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E
z
,
V/m
250
2
t
, s
0
5
10
1
-250
Fig. 11.9
Vertical electric field arising in the surface atmospheric layer under a cratering explosion
of HE with mass 23.8 g. The explosion was performed at normalized depth 0.68 m/kg
1=3
.
1
—
theoretical calculations,
2
—measurements at distance 5.2 m from the explosion site. Adapted from
Adushkin et al. (
1990
)
3000
E
z
, V/m
2500
2000
a
1500
1000
b
500
c
t
, s
0
0
100
200
300
400
500
600
700
800
900
Fig. 11.10
Variations of vertical electric field caused by the HE explosion with mass 500 t as
observed at different distances R from the explosion site (Soloviev and Surkov
2000
). (
a
) R
D
1:5 km; (
b
) R
D
2 km; (
c
) R
D
1:5 km (model calculation)
and experimental data at the moment 40 s corresponds to the following parameters:
q
1
D
1:3
˙
0:1 C, h
1
D
1:39
˙
0:06 km, q
2
D
0:4
˙
0:1C, and h
2
D
0:30
˙
0:06 km.
A series of surface detonations of HE charges with mass of a few kilograms were
carried out by Soloviev et al. (
2002
). The study showed that the amplitude of the
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