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IEC BS EN 60909-0 Currents during two separate sim

三相交流系统中的短路电流 第0部分:电流计算

IEC BS EN 60909-0 Currents during two separate simultaneous line-to-earth short circuits and partial short-circuit currents flowing through earth

Short-circuit currents in three-phase a.c. systems Part 0: Calculation of currents

版本年份 2001 文件语言 英语 全文 6 页 格式 PDF
IEC BS EN 60909-0 Currents during two separate sim 三相交流系统中的短路电流 第0部分:电流计算封面

标准信息

STANDARD INFORMATION
标准编号
IEC BS EN 60909-0 Currents during two separate sim
所属分类
IEC 国际电工标准
发布机构
BSI
版本年份
2001
文件语言
英语
文件格式
PDF
文件页数
6 页
文件大小
5.33 MB

中文名称为参考译名,文件语言以原文为准。

· 更新:

标准简介

OVERVIEW

中文简介

该标准规定了低压和高压三相交流系统(50Hz或60Hz)中短路电流的计算方法。它建立了一种通用、实用且简洁的计算程序,通过引入短路点处的等效电压源,计算对称和非对称短路情况下的预期短路电流、峰值短路电流及直流分量等参数。

English summary

This standard specifies the calculation of short-circuit currents in low-voltage and high-voltage three-phase a.c. systems operating at 50 Hz or 60 Hz. It establishes a general, practicable, and concise procedure using an equivalent voltage source at the short-circuit location to determine prospective short-circuit currents, peak currents, and DC components for both balanced and unbalanced faults.

以上为根据文件整理的内容简介。

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IEC BS EN 60909-0 Currents during two separate simPDF 第 1 页 · 原页码 1

1.3 Definitions

For the purposes of this part of IEC 60909, the definitions given in IEC 60050(131) and the following definitions apply.

1.3.1 short circuit

accidental or intentional conductive path between two or more conductive parts forcing the electric potential differences between these conductive parts to be equal or close to zero

1.3.1.1 line-to-line short circuit

accidental or intentional conductive path between two or more line conductors with or without earth connection

1.3.1.2 line-to-earth short circuit

accidental or intentional conductive path in a solidly earthed neutral system or an impedance earthed neutral system between a line conductor and local earth

1.3.2 short-circuit current

over-current resulting from a short circuit in an electric system

NOTE It is necessary to distinguish between the short-circuit current at the short-circuit location and partial short-circuit currents in the network branches (see figure 3) at any point of the network.

1.3.3 prospective (available) short-circuit current

current that would flow if the short circuit were replaced by an ideal connection of negligible impedance without any change of the supply (see note of 1.1)

1.3.4 symmetrical short-circuit current

r.m.s. value of the a.c. symmetrical component of a prospective (available) short-circuit current (see 1.3.3), the aperiodic component of current, if any, being neglected

1.3.5 initial symmetrical short-circuit current Ik

r.m.s. value of the a.c. symmetrical component of a prospective (available) short-circuit current (see 1.3.3), applicable at the instant of short circuit if the impedance remains at zero-time value (see figures 1 and 2)

1.3.6 initial symmetrical short-circuit power Sk

fictitious value determined as a product of the initial symmetrical short-circuit current Ik (see 1.3.5), the nominal system voltage Un (see 1.3.13) and the factor √3: Sk = √3 Un Ik

NOTE The initial symmetrical short-circuit power Sk is not used for the calculation procedure in this standard. If Sk is used in spite of this in connection with short-circuit calculations, for instance to calculate the internal impedance of a network feeder at the connection point Q, then the definition given should be used in the following form: SkQ = √3 UnQ IkQ or ZQ = cUnQ² / SkQ.

1.3.7 decaying (aperiodic) component id.c. of short-circuit current

mean value between the top and bottom envelope of a short-circuit current decaying from an initial value to zero according to figures 1 and 2

1.3.8 peak short-circuit current ip

maximum possible instantaneous value of the prospective (available) short-circuit current (see figures 1 and 2)

NOTE The magnitude of the peak short-circuit current varies in accordance with the moment at which the short circuit occurs. The calculation of the three-phase peak short-circuit current ip applies to the line conductor and to the instant at which the greatest possible short-circuit current exists. Sequential short circuits are not considered.

1.3.9 symmetrical short-circuit breaking current Ib

r.m.s. value of an integral cycle of the symmetrical a.c. component of the prospective short-circuit current at the instant of contact separation of the first pole to open of a switching device

1.3.10 steady-state short-circuit current Ik

r.m.s. value of the short-circuit current which remains after the decay of the transient phenomena (see figures 1 and 2)

1) To be published.

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