Streamer discharge


A streamer discharge, also known as filamentary discharge, is a type of transient electrical discharge which forms at the surface of a conductive electrode carrying a high voltage in an insulating medium such as air. Streamers are luminous writhing branching sparks, plasma channels composed of ionized air molecules, which repeatedly strike out from the electrode into the air.
Like the related corona discharges and brush discharges, a streamer discharge represents a region around a high voltage conductor where the air has suffered electrical breakdown and become conductive, so electric charge is leaking off the electrode into the air. It occurs when the electric field at the surface of a conductor exceeds the dielectric strength of air, around 30 kilovolts per centimeter. When the electric field created by the applied voltage reaches this threshold, accelerated electrons strike air molecules with enough energy to knock other electrons off them, ionizing them, and the freed electrons go on to strike more molecules in a chain reaction. These electron avalanches create ionized, electrically conductive regions in the air near the electrode. The space charge created by the electron avalanches gives rise to an additional electric field, causing the ionized region to grow at its ends, forming a finger-like discharge called a streamer.
Streamers are transient and filamentary, which makes them different from corona discharges. They are used in applications such as ozone production, air purification or plasma medicine. If a streamer reaches the opposite polarity conductor it creates an ionized conductive path through which a large current can flow, releasing a large amount of heat, resulting in an electric arc; this is the process through which lightning leaders create a path for lightning bolts. Streamers can also be observed as sprites in the upper atmosphere. Due to the low pressure, sprites are much larger than streamers at ground pressure, see the [|similarity laws] below.

History

The theory of streamer discharges was preceded by John Sealy Townsend's discharge theory
from around 1900.
However, it became clear that this theory was sometimes inconsistent with observations.
This was especially true for discharges that were longer or at higher pressure.
In 1939, Loeb
and Raether
independently described a new type of discharge, based on their experimental observations.
Shortly thereafter, in 1940, Meek presented the theory of spark discharge,
which quantitatively explained the formation of a self-propagating streamer.
This new theory of streamer discharges successfully explained the experimental observations.

Applications

Streamers are used in applications such as ozone generation, air purification and plasma-assisted combustion.
An important property is that the plasma they generate is strongly non-equilibrium: the electrons have much higher energies than the ions.
Therefore, chemical reactions can be triggered in a gas without heating it.
This is important for plasma medicine, where "plasma bullets", or guided streamers, can be used for wound treatment, although this is still experimental.

Streamer physics

Streamers can emerge when a strong electric field is applied to an insulating material, typically a gas. Streamers can only form in areas where the electric field exceeds the dielectric strength of the medium. For air at atmospheric pressure, this is roughly 30 kV per centimeter.
The electric field accelerates the few electrons and ions that are always present in air, due to natural processes such as cosmic rays, radioactive decay, or photoionization. Ions are much heavier, so they move very slowly compared to electrons.
As the electrons move through the medium, they collide with the neutral molecules or atoms.
Important collisions are:
When the electric field approaches the breakdown field, the electrons gain enough energy between collisions to ionize the gas atoms, knocking an electron off the atom. At the breakdown field, there is a balance between the production of new electrons and the loss of electrons.
Above the breakdown field, the number of electrons starts to grow exponentially, and an electron avalanche forms.
The electron avalanches leave behind positive ions, so in time more and more space charge is building up.
.
Eventually, the electric field from all the space charge becomes comparable to the background electric field.
This is sometimes referred to as the "avalanche to streamer transition".
In some regions the total electric field will be smaller than before, but in other regions it will get larger, which is called electric field enhancement.
New avalanches predominantly grow in the high-field regions, so a self-propagating structure can emerge: a streamer.

Positive and negative streamers

There are positive and negative streamers.
Negative streamers propagate against the direction of the electric field, that is, in the same direction as the electrons drift velocity.
Positive streamers propagate in the opposite direction.
In both cases, the streamer channel is electrically neutral, and it is shielded by a thin space charge layer.
This leads to an enhanced electric field at the end of the channel, the "head" of the streamer.
Both positive and negative streamers grow by impact ionization in this high-field region, but the source of electrons is very different.
For negative streamers, free electrons are accelerated from the channel to the head region.
However, for positive streamers, these free electrons have to come from farther away, as they accelerate into the streamer channel.
Therefore, negative streamers grow in a more diffuse way than positive streamers.
Because a diffuse streamer has less field enhancement, negative streamers require higher electric fields than positive streamers.
In nature and in applications, positive streamers are therefore much more common.
As noted above, an important difference is also that positive streamers need a source of free electrons for their propagation.
In many cases photoionization is believed to be this source. In nitrogen-oxygen gas mixtures with high oxygen concentrations, excited nitrogen emits UV photons which subsequently ionize oxygen. In pure nitrogen or in nitrogen with small oxygen admixtures, the dominant production mechanism of photons, however, is the Bremsstrahlung process.

Similarity laws

Most processes in a streamer discharge are two-body processes, where an electron collides with a neutral molecule.
An important example is impact ionization, where an electron ionizes a neutral molecule.
Therefore, the mean free path is inversely proportional to the gas number density.
If the electric field is changed linearly with the gas number density, then electrons gain on average the same energy between collisions.
In other words, if the ratio between electric field and number density is constant, we expect similar dynamics.
Typical lengths scale as, as they are related to the mean free path.
This also motivates the Townsend unit, which is a physical unit of the ratio.

Emission of run-away electrons and high-energy photons

It has been observed that discharges in laboratory experiments emit X-rays and that lightning discharges emit X-rays and terrestrial gamma-ray flashes, bursts of photons with energies of up to 40 MeV. These photons are produced by runaway electrons, electrons which have overcome the friction force, through the Bremsstrahlung process. However, it has not been fully understood how electrons can gain such high energies in the first place since they constantly collide with air molecules and lose energy. A possible explanation is the acceleration of electrons in the enhanced electric fields of the streamer tips. However, it is uncertain whether this process can really explain a sufficiently high production rate. Recently, it has been proposed that ambient air is perturbed in the vicinity of streamer discharges and that this perturbation facilitates the acceleration of electrons into the run-away regime