JP2008067437A - Load current calculation method and load current calculation device - Google Patents

Load current calculation method and load current calculation device Download PDF

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JP2008067437A
JP2008067437A JP2006240143A JP2006240143A JP2008067437A JP 2008067437 A JP2008067437 A JP 2008067437A JP 2006240143 A JP2006240143 A JP 2006240143A JP 2006240143 A JP2006240143 A JP 2006240143A JP 2008067437 A JP2008067437 A JP 2008067437A
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current
distribution line
load
load current
outlet
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JP5000952B2 (en
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Hidehisa Baba
秀央 馬場
Koji Tsubone
浩二 坪根
Satoru Arikata
悟 有方
Hiroshi Inoue
汎 井上
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Chugoku Electric Power Co Inc
Hitachi Ltd
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Hitachi Ltd
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/70Smart grids as climate change mitigation technology in the energy generation sector
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y04INFORMATION OR COMMUNICATION TECHNOLOGIES HAVING AN IMPACT ON OTHER TECHNOLOGY AREAS
    • Y04SSYSTEMS INTEGRATING TECHNOLOGIES RELATED TO POWER NETWORK OPERATION, COMMUNICATION OR INFORMATION TECHNOLOGIES FOR IMPROVING THE ELECTRICAL POWER GENERATION, TRANSMISSION, DISTRIBUTION, MANAGEMENT OR USAGE, i.e. SMART GRIDS
    • Y04S10/00Systems supporting electrical power generation, transmission or distribution
    • Y04S10/12Monitoring or controlling equipment for energy generation units, e.g. distributed energy generation [DER] or load-side generation

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Abstract

<P>PROBLEM TO BE SOLVED: To eliminate an error caused by a difference between the power factor of an outlet current and that of a power source current in calculating a load current in a distribution line. <P>SOLUTION: A load current calculation device 1 is made up of an outlet current obtaining means 2, a power source current obtaining means 3, a load current calculation means 4, and a load current output means 5. The outlet current obtaining means 2 obtains the values of currents (an active current and a reactive current) that flow in an outlet, a portion where electric power from a feeder connected to a transformer is received, in the distribution line. The power source current obtaining means 3 obtains the values of currents (an active current and a reactive current) supplied by distributed power sources (power sources such as a generator) connected to the distribution line. The load current calculation means 4 calculates a value of the load current of the distribution line by vector operation from the values of the outlet current obtained by the outlet current obtaining means 2 and those of the currents of the distributed power sources obtained by the power source current obtaining means 3. The load current output means 5 outputs the load currents of the distribution line calculated by the load current calculation means 4. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

本発明は、配電線の引出し口の電流及び電源の発電電流から配電線の負荷電流を計算する負荷電流計算方法及び負荷電流計算装置に関する。   The present invention relates to a load current calculation method and a load current calculation device for calculating a load current of a distribution line from a current at an outlet of the distribution line and a generated current of a power source.

従来、配電線の負荷電流(以下、配電線負荷電流という)を求める場合に、配電線の引出し口の電流(以下、引出し口電流という)と、分散型電源の発電電流(以下、分散型電源電流という)との合計値を計算し、当該合計値を各区間に按分していた。特許文献1には、当該計算を行う配電線の区間負荷算出装置が開示されている。
特開2003−61247号公報
Conventionally, when calculating the load current of the distribution line (hereinafter referred to as distribution line load current), the current at the outlet of the distribution line (hereinafter referred to as drawer current) and the generated current of the distributed power source (hereinafter referred to as distributed power source) The current value) and the total value was apportioned to each section. Patent Document 1 discloses a section load calculation device for a distribution line that performs the calculation.
JP 2003-61247 A

しかしながら、昨今、マイクロガスタービンなどの分散型電源の普及に伴って、配電線に接続される分散型電源の台数が増加する傾向にある。そして、引出し口電流の力率と、分散型電源電流の力率とが大きく異なる場合もあるため、計算した配電線負荷電流に誤差が生じるという問題がある。   However, with the recent spread of distributed power sources such as micro gas turbines, the number of distributed power sources connected to distribution lines tends to increase. And since there is a case where the power factor of the outlet current and the power factor of the distributed power source current are greatly different, there is a problem that an error occurs in the calculated distribution line load current.

本発明は、上記課題を鑑みてなされたものであり、配電線負荷電流を計算する上で、引出し口電流の力率と、電源電流の力率との相違による誤差をなくすことを主たる目的とする。   The present invention has been made in view of the above problems, and in calculating the distribution line load current, the main object is to eliminate errors due to the difference between the power factor of the outlet current and the power factor of the power source current. To do.

上記課題を解決するために、本発明は、装置により配電線の負荷電流を計算する負荷電流計算方法であって、前記装置が、前記配電線の引出し口の有効電流及び無効電流を取得する第1のステップと、前記装置が、前記配電線に接続された1以上の電源の有効電流及び無効電流を取得する第2のステップと、前記装置が、前記第1のステップで取得した前記引出し口の有効電流及び無効電流と、前記第2のステップで取得した電源の有効電流及び無効電流とから、ベクトル演算により前記配電線の負荷の有効電流及び無効電流を計算する第3のステップと、前記装置が、前記第3のステップで計算した前記配電線の負荷の有効電流及び無効電流を出力する第4のステップとを含むことを特徴とする。   In order to solve the above-mentioned problems, the present invention provides a load current calculation method for calculating a load current of a distribution line by an apparatus, wherein the apparatus acquires an effective current and a reactive current of an outlet of the distribution line. 1 step, a second step in which the device acquires effective current and reactive current of one or more power supplies connected to the distribution line, and the drawer in which the device has acquired in the first step. A third step of calculating the effective current and reactive current of the load of the distribution line by vector calculation from the active current and reactive current of the power source and the active current and reactive current of the power source acquired in the second step; The apparatus includes a fourth step of outputting an effective current and a reactive current of the load of the distribution line calculated in the third step.

この方法によれば、配電線の引出し口の電流と、配電線に接続された電源の電流とから、配電線の負荷の電流を計算する場合に、スカラー演算ではなく、ベクトル演算を用いるので、引出し口の電流の力率と、電源の電流の力率とが異なっていても、配電線の負荷の電流を正しく求めることができる。   According to this method, when calculating the load current of the distribution line from the current of the outlet of the distribution line and the current of the power source connected to the distribution line, vector calculation is used instead of scalar calculation. Even if the power factor of the current at the outlet differs from the power factor of the power source current, the load current of the distribution line can be obtained correctly.

また、本発明は、負荷電流計算装置であって、配電線の引出し口の有効電流及び無効電流を取得する引出し口電流取得手段と、前記配電線に接続された1以上の電源の有効電流及び無効電流を取得する電源電流取得手段と、前記引出し口電流取得手段が取得した前記引出し口の有効電流及び無効電流と、前記電源電流取得手段が取得した電源の有効電流及び無効電流とから、ベクトル演算により前記配電線の負荷の有効電流及び無効電流を計算する負荷電流計算手段と、前記負荷電流計算手段が計算した前記配電線の負荷の有効電流及び無効電流を出力する負荷電流出力手段とを含んで構成されることを特徴とする。   Further, the present invention is a load current calculation device, wherein the outlet current acquisition means for acquiring the effective current and reactive current of the outlet of the distribution line, the effective current of one or more power sources connected to the distribution line, and A power source current acquisition unit that acquires a reactive current, an effective current and a reactive current of the extraction port acquired by the extraction port current acquisition unit, and a power source effective current and a reactive current acquired by the power source current acquisition unit, and a vector Load current calculation means for calculating the effective current and reactive current of the load of the distribution line by calculation, and load current output means for outputting the effective current and reactive current of the load of the distribution line calculated by the load current calculation means It is characterized by comprising.

この構成によれば、配電線の引出し口の電流と、配電線に接続された電源の電流とから、配電線の負荷の電流を計算する場合に、スカラー演算ではなく、ベクトル演算を用いるので、引出し口の電流の力率と、電源の電流の力率とが異なっていても、配電線の負荷の電流を正しく求めることができる。   According to this configuration, when calculating the load current of the distribution line from the current of the outlet of the distribution line and the current of the power source connected to the distribution line, vector calculation is used instead of scalar calculation. Even if the power factor of the current at the outlet differs from the power factor of the power source current, the load current of the distribution line can be obtained correctly.

その他、本願が開示する課題およびその解決方法は、発明を実施するための最良の形態の欄、及び図面により明らかにされる。   In addition, the problems disclosed in the present application and the solutions thereof will be clarified by the description of the best mode for carrying out the invention and the drawings.

本発明によれば、配電線負荷電流を計算する上で、引出し口電流の力率と、分散型電源電流の力率との相違による誤差をなくすことができる。   According to the present invention, in calculating the distribution line load current, it is possible to eliminate an error due to the difference between the power factor of the outlet current and the power factor of the distributed power source current.

以下、図面を参照しながら、本発明を実施するための最良の形態を説明する。本発明の実施の形態に係る負荷電流計算装置は、配電線の各区間において電圧の位相のずれがないとみなすことにより、配電線の引出し口の電流と、分散型電源の発電電流とから、ベクトル演算により配電線の負荷電流を計算し、出力する装置である。   Hereinafter, the best mode for carrying out the present invention will be described with reference to the drawings. The load current calculation device according to the embodiment of the present invention assumes that there is no phase shift of the voltage in each section of the distribution line, and from the current at the outlet of the distribution line and the generated current of the distributed power source, It is a device that calculates and outputs the load current of the distribution line by vector calculation.

≪装置の構成と動作≫
図1は、負荷電流計算装置の構成例を示す図である。負荷電流計算装置1は、引出し口電流取得手段2、電源電流取得手段3、負荷電流計算手段4及び負荷電流出力手段5を含んで構成される。
≪Device configuration and operation≫
FIG. 1 is a diagram illustrating a configuration example of a load current calculation apparatus. The load current calculation device 1 includes an outlet current acquisition unit 2, a power supply current acquisition unit 3, a load current calculation unit 4, and a load current output unit 5.

引出し口電流取得手段2は、配電線において、変圧器に接続されたフィーダから電力の供給を受ける部分である引出し口を流れる電流(有効電流及び無効電流)の値を取得する。具体的には、引出し口又はその近傍に設置された電流計から直接取得してもよいし、当該電流計を見た電力会社の担当者が入力操作したデータを取得してもよい。電源電流取得手段3は、配電線に接続された分散型電源(発電機などの電源)が供給する電流(有効電流及び無効電流)の値を取得する。具体的には、分散型電源又はその近傍に設置された電流計から直接取得してもよいし、当該電流計を見た電力会社の担当者が入力操作したデータを取得してもよい。引出し口電流取得手段2及び電源電流取得手段3は、電流計から電流値を取得するインタフェース又は負荷電流計算装置1が備えるキーボードやマウスなどの入力機器によって実現される。   The outlet current acquisition means 2 acquires the value of current (effective current and reactive current) flowing through the outlet that is a part that receives power supply from a feeder connected to the transformer in the distribution line. Specifically, it may be acquired directly from an ammeter installed at or near the outlet, or data input by a person in charge of the electric power company who saw the ammeter may be acquired. The power source current acquisition unit 3 acquires values of currents (active current and reactive current) supplied by a distributed power source (power source such as a generator) connected to the distribution line. Specifically, it may be acquired directly from a distributed power source or an ammeter installed in the vicinity thereof, or data input by a person in charge of an electric power company who viewed the ammeter may be acquired. The outlet current acquisition means 2 and the power supply current acquisition means 3 are realized by an interface for acquiring a current value from an ammeter or an input device such as a keyboard or a mouse provided in the load current calculation device 1.

負荷電流計算手段4は、引出し口電流取得手段2が取得した引出し口電流の値と、電源電流取得手段3が取得した分散型電源電流の値とから、ベクトル演算により配電線負荷電流の値を計算する。各電流は、有効電流及び無効電流からなり、それぞれを加算することによってベクトル演算ができる。詳細は後記する。負荷電流計算手段4は、CPU(Central Processing Unit)によるプログラムの実行又はハードウェアとしての演算回路の動作によって実現される。負荷電流出力手段5は、負荷電流演算手段4が計算した配電線負荷電流を出力する。具体的には、負荷電流計算装置1が備えるディスプレイに表示してもよいし、ネットワークやその他のインタフェースを介して別の装置に出力してもよい。   The load current calculation unit 4 calculates the distribution line load current value by vector calculation from the value of the extraction port current acquired by the extraction port current acquisition unit 2 and the value of the distributed power supply current acquired by the power supply current acquisition unit 3. calculate. Each current includes an active current and a reactive current, and a vector operation can be performed by adding the currents. Details will be described later. The load current calculation means 4 is realized by execution of a program by a CPU (Central Processing Unit) or operation of an arithmetic circuit as hardware. The load current output means 5 outputs the distribution line load current calculated by the load current calculation means 4. Specifically, it may be displayed on a display provided in the load current calculation device 1 or may be output to another device via a network or other interface.

図2は、負荷電流計算手段4が行うベクトル演算を説明する図である。図2(a)は、配電線の構成例を示す。配電線Lは、引出し口F、開閉器A1及びA2により、区間S1、S2及びS3に区切られている。配電線Lの区間S2には、発電機(電源)Gが接続されている。引出し口Fを流れる電流は、ベクトルIFCBで示され、発電機Gから供給される電流は、ベクトルIGで示される。そして、配電線Lの区間S3を流れる負荷電流は、ベクトルILで示される。なお、図2(a)では発電機Gが1つ示されているが、これに限定されることなく、2以上の電源が配電線Lに接続されていてもよい。   FIG. 2 is a diagram for explaining the vector calculation performed by the load current calculation means 4. Fig.2 (a) shows the structural example of a distribution line. The distribution line L is divided into sections S1, S2, and S3 by the outlet F and the switches A1 and A2. A generator (power source) G is connected to the section S2 of the distribution line L. The current flowing through the outlet F is indicated by a vector IFCB, and the current supplied from the generator G is indicated by a vector IG. And the load current which flows through area S3 of the distribution line L is shown by vector IL. 2A shows one generator G, the present invention is not limited to this, and two or more power sources may be connected to the distribution line L.

図2(b)は、電流ベクトルの演算を示す。従来、配電線負荷電流ILの大きさを、次の式1のように計算していた。
|IL|=|IFCB|+|IG| ・・・式1
FIG. 2B shows the calculation of the current vector. Conventionally, the magnitude of the distribution line load current IL has been calculated as in the following Expression 1.
| IL | = | IFCB | + | IG |

式1は、スカラー和を求めるものであり、引出し口電流IFCBの力率と、分散型電源電流IGの力率とが同じである、すなわち、図2(b)におけるベクトルIFCBの傾きと、ベクトルIGの傾きとが同じである場合には、問題なく利用できる。ところが、電流の力率、すなわち、ベクトルの傾きが異なる場合には、式1によって求めた配電線負荷電流ILの大きさは、誤差を含んだ値になる。   Equation 1 is to obtain a scalar sum, and the power factor of the extraction port current IFCB and the power factor of the distributed power source current IG are the same, that is, the slope of the vector IFCB in FIG. When the inclination of IG is the same, it can be used without any problem. However, when the power factor of the current, that is, the gradient of the vector is different, the magnitude of the distribution line load current IL obtained by Expression 1 becomes a value including an error.

そこで、本発明の実施の形態では、配電線負荷電流ILの大きさを、次の式2のように計算する。
|IL|=|IFCB+IG| ・・・式2
Therefore, in the embodiment of the present invention, the magnitude of the distribution line load current IL is calculated as the following Expression 2.
| IL | = | IFCB + IG |

式2は、ベクトル和を求めた後、その大きさを計算するものである。各ベクトルの有効電流の大きさを添え字rにより示し、無効電流の大きさを添え字iにより示し、虚数単位をjとすれば、配電線負荷電流ILの大きさは、式3のように求められる。
IFCB=IFCBr+j・IFCBi
IG =IGr +j・IGi
|IL|=|IFCBr+IGr+j・(IFCBi+IGi)|
=√{(IFCBr+IGr)+(IFCBi+IGi)} ・・・式3
Equation 2 calculates the magnitude after obtaining the vector sum. If the magnitude of the active current of each vector is indicated by the subscript r, the magnitude of the reactive current is indicated by the subscript i, and the imaginary unit is j, the magnitude of the distribution line load current IL is as shown in Equation 3. Desired.
IFCB = IFCBr + j · IFCBi
IG = IGr + j · IGi
| IL | = | IFCBr + IGr + j · (IFCBi + IGi) |
= √ {(IFCBr + IGr) 2 + (IFCBi + IGi) 2 } Equation 3

なお、負荷電流出力手段5は、ベクトルIL(有効電流及び無効電流)を出力してもよし、ベクトルILの大きさ|IL|を出力してもよい。負荷電流出力手段5がベクトルILを出力するか、その大きさ|IL|を出力するかは、負荷電流出力手段5から出力を受ける側の当該出力データの使い方によって適宜変更可能である。   Note that the load current output means 5 may output a vector IL (effective current and reactive current), or may output the magnitude | IL | of the vector IL. Whether the load current output means 5 outputs the vector IL or the magnitude | IL | can be appropriately changed depending on how the output data on the side receiving the output from the load current output means 5 is used.

≪計算方法の効果≫
負荷電流計算装置1の負荷電流計算手段4が、従来スカラー演算していた配電線負荷電流を、ベクトル演算することにより、引出し口の電流の力率と、電源の電流の力率との相違が考慮されるので、精度よく計算することができる。これによれば、停電時の負荷融通において、従来は融通不可と判断されたとしても、融通可能と判断できる場合がある。そして、配電線の負荷を精度よく計算することによって、電圧計算を精度よく行うことができる。以下、そのような効果について、具体例を用いて説明する。
≪Effect of calculation method≫
The load current calculation means 4 of the load current calculation device 1 performs vector calculation on the distribution line load current, which has been conventionally scalar calculation, so that the difference between the power factor of the outlet current and the power factor of the power source current can be reduced. Since it is taken into consideration, it is possible to calculate with high accuracy. According to this, in the case of load accommodation at the time of a power failure, even if it is conventionally determined that accommodation is not possible, it may be determined that accommodation is possible. And voltage calculation can be performed accurately by calculating the load of a distribution line accurately. Hereinafter, such an effect will be described using a specific example.

<停電時の負荷融通の例>
図3は、停電時の負荷融通の例を示す図である。配電線L1は、引出し口F1、開閉器A1及びA2により、区間S1、S2及びS3に区切られている。配電線L1の区間S3には、発電機(電源)G1が接続されている。一方、配電線L2は、引出し口F2、開閉器A3及びA4により、区間S4、S5及びS6に区切られている。配電線L2の区間S6には、発電機(電源)G2が接続されている。また、配電線L1の区間S3と、配電線L2の区間S6とは、開閉器A5によって接続されている。
<Examples of load accommodation during power outages>
FIG. 3 is a diagram illustrating an example of load accommodation during a power failure. The distribution line L1 is divided into sections S1, S2, and S3 by the outlet F1 and the switches A1 and A2. A generator (power source) G1 is connected to the section S3 of the distribution line L1. On the other hand, the distribution line L2 is divided into sections S4, S5, and S6 by the outlet F2 and the switches A3 and A4. A generator (power source) G2 is connected to the section S6 of the distribution line L2. The section S3 of the distribution line L1 and the section S6 of the distribution line L2 are connected by a switch A5.

ここで、図3に示す配電系統において、配電線L1の区間S2で停電作業するために、区間S3の電力を配電線L2から融通する場合を考える。停電前の配電線L1、L2の引出し口電流を100+j20[A]とし、発電機G1、G2の発電電流を30−j10[A]とする。この場合、配電線負荷電流は、配電線L1、L2ともに130+j10[A]となる。従来の計算方法では、引出し口電流が102.0(=√(100+20))[A]、発電機電流が31.6(=√(30+10))[A]となり、スカラー和により配電線負荷電流は133.6[A]となる。 Here, in the distribution system shown in FIG. 3, in order to perform a power failure operation in the section S2 of the distribution line L1, consider the case where the power in the section S3 is interchanged from the distribution line L2. The outlet current of the distribution lines L1 and L2 before the power failure is 100 + j20 [A], and the generated current of the generators G1 and G2 is 30-j10 [A]. In this case, the distribution line load current is 130 + j10 [A] for both the distribution lines L1 and L2. In the conventional calculation method, the outlet current is 102.0 (= √ (100 2 +20 2 )) [A], and the generator current is 31.6 (= √ (30 2 +10 2 )) [A]. The sum of the distribution line load current is 133.6 [A].

配電線L1、L2の区間負荷比率を、区間S1:区間S2:区間S3=区間S4:区間S5:区間S6=0:1:1とする。この場合、配電線L2から融通すべき電流値は(130+j10)÷2=65+j5[A]であり、融通後の配電線L2の引出し口電流は、|130+j10+65+j5|=√(195+15)=195.6[A]となる。従来の計算方法では、配電線L2から融通すべき電流値は133.6÷2=66.8[A]であり、融通後の配電線L2の引出し口電流は、133.6+66.8=200.4[A]となる。 The section load ratio of the distribution lines L1 and L2 is set to section S1: section S2: section S3 = section S4: section S5: section S6 = 0: 1: 1. In this case, the current value to be accommodated from the distribution line L2 is (130 + j10) / 2 = 65 + j5 [A], and the outlet current of the distribution line L2 after accommodation is | 130 + j10 + 65 + j5 | = √ (195 2 +15 2 ) = 195.6 [A]. In the conventional calculation method, the current value to be accommodated from the distribution line L2 is 133.6 / 2 = 66.8 [A], and the outlet current of the distribution line L2 after the interchange is 133.6 + 66.8 = 200. 4 [A].

配電線L2の引出し口電流の上限値が200[A]であった場合、従来の計算方法では200.4>200となって融通不可であると判断されたが、本発明の実施の形態では195.6<200となって融通可能であると判断され、より効率よく配電系統を運用することが可能になる。なお、配電線L2から配電線L1の区間S3に電力の融通を受ける場合には、区間S3に接続された発電機G1及び区間S6に接続された発電機G2は解列(停止)するので、融通後の引出し口電流は、発電機G1及び発電機G2がが解列された状態で計算している。   In the case where the upper limit value of the outlet current of the distribution line L2 is 200 [A], it has been determined that 200.4> 200 in the conventional calculation method and the interchange is impossible, but in the embodiment of the present invention, Since 195.6 <200, it is determined that the system can be accommodated, and the power distribution system can be operated more efficiently. In addition, when receiving power interchange from the distribution line L2 to the section S3 of the distribution line L1, the generator G1 connected to the section S3 and the generator G2 connected to the section S6 are disconnected (stopped). The outlet current after accommodation is calculated in a state where the generator G1 and the generator G2 are disconnected.

<電圧判定の例その1>
図4は、電圧降下を計算して、電圧が融通できるか否かを判定する(電圧判定の例)を示す図である。配電線L1、L2の構成は、図3と同様である。ただし、発電機G1、G2は、解列状態であるとされ、図示されていない。この場合、電圧降下は、次の式4により表される。
ΔV≒I(Rcosθ+Xsinθ)×√3 ・・・式4
(R:インピーダンスの抵抗成分、
X:インピーダンスのリアクタンス成分、
cosθ:負荷力率)
<Example of voltage determination 1>
FIG. 4 is a diagram illustrating calculation of a voltage drop to determine whether or not the voltage can be accommodated (an example of voltage determination). The configurations of the distribution lines L1 and L2 are the same as those in FIG. However, the generators G1 and G2 are assumed to be in a disconnected state and are not illustrated. In this case, the voltage drop is expressed by the following equation 4.
ΔV≈I (R cos θ + X sin θ) × √3 Equation 4
(R: resistance component of impedance,
X: reactance component of impedance,
cos θ: load power factor)

本例では、配電線の各区間のインピーダンスをR+jX=0.5+j1.5[Ω]として融通時(発電機解列状態)の電圧降下を計算する。また、負荷力率は配電線ごとに定義されており、0.99として計算する。   In this example, assuming that the impedance of each section of the distribution line is R + jX = 0.5 + j1.5 [Ω], the voltage drop at the time of interchange (generator disconnected state) is calculated. The load power factor is defined for each distribution line and is calculated as 0.99.

従来の計算方法では、次のようになる。区間S4の電圧降下は、200.4×(0.5×0.99+1.5×0.14)×√3=244.7[V]になる。区間S5の電圧降下は、(200.4+133.6)/2×(0.5×0.99+1.5×0.14)×√3=203.9[V]になる。区間S6の電圧降下は、(133.6+66.8)/2×(0.5×0.99+1.5×0.14)×√3=122.4[V]になる。区間S3の電圧降下は、66.8/2×(0.5×0.99+1.5×0.14)×√3=40.8[V]になる。全体での電圧降下は、244.7+203.9+122.4+40.8=611.8[V]になる。送電端電圧を6700[V]とすると、末端の電圧は、6700−611.8=6088.2[V]となる。   The conventional calculation method is as follows. The voltage drop in the section S4 is 200.4 × (0.5 × 0.99 + 1.5 × 0.14) × √3 = 244.7 [V]. The voltage drop in the section S5 is (200.4 + 133.6) / 2 × (0.5 × 0.99 + 1.5 × 0.14) × √3 = 203.9 [V]. The voltage drop in the section S6 is (133.6 + 66.8) / 2 × (0.5 × 0.99 + 1.5 × 0.14) × √3 = 12.4 [V]. The voltage drop in the section S3 is 66.8 / 2 × (0.5 × 0.99 + 1.5 × 0.14) × √3 = 40.8 [V]. The overall voltage drop is 244.7 + 203.9 + 122.4 + 40.8 = 611.8 [V]. When the power transmission terminal voltage is 6700 [V], the terminal voltage is 6700−611.8 = 6088.2 [V].

本発明の実施の形態に係る計算方法では、次のようになる。区間S4の平均区間電流は|195+j15|=195.6[A]になり、電圧降下は195.6×(0.5×0.99+1.5×0.14)×√3=238.8[V]になる。区間S5の平均区間電流は|(195+j15+130+j10)/2|=163.0[A]になり、電圧降下は163.0×(0.5×0.99+1.5×0.14)×√3=199.0[V]になる。区間S6の平均区間電流は|(130+j10+65+j5)/2|=97.8[A]になり、電圧降下は97.8×(0.5×0.99+1.5×0.14)×√3=119.4[V]になる。区間3の平均区間電流は|(65+j5)/2|=32.6になり、電圧降下は32.6×(0.5×0.99+1.5×0.14)×√3=39.8[V]になる。全体での電圧降下は、238.8+199.0+119.4+39.8=597.0[V]となる。送電端電圧を6700[V]とすると、末端の電圧は、6700−597.0=6103.0[V]となる。   The calculation method according to the embodiment of the present invention is as follows. The average current of the section S4 is | 195 + j15 | = 195.6 [A], and the voltage drop is 195.6 × (0.5 × 0.99 + 1.5 × 0.14) × √3 = 23.88 [ V]. The average section current in section S5 is | (195 + j15 + 130 + j10) /2|=163.0 [A], and the voltage drop is 163.0 × (0.5 × 0.99 + 1.5 × 0.14) × √3 = It becomes 199.0 [V]. The average section current in section S6 is | (130 + j10 + 65 + j5) /2|=97.8 [A], and the voltage drop is 97.8 × (0.5 × 0.99 + 1.5 × 0.14) × √3 = 119.4 [V]. The average section current of section 3 is | (65 + j5) /2|=32.6, and the voltage drop is 32.6 × (0.5 × 0.99 + 1.5 × 0.14) × √3 = 39.8. [V]. The overall voltage drop is 238.8 + 199.0 + 119.4 + 39.8 = 597.0 [V]. When the power transmission terminal voltage is 6700 [V], the terminal voltage is 6700−597.0 = 6103.0 [V].

これによれば、6103.0>6088.2であり、本発明の実施の形態に係る計算方法の結果は従来の計算方法の結果に比べて電圧降下が小さく、末端の電圧が高くなるので、従来の計算方法では電圧降下が大きく、末端の電圧が低くて融通不可であったとしても、本発明の実施の形態に係る計算方法では融通可能であると判断できる場合がある。   According to this, since 6103.0> 6088.2, the result of the calculation method according to the embodiment of the present invention has a smaller voltage drop and a higher terminal voltage than the result of the conventional calculation method. Even if the conventional calculation method has a large voltage drop and the terminal voltage is low and cannot be accommodated, it may be determined that the calculation method according to the embodiment of the present invention is interchangeable.

<電圧判定の例その2>
前記電圧判定の例その1では、電圧降下をスカラー演算していたが、これをベクトル演算することによって、さらに精度を上げることができる。この場合、電圧降下は、次の式5により表される。

Figure 2008067437
<Example 2 of voltage determination>
In the first voltage determination example, the voltage drop is scalar-calculated, but the accuracy can be further improved by performing a vector operation on the voltage drop. In this case, the voltage drop is expressed by the following Equation 5.
Figure 2008067437

本発明の実施の形態に係る計算方法では、次のようになる。区間S4の電圧降下は、195.6×{(0.5×0.99+1.5×0.14)+j(1.5×0.99−0.5×0.14)}×√3=238.8+j479.4[V]となる。区間5の電圧降下は、163.0×{(0.5×0.99+1.5×0.14)+j(1.5×0.99−0.5×0.14)}×√3=199.0+j399.5[V]となる。区間6の電圧降下は、97.8×{(0.5×0.99+1.5×0.14)+j(1.5×0.99−0.5×0.14)}×√3=119.4+j239.7[V]となる。区間3の電圧降下は、32.6×{(0.5×0.99+1.5×0.14)+j(1.5×0.99−0.5×0.14)}×√3=39.8+j79.9[V]となる。   The calculation method according to the embodiment of the present invention is as follows. The voltage drop in the section S4 is 195.6 × {(0.5 × 0.99 + 1.5 × 0.14) + j (1.5 × 0.99−0.5 × 0.14)} × √3 = 238.8 + j479.4 [V]. The voltage drop in section 5 is 163.0 × {(0.5 × 0.99 + 1.5 × 0.14) + j (1.5 × 0.99−0.5 × 0.14)} × √3 = It becomes 199.0 + j399.5 [V]. The voltage drop of the section 6 is 97.8 × {(0.5 × 0.99 + 1.5 × 0.14) + j (1.5 × 0.99−0.5 × 0.14)} × √3 = 119.4 + j239.7 [V]. The voltage drop in section 3 is 32.6 × {(0.5 × 0.99 + 1.5 × 0.14) + j (1.5 × 0.99−0.5 × 0.14)} × √3 = 39.8 + j79.9 [V].

全体での電圧降下は、以上のベクトル和であり、597.0+j1198.5となる。送電端電圧を6700[V]とすると、末端の電圧は、|6700−597.0−j1198.5|=6219.6[V]となる。   The overall voltage drop is the above vector sum, which is 597.0 + j118.5. When the power transmission end voltage is 6700 [V], the terminal voltage is | 6700-597.0-j118.5 | = 6219.6 [V].

以上説明した計算方法の効果によれば、短期的には停電を減少させることができ、長期的には停電の対策費用を抑制することができる。   According to the effect of the calculation method described above, the power outage can be reduced in the short term, and the countermeasure cost for the power outage can be suppressed in the long term.

以上説明した本発明の実施の形態によれば、負荷電流計算装置1の負荷電流計算手段4が、引出し口電流と、分散型電源電流とから配電線負荷電流を計算するにあたって、引出し口電流の力率及び電源電流の力率を考慮して、電流の合計値をベクトル演算で求めることによって、引出し口電流の力率と、分散型電源電流の力率とが大きく異なる場合であっても、配電線負荷電流を正しく求めることができる。配電線負荷電流が正しく分かれば電圧降下も正しく分かるので、当該電圧降下の値に基づいて電力供給の可否を判断する場合にも、ベクトル演算を有効に適用することができる。すなわち、従来スカラー演算により配電線負荷電流を求めていた場合には、配電線負荷電流を過大評価した結果、必要な電力供給ができないと判断していたところ、本発明の実施の形態ではベクトル演算により配電線負荷電流を正確に評価することによって電力供給ができるという判断が可能になる。   According to the embodiment of the present invention described above, when the load current calculation unit 4 of the load current calculation device 1 calculates the distribution line load current from the extraction port current and the distributed power source current, Considering the power factor and the power factor of the power source current, by calculating the total value of the current by vector calculation, even if the power factor of the outlet current and the power factor of the distributed power source current are significantly different, Distribution line load current can be obtained correctly. If the distribution line load current is correctly known, the voltage drop can be correctly understood. Therefore, the vector calculation can be effectively applied even when determining whether or not power supply is possible based on the value of the voltage drop. In other words, when the distribution line load current is obtained by scalar calculation in the past, it has been determined that the necessary power supply cannot be performed as a result of overestimation of the distribution line load current. Thus, it is possible to determine that power can be supplied by accurately evaluating the distribution line load current.

また、本発明の実施の形態を、電圧の位相のずれを考慮した厳密な計算方法(AC法潮流計算など)と比較すると、配電線の各区間において電圧の位相のずれがないとみなすことにより簡単な計算で配電線負荷電流を求めるので、プログラミングや演算回路の設計が容易にでき、メモリなどの資源が少なくて済む。従って、これを実現する装置(負荷電流計算装置1)を簡単な構成にすることができ、計算処理を高速に行うことができる。これによれば、停電作業などのために電力を融通する場合に、迅速に対応することができる。   In addition, when the embodiment of the present invention is compared with a strict calculation method (AC method power flow calculation or the like) considering the voltage phase shift, it is assumed that there is no voltage phase shift in each section of the distribution line. Since the distribution line load current is obtained by simple calculation, programming and arithmetic circuit design can be easily performed, and resources such as memory can be reduced. Therefore, the apparatus (load current calculation apparatus 1) for realizing this can be configured simply and the calculation process can be performed at high speed. According to this, when power is interchanged for power outage work, etc., it can respond quickly.

以上、本発明を実施するための最良の形態について説明したが、上記実施の形態は本発明の理解を容易にするためのものであり、本発明を限定して解釈するためのものではない。本発明はその趣旨を逸脱することなく変更、改良され得るとともに、本発明にはその等価物も含まれる。   Although the best mode for carrying out the present invention has been described above, the above embodiment is intended to facilitate understanding of the present invention and is not intended to limit the present invention. The present invention can be changed and improved without departing from the gist thereof, and equivalents thereof are also included in the present invention.

本発明の実施の形態に係る負荷電流計算装置の構成例を示す図である。It is a figure which shows the structural example of the load current calculation apparatus which concerns on embodiment of this invention. 負荷電流計算装置の負荷電流計算手段が行うベクトル演算を説明する図であり、(a)は配電線の構成例を示し、(b)は電流ベクトルの演算を示す。It is a figure explaining the vector calculation which the load current calculation means of a load current calculation apparatus performs, (a) shows the example of a structure of a distribution line, (b) shows the calculation of a current vector. 停電時の負荷融通の例を示す図である。It is a figure which shows the example of the load accommodation at the time of a power failure. 電圧判定の例を示す図である。It is a figure which shows the example of voltage determination.

符号の説明Explanation of symbols

1 負荷電流計算装置
2 引出し口電流取得手段
3 電源電流取得手段
4 負荷電流計算手段
5 負荷電流出力手段
L、L1、L2 配電線
G、G1、G2 発電機(電源)
DESCRIPTION OF SYMBOLS 1 Load current calculation apparatus 2 Drawer outlet current acquisition means 3 Power supply current acquisition means 4 Load current calculation means 5 Load current output means L, L1, L2 Distribution line G, G1, G2 Generator (power supply)

Claims (2)

装置により配電線の負荷電流を計算する負荷電流計算方法であって、
前記装置が、前記配電線の引出し口の有効電流及び無効電流を取得する第1のステップと、
前記装置が、前記配電線に接続された1以上の電源の有効電流及び無効電流を取得する第2のステップと、
前記装置が、前記第1のステップで取得した前記引出し口の有効電流及び無効電流と、前記第2のステップで取得した電源の有効電流及び無効電流とから、ベクトル演算により前記配電線の負荷の有効電流及び無効電流を計算する第3のステップと、
前記装置が、前記第3のステップで計算した前記配電線の負荷の有効電流及び無効電流を出力する第4のステップと、
を含むことを特徴とする負荷電流計算方法。
A load current calculation method for calculating a load current of a distribution line by a device,
A first step in which the apparatus obtains an effective current and a reactive current of the outlet of the distribution line;
A second step in which the apparatus obtains active and reactive currents of one or more power supplies connected to the distribution line;
From the effective current and reactive current of the outlet acquired in the first step and the effective current and reactive current of the power source acquired in the second step, the device calculates the load of the distribution line by vector calculation. A third step of calculating active and reactive currents;
A fourth step in which the device outputs an effective current and a reactive current of the load of the distribution line calculated in the third step;
The load current calculation method characterized by including.
配電線の引出し口の有効電流及び無効電流を取得する引出し口電流取得手段と、
前記配電線に接続された1以上の電源の有効電流及び無効電流を取得する電源電流取得手段と、
前記引出し口電流取得手段が取得した前記引出し口の有効電流及び無効電流と、前記電源電流取得手段が取得した電源の有効電流及び無効電流とから、ベクトル演算により前記配電線の負荷の有効電流及び無効電流を計算する負荷電流計算手段と、
前記負荷電流計算手段が計算した前記配電線の負荷の有効電流及び無効電流を出力する負荷電流出力手段と、
を含んで構成されることを特徴とする負荷電流計算装置。
An outlet current acquisition means for acquiring an effective current and a reactive current of the outlet of the distribution line;
Power supply current acquisition means for acquiring effective current and reactive current of one or more power supplies connected to the distribution line;
From the effective current and reactive current of the outlet acquired by the outlet current acquisition means and the effective current and reactive current of the power source acquired by the power supply current acquisition means, the effective current of the load of the distribution line and Load current calculation means for calculating reactive current;
Load current output means for outputting effective current and reactive current of the load of the distribution line calculated by the load current calculating means;
A load current calculation device comprising:
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