Formative time-lag studies with high-frequency discharges

1954 ◽  
Vol 101 (74) ◽  
pp. 407-408
Author(s):  
A.W. Bright ◽  
H.C. Huang
2020 ◽  
Vol 11 (3) ◽  
pp. 319-339
Author(s):  
Francisco Hernandez ◽  
Xihong Zhang ◽  
Hong Hao

This article conducts a comparative study on the effectiveness of ventilation to mitigate blasting effects on spherical chambers subjected to internal detonations of high explosives through finite element analysis using the software package AUTODYN. Numerical simulations show that ventilation is ineffective in mitigating the damage of spherical chambers subjected to internal high explosives explosions because the chamber response is mainly described by high-frequency membrane modes. Openings do not reduce the chamber response despite they can reduce the blast overpressure after the chamber reaches its peak response. Worse still, openings lead to stress concentration, which weakens the structure. Therefore, small openings may reduce the capacity of the chamber to resist internal explosions. In addition, because large shock waves impose the chamber to respond to a reverberation frequency associated with the re-reflected shock wave pulses, secondary re-reflected shock waves can govern the chamber response, and plastic/elastic resonance can occur to the chamber. Simulations show that the time lag between the first and the second shock wave ranges from 3 to 7 times the arrival time of the first shock wave, implying that the current simplified design approach should be revised. The response of chambers subjected to eccentric detonations is also studied. Results show that due to asymmetric explosions, other membrane modes may govern the chamber response and causes localized damage, implying that ventilation is also ineffective to mitigate the damage of spherical chambers subjected to eccentric detonations.


Previous investigators, when measuring the electric strength of hydrocarbon liquids with short-duration rectangular pulses, have assumed that the statistical component of the breakdown time was insignificant com pared with the formative time. In the present investigation, however, the time to breakdown was measured directly by the use of step-function pulses, and clear evidence for a statistical time lag was found. The formative time was ~ 0.1 us, being less than that given by previous estimates. A statistical interpretation of short-pulse measurements is presented and this provides a consistent explanation of the results of other workers. Furthermore, by using an experimentally derived equation for the variation of the mean rate of breakdown f ( E ) with applied stress E , it has been shown that the form of the relationship between strength and pulse duration obtained by other workers agrees with that obtained by a statistical analysis. Experiments on air-saturated n -hexane with both short-duration and step-function pulses support the statistical ideas presented and indicate that electrode conditions are extremely important. It was found that strength and time to breakdown were affected by the number of breakdown measurements on a sample. Experiments with gas-free n -hexane and non-uniform fields have demonstrated the importance of air content when long duration pulses are used. It was found that, although the statistical time lag was insignificant, formative time lags as long as 10 ys occurred with a point cathode-sphere anode configuration.


2013 ◽  
pp. 251-258
Author(s):  
W. Pfeiffer ◽  
P. Völker
Keyword(s):  
Time Lag ◽  

An image converter and a 4-stage image intensifier have been used to investigate the development of spark breakdown in a 3-cm, uniform-field, gas-discharge gap. The growth of ionization, initiated by a burst of electrons a t the cathode, has been observed for overvoltages up to 25 % in nitrogen, oxygen and sulphur hexafluoride a t pressures in the range 13 to 40kPa (100 to 300 Torr). In nitrogen, time resolved shutter and streak records have been obtained which demonstrate, that, at low overvoltages, breakdown is preceded by the formation of a diffuse glow discharge whereas, at voltages well in excess of the static breakdown voltage, the arc discharge is formed directly in the track of the initial electron avalanche, as a result of space-charge distortion of the applied electric field. This change with overvoltage has previously been ascribed to a transition from a Townsend to a streamer breakdown mechanism; the present results, however, do not entirely support this view. In oxygen and sulphur hexafluoride, no such change in the form of ionization development has been observed and it is concluded from the evidence obtained that, even a t very small overvoltages, the development of ionization is strongly affected by space-charge distortion of the applied field. Photographs obtained in sulphur hexafluoride have been correlated with measured formative-time-lag data showing the time-lag-free region reported previously by Kuffel. Some conclusions have been drawn regarding the breakdown mechanism under these conditions.


1979 ◽  
Vol 18 (11) ◽  
pp. 2187-2188 ◽  
Author(s):  
Kiichiro Kagawa ◽  
Hiroyuki Kobayashi ◽  
Masuo Ishikane
Keyword(s):  
Time Lag ◽  

A study was made of electrical breakdown of a liquid (hexachlorodiphenyl) the viscosity of which is very dependent on temperature. It is shown that in uniform fields breakdown results from formation and growth of a vapour bubble in the liquid. This was established by direct microscopic observations of the ‘breakdown event’ at room temperature and by measurements of times to breakdown as the viscosity was changed by five orders of magnitude between room temperature and 56.5 °C. When the time of voltage application is too short for the vapour bubble to grow to its critical size then the breakdown strength is higher than that obtained under direct voltages. Under 10/50 μs impulses the breakdown strength of hexachlorodiphenyl at room temperature was 5 MV/cm. It is suggested that vaporization was initiated by development of points of zero pressure in the liquid. Assuming that, in an electric field, development of points of zero pressure resulted from the presence of submicroscopic particle impurities in the liquid, a simple expression was derived for the onset of vaporization. It is shown that this expression gives good predictions for the known dependences of breakdown strength of n -hexane on both temperature and pressure and for the variation of breakdown strength of aliphatic hydrocarbons with molecular weight. It is further shown that the time required for a vapour bubble in n -hexane to grow to the size at which breakdown occurs is comparable with the experimentally measured formative time lag.


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