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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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