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plasmas are considered quasi-neutral on large length scales greater than a few Debye lengths, also known as the sheath thickness [78]. The Debye length, or Debye radius as it is also referred, is the characteristic length scale by which a charged particle will be ’shielded’ by particles of opposite polarity. For example, if a positive ion is inserted into an initially neutral and spatially uniform plasma system, a displacement of plasma electrons and negative ions will occur as they are attracted to the positive ion creating a charge cloud surrounding the particle. This charge cloud results in a shielding effect, partially canceling out the test particle potential [78]. This charge separation created by the positive ion and the negative charge cloud over the distance of a few Debye lengths produces a region of non-neutrality within the plasma. For Debye shielding to be relevant, the length scale must be small compared to the overall plasma dimensions, otherwise plasma particles would not exist outside of the Debye radius. 3.1.2 Collisional Processes in Plasmas Now that the basic properties of plasmas have been described, the collisional processes that occur between charged and neutral species which are essential for plasma production and plasma chemistry will be discussed. In most weakly ionized plasmas, electrons are the primary energy carrier and are responsible for transferring energy to heavy particles via collisions. These collisional processes can become very complex when dealing with molecular plasmas due to the creation of various chemically active species such as excited atoms and molecules, charged particles, neutral species, and radicals. Each component of the plasma plays a role in the output of a given chemical process, and it is necessary to understand how collisions can be manipulated to achieve a desired result. Before describing the different types of collisional processes, an explanation of how a collision is defined should first be identified. There are generally two classes of 31PDF Image | CO2 Conversion in a Microwave Plasma Catalyst System
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