Information Technology Reference
In-Depth Information
Fig. 1.13
Dispersion relations between the real,
R
, and imaginary,
X
, parts of normalized
impedance
Z
50
◦
; solid line -
initial curve, broken line - curve compuded by (1.98); calculated for a model shown in Fig. 1.11
45
◦
,
/
i
0
at a point O with coordinates
r
=
0.129 km,
=
=
Dear colleagues,
The loss of our colleague and my friend Leonid Vanyan is truly sad, and I am personally
devastated by the news. Just two weeks ago Leo sent me this email message, with the germ
of an idea for how to make “old” apparent resistivity and phase data useful by requiring them
to be consistent using an iterative approach. He and I were going to work on this together,
but that will not happen now. Rather than work on this alone, I would like to share this idea
with you all. If any of you should find it useful, please name it the
Vanyan correction
in
Leonid's honor. Those of you who were at Victoria in 1982 will smile at Leonid's comment
about our agreement on the importance of comparing
and
. Alan Jones
