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Reaction of surge protection devices on overvoltage signals with different steepness

The result's identifiers

  • Result code in IS VaVaI

    <a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F49777513%3A23220%2F16%3A43928843" target="_blank" >RIV/49777513:23220/16:43928843 - isvavai.cz</a>

  • Result on the web

    <a href="http://ieeexplore.ieee.org/document/7521734/" target="_blank" >http://ieeexplore.ieee.org/document/7521734/</a>

  • DOI - Digital Object Identifier

    <a href="http://dx.doi.org/10.1109/EPE.2016.7521734" target="_blank" >10.1109/EPE.2016.7521734</a>

Alternative languages

  • Result language

    angličtina

  • Original language name

    Reaction of surge protection devices on overvoltage signals with different steepness

  • Original language description

    Surge protection devices are designed and tested for an overvoltage limitation that can appear on the power line at a direct lightning strike to the power lines or a near strike because of an inductive coupling. This lightning pulse is characterized by a great destructive power. The comparison of operation of different overvoltage protections by this surge voltage stress can be found in scientific publications. This paper is focused on analysing the behavior of elements of the overvoltage protection, by the different stress voltage than the surge impulse. Modern protection devices act fast enough to eliminate or at least suppress pulses shorter than lightning or switching pulses. The first type of such a signal is EFT - Electrical Fast Transient (Burst signal). The Burst Signal simulates surges generated in the network during fast switching operations. It is characterized by a great steepness and a high repetition rate. The energy of these pulses isn't usually high enough to destroy the equipment, but they can easily disturb the internal useful signals. Another type of overvoltage pulse is very fast and dangerous and can be formed directly by electrical appliances. This is an electrostatic discharge (ESD). The electrostatic discharge is often generated by touching the casing of the device. ESD can get through the inductive and capacitive coupling to the power circuits of the device or by a direct physical touching to the uncapped power wire. ESD achieves high levels of voltage at low pulse energy. All these signals were applied to a gas discharge tube, metal oxide varistors, bipolar and unipolar TVS diodes. Their behavior was evaluated by passing the test signals, specifically the current flowing through the protection device to the ground, the residual voltage and the reaction time to the test signal. The time dependence of these variables was recorded using an oscilloscope.

  • Czech name

  • Czech description

Classification

  • Type

    D - Article in proceedings

  • CEP classification

    JE - Non-nuclear power engineering, energy consumption and utilization

  • OECD FORD branch

Result continuities

  • Project

  • Continuities

    S - Specificky vyzkum na vysokych skolach

Others

  • Publication year

    2016

  • Confidentiality

    S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů

Data specific for result type

  • Article name in the collection

    Proceedings of the 2016 17th International Scientific Conference on Electric Power Engineering (EPE)

  • ISBN

    978-1-5090-0907-7

  • ISSN

  • e-ISSN

  • Number of pages

    5

  • Pages from-to

    311-315

  • Publisher name

    Czech Technical University in Prague

  • Place of publication

    Prague

  • Event location

    Praha, Česká republika

  • Event date

    May 16, 2016

  • Type of event by nationality

    WRD - Celosvětová akce

  • UT code for WoS article

    000382934600020