Geoscience Reference
In-Depth Information
density P of fractal fluctuations. Therefore, the probability density P in the primary
eddy growth region (σ ≥ 1 and σ ≤ − 1) is given using the computed value of k as
P
= τ 4 (Eq. 1.20).
The normalized radius r an is given in terms of σ and the golden mean τ from
Eqs. (1.25) and (1.31) as follows:
k
3
2
23 23
ln
z
=
ln
r
(1.34)
an
/
τ σ
/
r
=
z
=
.
an
The normalized aerosol size spectrum is obtained by plotting a graph of normalized
aerosol concentration 1
2
3
σ
dN
dr P
3
2
=
τ
(Eq. 1.33) versus the normalized aero-
N
(ln)
an
sol radius r an = τ 2/ (Eq. 1.34). The normalized aerosol size spectrum is derived di-
rectly from the universal probability density P distribution characteristics of fractal
fluctuations (Eqs. 1.16 and 1.20) and is independent of the height z of measurement
and is universal for aerosols in turbulent atmospheric flows. The aerosol size spec-
trum is computed starting from the minimum size, the corresponding probability
density P (Eq. 1.33) refers to the cumulative probability density starting from 1 and
is computed as equal to P =−
τ σ .
1
The universal normalized aerosol size spectrum represented by 1
N
N
lnr
d
an ) ver-
d(
sus r an is shown in Fig. 1.9 .
1.6.5
Large Eddy Growth Time
The time Γ taken for the steady-state aerosol concentration f to be established at
the normalized height z is equal to the time taken for the large eddy to grow to the
height z and is computed as follows.
The time required for the large eddy of radius R to grow from the primary turbu-
lence scale radius r * is computed as follows.
The scale ratio z
R
r
=
.
*
Therefore, for constant turbulence radius r *
dR
r
dz
=
.
*
The incremental growth d R of large eddy radius is equal to
dR rdz
= *
.
The time period d t for the incremental cloud growth is expressed as follows:
 
Search WWH ::




Custom Search