TY - JOUR
T1 - Positive and negative streamers in ambient air: measuring diameter, velocity and dissipated energy
AU - Briels, T.M.P.
AU - Kos, J.
AU - Winands, G.J.J.
AU - Veldhuizen, van, E.M.
AU - Ebert, U.M.
PY - 2008
Y1 - 2008
N2 - Positive and negative streamers are studied in ambient air at 1 bar; they emerge from a needle electrode placed 40mm above a planar electrode. The amplitudes of the applied voltage pulses range from 5 to 96 kV; most pulses have rise times of 30 ns or shorter. Diameters, velocities and energies of the streamers are measured. Two regimes are identified; a low voltage regime where only positive streamers appear and a high voltage regime where both positive and negative streamers exist. Below 5 kV, no streamers emerge. In the range from 5 to 40 kV, positive streamers form, while the negative discharges only form a glowing cloud at the electrode tip, but no streamers. For 5–20 kV, diameters and velocities of the positive streamers have the minimal values of d = 0.2mm and v ˜ 105 ms-1. For 20–40 kV, their diameters increase by a factor of 6 while the voltage increases only by a factor of 2. Above the transition value of 40 kV, streamers of both polarities form; they strongly resemble each other, though the positive ones propagate further; their diameters continue to increase with applied voltage.
For 96 kV, positive streamers attain diameters of 3mm and velocities of 4 × 106 ms-1;
negative streamers are about 20% slower and thinner. An empirical fit formula for the relation between velocity v and diameter d is v = 0.5d2 mm-1 ns-1 for both polarities. Streamers of both polarities dissipate energies of the order of several millijoules per streamer while crossing the gap.
AB - Positive and negative streamers are studied in ambient air at 1 bar; they emerge from a needle electrode placed 40mm above a planar electrode. The amplitudes of the applied voltage pulses range from 5 to 96 kV; most pulses have rise times of 30 ns or shorter. Diameters, velocities and energies of the streamers are measured. Two regimes are identified; a low voltage regime where only positive streamers appear and a high voltage regime where both positive and negative streamers exist. Below 5 kV, no streamers emerge. In the range from 5 to 40 kV, positive streamers form, while the negative discharges only form a glowing cloud at the electrode tip, but no streamers. For 5–20 kV, diameters and velocities of the positive streamers have the minimal values of d = 0.2mm and v ˜ 105 ms-1. For 20–40 kV, their diameters increase by a factor of 6 while the voltage increases only by a factor of 2. Above the transition value of 40 kV, streamers of both polarities form; they strongly resemble each other, though the positive ones propagate further; their diameters continue to increase with applied voltage.
For 96 kV, positive streamers attain diameters of 3mm and velocities of 4 × 106 ms-1;
negative streamers are about 20% slower and thinner. An empirical fit formula for the relation between velocity v and diameter d is v = 0.5d2 mm-1 ns-1 for both polarities. Streamers of both polarities dissipate energies of the order of several millijoules per streamer while crossing the gap.
U2 - 10.1088/0022-3727/41/23/234004
DO - 10.1088/0022-3727/41/23/234004
M3 - Article
SN - 0022-3727
VL - 41
SP - 234004-1/11
JO - Journal of Physics D: Applied Physics
JF - Journal of Physics D: Applied Physics
IS - 23
ER -