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I. INTRODUCTION
Une protection efficace contre les surtensions est essentielle pour garantir un fonctionnement fiable et ininterrompu des réseaux électriques basse tension modernes qui intègrent des équipements électriques et électroniques sensibles. Les dispositifs de protection contre les surtensions (SPD) sont installés dans les systèmes d'alimentation CA qui intègrent des composants de différents matériaux et technologies, tels que des varistances à oxyde métallique, des éclateurs et des tubes à décharge de gaz. En fait, la technologie des éclateurs est couramment utilisée dans les SPD et les systèmes en Europe, grâce à la capacité des éclateurs à (i) gérer les courants de surtension à haute teneur énergétique, (ii) présenter un courant de fuite nul et (iii) interrompre efficacement le courant de suivi de fréquence du réseau électrique après un fonctionnement réussi.
Bien que des travaux approfondis aient été menés sur le comportement transitoire des SPD à éclateurs, en mettant l'accent sur l'interruption du courant de suivi à fréquence industrielle, le temps de réponse des éclateurs est rarement étudié et discuté dans la littérature. De plus, la norme UL1449 et la prochaine norme IEC61643-01 ne définissent pas le temps de réponse des SPD ; une analyse intéressante sur le temps de réponse des SPD a été fournie dans , couvrant cependant uniquement la technologie des varistances.
Cette étude se concentre sur la réponse transitoire des SPD qui intègrent la technologie des éclateurs à étincelle. Le temps de réponse des SPD à éclateurs à étincelle disponibles dans le commerce, généralement installés dans les tableaux principaux des systèmes d'alimentation en courant alternatif (tension nominale : 230/400 V), est étudié en utilisant des tensions d'impulsion de foudre et de commutation. Ainsi, le comportement impulsionnel des SPD est étudié pour une large gamme d'événements de surtension auxquels ils peuvent être exposés sur le terrain dans le cas de transitoires à front rapide et de commutation. Les résultats expérimentaux sont analysés et l'effet de la forme d'onde de tension d'impulsion appliquée est discuté.
II. DISPOSITIF EXPÉRIMENTAL
Le dispositif testé (DUT) est un dispositif de protection contre les surtensions (SPD) à commutation de tension utilisant des éclateurs à étincelles déclenchés entre les lignes électriques et la terre. Il convient de mentionner que le SPD adopte une configuration de connexion de type 1 selon la norme IEC 61643-12, qui est applicable aux systèmes TN-C triphasés (230/400 V). La figure 1 illustre le schéma de la configuration des composants de protection contre les surtensions intégrés dans le DUT disponible dans le commerce avec un temps de réponse déclaré < 100 ns et un niveau de protection de 1500 V ; ces valeurs nominales sont généralement revendiquées par les fabricants de SPD 230 V.
The response time of the SPD was determined by employing lightning and switching impulse voltages of 1.2/50μs and 250/2500μs waveforms, respectively; 5 hits of positive and 5 hits of negative voltage polarity, were applied to the DUT. Experiments were conducted at the High Voltage Laboratory of the Aristotle University of Thessaloniki, Greece. This experimental investigation is important when considering that the sparkover voltage-time curve of spark gap is statistical in nature (spread δU, δt in Fig. 2) and highly dependent on the steepness of the applied voltage (Fig. 2); this sparkover behavior is inherent in spark gap technology.
Fig. 3 shows the single-stage impulse voltage generator (140kV/ 245J), with interchangeable components, that was used to stress the line to earth protection mode of the SPD (L-PEN). The voltage at SPD terminals was monitored by a high voltage probe Tektronix P6015A and the discharge current was measured by using a Pearson 310 current transformer both connected to a Tektronix ΤDS 3064B digital oscilloscope (600 MHz, 10 GS/s). Both voltage and current data were acquired via connecting the digital oscilloscope to a personal computer through a KUSB-488B adapter enabling live data monitoring.
III. RESULTS AND DISCUSSION
For the purpose of this work, the response time of spark gap-based surge protective devices (SPDs) is defined as the time duration that the overvoltage at SPD terminals attains values that threaten the safe operation of protected equipment. A schematic representation of the proposed definition is given in Fig. 4. It is suggested that the “clock” starts counting the response time at the time instant that the voltage exceeds a threshold value, that is, the temporary overvoltage peak of 630 V (√3 ∙ 255 ∙√2), that may originate due to LV-system faults per IEC 61643-11, up to the time instant that the overvoltage is mitigated to values lower than the half of the sparkover voltage peak.
A. Lightning Impulse Voltage Tests
Standard lightning impulse voltages up to 17kV have been used to study the transient response of SPDs against lightning-related overvoltages.
Figs. 5a and 5b depict the open circuit impulse voltage of 6kV, 1.2/50 μs, and the corresponding typical voltage record at the SPD terminals (L-PEN), respectively. The voltage at the SPD terminals increases up to the sparkover of the spark gap (~1450 V) and then, due to the sudden change of the SPD impedance, a discharge current flows resulting in a residual voltage of ~1000V associated with the relatively low current flow from the impulse voltage generator; the response time of the SPD is estimated as ~70ns, in line with the declared response time (< 100ns) by the manufacturer.
Fig. 6 shows the experimentally derived variation of the mean response time of the SPD as a function of the impulse voltage peak. It is evident that the response time of the SPD decreases with increasing impulse voltage peak. It must be noted that for impulse voltages with a peak lower than ~4000 V, the response time is longer than the value of 100ns, which is the upper limit declared by the SPD manufacturer. Thus, lightning impulse voltage tests with a peak lower than the standard value of 6000V, 1.2/50μs, as specified by IEC 61643-11 [15] and UL 1449, shall be integrated into updated standards to evaluate the response of SPDs realistically. Longer response times, although associated with lower sparkover voltages (Fig. 7), may impose a high risk of failure of sensitive equipment. The reason behind this is that the destructive effect on equipment can be attributed not only to the peak overvoltage but also to the duration of the overvoltage that affects the specific energy stressing the protected equipment . It is noteworthy that lightning impulse voltage tests with peak values higher than 6 kV, as suggested by IEC and UL , may result in sparkover voltages exceeding the declared protection level of the SPD.
B. Switching Impulse Voltage Tests
Standard switching impulse voltages up to 17kV have been used to study the transient response of SPDs against switching transients. Figs. 8a and 8b depict the open circuit impulse voltage of 6kV, 250/2500 μs, and the corresponding typical voltage and current record at the SPD (L-PEN), respectively. The voltage at the SPD terminals increases up to the sparkover of the spark gap followed by a sudden drop of the SPD impedance, which is associated with a response time of ~3000ns! The significantly longer response times than the commonly declared value of 100 ns (i) call for further investigations on the performance of the trigger circuit (component T in Fig. 1) of spark gaps under overvoltages with a low rate of rise and (ii) question the technical value of the declared response time by manufacturers in case of switching transients.
Fig. 9 shows the experimentally derived variation of the mean response time of the SPD as a function of the switching impulse voltage peak. Obviously, there is a sharp decrease in the response time of the SPD with increasing switching impulse voltage peak, but the response time is always at least an order higher than the declared response time of 100 ns. It must be noted that these long response times are associated with relatively low sparkover voltages that attain values in the range of ~850-1000 V (Fig. 10), which even though they are certainly below the declared protection level of 1500 V they may still be harmful to sensitive equipment in case of prolonged duration. These experimental findings on long response times, which are well beyond the response time declared by manufacturers, stress the need for a new category of the response time of SPDs against switching transients; the latter may occur in power systems and the response time of the SPDs against slowly rising overvoltages can be a critical protection parameter.
It should be mentioned that results of this work regarding the response time are not only related to the spark gap technology but can be also directly associated with other switching and combination type SPDs employing air gaps and gas discharge tubes.
IV. CONCLUSIONS
The response time of surge protective devices employing triggered spark gap technology has been experimentally investigated by employing lightning and switching impulse voltage tests. Experimental results have shown that the response time of spark gap-based surge protective devices declared by manufacturers, that is typically 100 ns, is dubious in the case of fast-front transients and is certainly exceeded in the case of switching transients. These findings stress the need for an update of forthcoming standards to include a strict definition of the response time of surge protective devices; this amendment will resolve issues associated with manufacturers' subjective declaration of response time in the surge protection industry.