Sentence examples for charging of dust from inspiring English sources

Particle rezoning is then applied to 1D studies of collisionless shocks and the 2D simulations of charging of dust immersed in a plasma.

Charging of dust (positive or negative) depends upon the charging processes (e.g., photoionization, secondary electron emission, thermionic emission or by electron ion bombardments on surface of dust particles).

There has recently been a renewed interest in the charging of dust grains in a plasma and its effect not only on dust dynamics in astrophysical and solar system environments but also in laboratory plasma processing and semiconductor manufacturing.

The plasma environment around Neptune (which controls charging of the dust) was also examined by the Voyager spacecraft and is used to determine the charge on individual dust particles.

In this paper we re-examined the fundamental physics of charging of a dust particle in the moon environment by tenuous anisotropic solar wind plasma.

The diffuse E ring in Saturn's magnetosphere is an ideal laboratory for studying the charging processes of dust and spacecraft.

The majority of work on dusty (complex) plasmas is largely concerns with laboratory plasmas, in which charging process of dust grains is very fast, thus making practical the working concept of dynamically equilibrium floating potential and grain charge.

The charge of dust particles is formed by attachment of the free electrons and ions and by photo emission.

(j=1) for the condition (n_{d+}>n_{d-}) and (j=-1) for the condition (n_{d+}<,n_{d-}), i.e. the value of (j) dependents on net charge of dust grain and (beta ) is the mass ratio of negative ion to positive ion ((m_n/m_p)).

In the case of a non-monotonic plasma sheath, non-neutral plasma layers could also affect the charging of these dust grains.

For both the cases of charge density of dust grains ((j=1) or (j=-1)) the amplitude increases with propagation angle.