Geography Reference
In-Depth Information
9.6.1
Development of Rotation in Supercell Thunderstorms
The supercell thunderstorm is of particular dynamical interest because of its ten-
dency to develop a rotating mesocyclone from an initially nonrotating environment.
The dominance of cyclonic rotation in such systems might suggest that the Coriolis
force plays a role in supercell dynamics. However, it can be shown readily that the
rotation of the earth is not relevant to development of rotation in supercell storms.
Although a quantitative treatment of supercell dynamics requires that the den-
sity stratification of the atmosphere be taken into account, for purposes of under-
standing the processes that lead to development of rotation in such systems and
to the dominance of the right-moving cell, it is sufficient to use the Boussinesq
approximation. The Euler momentum equation and continuity equation may then
be expressed as
D U
Dt =
U
∂t +
1
ρ 0
·∇
=−
+
( U
) U
p
b k
∇·
=
U
0
Here, U
is the three-dimensional
del operator, ρ 0 is the constant basic state density, p is the deviation of pressure
from its horizontal mean, and b
V
+
k w is the three-dimensional velocity,
0 is the total buoyancy.
It is convenient to rewrite the momentum equation using the vector identity
≡−
U
·
U
( U
·∇
) U
=
U
×
(
×
U )
2
to obtain
p
ρ 0 +
U
∂t =−
U
·
U
+
U
× ω +
b k
(9.53)
2
Taking
(9.53) and recalling that the curl of the gradient vanishes, we obtain
the three-dimensional vorticity equation
×
∂t = ×
( U
× ω
)
+ ×
(b k )
(9.54)
Letting ζ
(9.54), we
obtain an equation for the tendency of ζ in a nonrotating reference frame:
=
k
· ω
be the vertical component of vorticity and taking k
·
∂ζ
∂t =
k
· ∇×
( U
× ω
)
(9.55)
Note that buoyancy only affects the horizontal vorticity components.
 
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