7 Numerical Simulation of Generation, Distribution, and Impact …
101
Fig. 7.9 Effect of destruction of the Si crystal lattice: a the resulting defect when a particle of
energy ε 0 = 10 keV is hit, b the resulting defect when a particle of energy ε 0 = 1000 keV is hit,
c trajectory of a plasma particle of energy ε 0 = 1000 keV
Thus, a complex study of both scientific and practical issues of the creation and
study of plasma guns was carried out in the work.
7.8 Conclusions
This work presents a sufficiently detailed numerical study of TPB parameters at the
initial stage of TPB motion and during further flight and interaction with strongly
rarefied air. The motion distance depends on the air density and can reach ten
kilometers in the upper ionosphere.
In this work, it was also shown that plasma guns actively developed at present can
serve as an effective tool for the destruction of glass coatings. Further theoretical and
experimental work in this area will make it possible to choose the optimal parameters
for both the plasma device and the plasma itself. The performed studies, in particular,
show that, in addition to a high velocity of the plasma flow, it is necessary to achieve
101
Fig. 7.9 Effect of destruction of the Si crystal lattice: a the resulting defect when a particle of
energy ε 0 = 10 keV is hit, b the resulting defect when a particle of energy ε 0 = 1000 keV is hit,
c trajectory of a plasma particle of energy ε 0 = 1000 keV
Thus, a complex study of both scientific and practical issues of the creation and
study of plasma guns was carried out in the work.
7.8 Conclusions
This work presents a sufficiently detailed numerical study of TPB parameters at the
initial stage of TPB motion and during further flight and interaction with strongly
rarefied air. The motion distance depends on the air density and can reach ten
kilometers in the upper ionosphere.
In this work, it was also shown that plasma guns actively developed at present can
serve as an effective tool for the destruction of glass coatings. Further theoretical and
experimental work in this area will make it possible to choose the optimal parameters
for both the plasma device and the plasma itself. The performed studies, in particular,
show that, in addition to a high velocity of the plasma flow, it is necessary to achieve