Figure 6-6. Logarithm of the normalized number of bubbles against depth from (6.13) at
various values of u
0
With a simplified parameterization for the turbulent mixing coefficient
B
K
u z
N
(6.11)
and the bubble decay rate
0
/ 1
/
z
z H
V D
(6.12)
(here
0
0 /
10
H
p gU |
m, and p 0 is the atmospheric pressure), Thorpe
(1982) obtained the following solution of (6.10):
Chapter 6: HIGH WIND SPEED REGIME
407
with parameters chosen to correspond to a = 50 mm. Reproduced
from Thorpe (1982) with the permission of the Royal Society of London.
various values of u
0
With a simplified parameterization for the turbulent mixing coefficient
B
K
u z
N
(6.11)
and the bubble decay rate
0
/ 1
/
z
z H
V D
(6.12)
(here
0
0 /
10
H
p gU |
m, and p 0 is the atmospheric pressure), Thorpe
(1982) obtained the following solution of (6.10):
Chapter 6: HIGH WIND SPEED REGIME
407
with parameters chosen to correspond to a = 50 mm. Reproduced
from Thorpe (1982) with the permission of the Royal Society of London.