・・送電線2.16,17,18.19・・・開
閉器。 なお図中の同一符号は同一部分ン示す。 代 理 人 太 kA 増 雄 第 1 図 fR2図 手続補正書(自発) 特許庁長官殿 1、事件の表示 特願昭58−117510号2、発明
の名称 潮流算出方式 3、補正をする者 審査 5、補正の対象 (1)明細書の特許請求の範囲の潤 (2)明細書の発明の詳細な説明の欄 6、補正の内容 (1)別紙の通り特許請求の範囲を補正する。 (2)明細書第2頁第1θ行目「負荷量につき」とある
のを「負荷量が」と補正する。 (3)明細書第2頁第11行目「計測計算推定」とある
のを「計測、計算、推定」と補正する。 (4)明細書第5頁第18行目「第3図は」とあるのを
「第3図の」と補正する。 (5)明細書第8頁第9行目「θ0は」とあるのを「θ
0を」と補正する。 (6)明細書第8頁第14行目「Δθ0は」とあるのを
「Δθ0を」と補正する。 (7)明細書第9頁第3行目「潮流の修正は」とあるの
を「潮流値の修正は」と補正する。 (8)明細書第9頁第15行目「潮流の感度係数」とあ
るのを「単位負荷潮流」と補正する。 補正後の特許請求の範囲 潮流状態が既知の電力系統に過負荷を発生させずに上記
系統内の特定の複数母線から上記系統外の負荷に対し取
り出せる電力量を算出する潮流算出方式において、上記
母線毎に単位負荷を与えると共に他の母線の発電量及び
負荷量を全て零に設定を−て、直流フロー法により算出
した複数の潮流計算の演算結果を用いて、上記各母線と
負荷に接続する母線とを継いだ場合の潮流状態をめ、続
いて上記負荷に接続する母線に単位負荷を継いだ場合の
潮流状態をめ、上記負荷に接続する母線より取り出せる
電力量を算出することを特徴とする潮流算出方式。
FIG. 1 is a processing block diagram showing a conventionally proposed power flow calculation method χ, FIG. 2 is a processing block diagram showing a power flow calculation method 2 according to an embodiment of the present invention, FIGS. 3, 4, 5, and 6 is a system configuration of a power system illustratively shown for explaining the operation of the embodiment in FIG. 2, and FIGS. 7 and 8 are characteristic diagrams of the power system. 1 to 9...processing block, 11...target generatrix 1%1
2... Focus bus 2, 16... Load bus, 14...
Power transmission line l. 15...Power transmission line 2.16, 17, 18.19...Switch. Note that the same reference numerals in the figures indicate the same parts. Agent Tai kA Masuo No. 1 Figure fR2 Procedural amendment (voluntary) Commissioner of the Japan Patent Office 1, Indication of case Japanese Patent Application No. 117510/1982 2, Invention name trend calculation method 3, Examination of the person making the amendment 5 , Subject of amendment (1) Explanation of the scope of claims in the specification (2) Column 6 of detailed explanation of the invention in the specification, Contents of amendment (1) Amend the scope of claims as shown in the attached sheet. (2) On page 2 of the specification, line 1θ, the phrase "per load amount" is corrected to read "by load amount." (3) In the 11th line of page 2 of the specification, "measurement, calculation, estimation" should be corrected to "measurement, calculation, estimation." (4) On page 5, line 18 of the specification, the phrase "Fig. 3 is" is amended to read "Fig. 3." (5) On page 8, line 9 of the specification, "θ0 is" should be replaced with "θ0".
Correct it as "0". (6) On page 8, line 14 of the specification, "Δθ0 is" is corrected to "Δθ0". (7) In the third line of page 9 of the specification, the phrase "correction of tidal current" is amended to "correction of tidal current value." (8) On page 9, line 15 of the specification, "sensitivity coefficient of power flow" is corrected to "unit load power flow." Claims after amendment: In a power flow calculation method that calculates the amount of power that can be extracted from a specific plurality of buses in the power system to a load outside the power system without overloading a power system in which the power flow state is known, By giving a unit load to each bus and setting all the power generation and load amounts of other buses to zero, connect the above buses and loads using the results of multiple power flow calculations calculated using the DC flow method. It is characterized by calculating the amount of power that can be taken out from the bus connected to the load by determining the power flow state when the unit load is connected to the bus connected to the load, and then calculating the power flow state when the unit load is connected to the bus connected to the load. A power flow calculation method.

Claims (1)

【特許請求の範囲】[Claims] 潮流状態が既知の電力系統に過負荷を発生させずに上記
系統内の特定の複数母線から上記系統外の負荷に対し取
り出せる電力量を算出する潮流算出方式において、上記
母線毎に単位負荷を与えると共に他の母線の発電量及び
負荷量を全て零に設定して、直流フロー法により算出し
た複数の潮流計算の演算結果ヶ用いて、上記各母線と負
荷に接続する母線とを継いた場合の潮流状態Z求め、続
いて上記負荷に接続する母線に単位負荷Y継いた場合の
潮流状態をめ、上記負荷に接続する母線より取り出せる
電力量を算出することを特徴とする潮流算出方式。 ・
In a power flow calculation method that calculates the amount of power that can be extracted from specific multiple buses within the system to loads outside the system without overloading the power system with known power flow conditions, a unit load is given to each bus. At the same time, the power generation amount and load amount of other buses are all set to zero, and the calculation results of multiple power flow calculations calculated by the DC flow method are used to calculate the case where each of the above buses and the bus connected to the load are connected. A power flow calculation method characterized in that the power flow state Z is determined, and then the power flow state when a unit load Y is connected to the bus connected to the load is calculated, and the amount of power that can be taken out from the bus connected to the load is calculated.・
JP58117510A 1983-06-27 1983-06-27 Tide calculating system Pending JPS609331A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58117510A JPS609331A (en) 1983-06-27 1983-06-27 Tide calculating system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58117510A JPS609331A (en) 1983-06-27 1983-06-27 Tide calculating system

Publications (1)

Publication Number Publication Date
JPS609331A true JPS609331A (en) 1985-01-18

Family

ID=14713541

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58117510A Pending JPS609331A (en) 1983-06-27 1983-06-27 Tide calculating system

Country Status (1)

Country Link
JP (1) JPS609331A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5826924A (en) * 1981-08-11 1983-02-17 Mitsubishi Electric Corp Air quantity controller for boiler
JPS5893987A (en) * 1981-11-27 1983-06-03 Kureha Chem Ind Co Ltd Method of controlling blast amount of blower

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5826924A (en) * 1981-08-11 1983-02-17 Mitsubishi Electric Corp Air quantity controller for boiler
JPS5893987A (en) * 1981-11-27 1983-06-03 Kureha Chem Ind Co Ltd Method of controlling blast amount of blower

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