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Fig. 2.4 Principal values of
the impedance tensor in a
superimposition model with a
-shaped near-surface
resistive inclusion and a 2D
deep regional conductive
prism shown in Fig. 2.3;
SSB - Swift-Sims-Bostick
method, SE - Swift-Eggers
method, LMK - La
Torraca-Madden-Korringa
method; T = 640 s
-
arg
ς
-
-
ς
arg
-
arg deg
ς
,
ς
,
Ohm
ς
1
ς
SSB
SE
LMK
2D
150.0
135.0
120.0
105.0
90.0
75.0
60.0
45.0
30.0
15.0
0.0
-15.0
-30.0
Fig. 2.5 Principal directions
of the impedance tensor in a
superimposition model with a
-shaped near-surface
resistive inclusion and a 2D
deep regional conductive
prism shown in Fig. 2.3;
SSB - Swift-Sims-Bostick
method, SE - Swift-Eggers
method, LMK - La
Torraca-Madden-Korringa
method, 2D-principal
directions of the regional
two-dimensional impedance
in the absence of the
near-surface inclusion;
T = 640 s
α 1
α 2
observation sites
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