Schmucker, 1970 (Scripps) - MTNet

K
Kf
Pv
pc(f)
p, q
Q
Q*
qH' qz
SX(f)
SXy(f)
t
y
Z (t)
'Z. Za
zH. zD. zz
zp
v2
ED' EH. EZ
C
7'}n. 7'} (k)
7'}s
7'}n(iz)
(J
T
propagation constant of downward diffusing field in stratified
conductors (eqs. 5.11 and 31).
Kertz's operator applied to f(x) (sec. 3.16)
skin-depth value of the vth layer (eq. 5.1)
skin-depth value of the uniform substitute conductor, Pc/2 is
the imaginary part of c (f)
perturbation arrows (sec. 3.10). pertaining to Ha and Da
normalized sheet-current density (eq. 6.4)
1-2 Q
transfer functions for ja (eq. 6.6)
power spectrum of X (t)
cross spectrum between X(t) and Y(t)
time
true east component of F (t)
vertical component of F (t), positive down
normal and anomalous part of Z (t)
transfer functions for Za (sec. 3.8)
projection of vertical transfer functions zH and zD on the direction
of a profile of field stations (eq. 3.26)
Laplacian operator
residuals of correlation analysis (sec. 3.9)
tangential electric variation vector (eq. 5.40)
induction parameter of uniform conductors (sec. 5.4)
induction parameter of shell-core models (sec. 5.8)
spherical Bessel functions of the 2nd kind (App. II)
electrical conductivity
total conductivity of thin sheets or shells (eq. 1.7)
normal and anomalous part of T
21Tf
xi