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Research topics

1. Fundamental research of atmospheric pressure plasmas
    1.1. Introduction
    1.2. Diagnostic methods
    1.3. Numerical modeling
    1.4. DC glow discharge
    1.5. Transient spark
    1.6. Microwave plasma
    1.7. Discharges in porous materials and capillaries
    1.8. Discharges with water
2. Bio-medical plasma applications
3. Environmental plasma applications
4. Non-plasmatic environmental technologies

1.5. Transient spark

Repetitively pulsed discharge in air is a power reduction strategy based on pulsed electron heating. Pulsed power is a very effective way of producing non-thermal plasmas at low energy costs. However, costly pulsed power generators able to produce ns-rise time pulses of several kV with frequencies of 10-100 kHz are needed. We therefore investigated an interesting pulsed discharge generated by a cheap DC power supply. This novel streamer-to-spark transition discharge with short strong current pulses (named Spontaneously Pulsing Transition Discharge, SPTD, or Transient Spark, TS) generates very active non-equilibrium (cold) plasma.

When a DC high voltage of a few kV is applied to the point electrode of a non-uniform field gap, streamer corona appears. It is typical with small current pulses of streamers (~10 mA) with a repetitive frequency of 10-30 kHz, during which the discharge voltage remains fairly constant. As the voltage is further increased, the streamers establish a conductive channel that leads to a spark formation with excessive current pulse (Fig. 1).

a)

b)

Fig. 1. Photograph of TS in needle - water gap 4 mm long (a). Typical voltage and current waveforms of TS (b).
 

In our case, the spark pulse current is limited in by 1) the ballast resistor R that drops the voltage as the current increases, and 2) the capacity C between the electrodes that is small (order of 10 pF). Thus, even if the sparks forms, it is only transient since the discharged energy is small (~0.1-1 mJ), that is why we call this discharge transient spark. After the pulse, C is recharged by a growing potential on the stressed electrode. As soon as C is charged enough again, it triggers a new pulse. This transient spark becomes then a repetitive streamer-to-spark transition discharge, with each spark pulse (~1 A) preceded by one or a sequence of streamer pulses. The repetitive frequency of pulses is 0.5-5 kHz, and increases with the growing applied voltage. Thanks to the very short spark pulse duration (~100 ns) given by the small C and a limiting R, the plasma remains cold.

By setting the values of R and C (C can be set by the length of the HV cable or by filtering C_cable + C_probe by a small resistor put very near the high voltage electrode, Fig. 2) we can either obtain the transient spark pulses and regulate their amplitude, or obtain a continuous discharge. This pulse-less DC glow discharge typically appears after the spark pulse if R ≤ 1 MΩ and so the voltage drops to a certain small value but not zero, high enough though to sustain a small current (~mA).

Fig. 2. Schematic of the electrical circuit of transient spark.
 

The TS has already been successfully tested for several environmental and bio-medical applications (see sections 2. Bio-medical plasma applications and 3. Environmental plasma applications ), and extensive fundamental research of TS using several electrical and optical diagnostic methods has been performed (see subsection 1.2. Diagnostic methods).

More details in:

Old website of our division.

In 2022 we organised 9th Central European symposium on Plasma Chemistry and COST Action CA19110 workshop.

In 2016 we organised 6th International Conference on Plasma Medicine, with almost 400 participants.

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