Chemistry Reference
In-Depth Information
From the detailed discussion of these equations (in a suitable dimensionless form)
concerning the chemical point of view and restricting on volume reactions the fol-
lowing general principles of plasma chemical similarity for homologous points of
two systems of the AZ result [17]
Similar systems agree in the spatial and temporal distributions of all their
components, expressed by identical values of
n i L 0 , τ 0
n 0
n i
,
L 0 , t 0
r 0
with n 0 =
(4.18)
τ 0
τ 0 is the residence time of gas mixture in the Active Zone, L 0 the char-
acteristic length (e.g., of reactor); here subscript “0” are the reference
parameters.
The plasma chemical similarity is described by the correspondence in
n i
n 0 ,
T
T 0 ,
n e
n e 0
U e
U e 0
,
, i
=
1, 2,
...
.
(4.19)
The conditions for this correspondence are the following one:
From outside in chemical similar plasmas two reduced physical fields
must be in correspondence
v L 0 , τ 0
v 0
E τ 0
E 0
,
.
(4.20)
Here, the geometrical similarity is manifested.
The dimensionless similarity parameters of the problem are:
τ 0 D i 0
L 0
λ W 0 T 0
L 0 p 0 v 0 =
λ e 0 E 0
U e 0
μ ion
μ e 0
λ e 0
L 0
τ e 0
τ 0
,
P e ,
,
and
,
,
(4.21)
P e is the Peclet Number. Both later ones are a consequence of introducing
kinetic reference parameters for the electron gas (subscript “0”).
For plasma chemical similarity the correspondence of all the reduced
source terms
τ 0 S i
n 0
τ 0 H
p 0
τ e 0 S e
n e 0
τ e 0 H e
U e 0
,
,
,
(4.22)
is required.
The widely general principle of plasma chemical similarity reflects
the underlying electronical similarity of the plasma.
 
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