I. Psencik et Jl. Martins, Properties of weak contrast PP reflection/transmission coefficients for weakly anisotropic elastic media, STUD GEOPH, 45(2), 2001, pp. 176-199
Approximate formulae for PP reflection/transmission (R/T) displacement coef
ficients for weak contrast interfaces separating weakly anisotropic media o
f an arbitrary symmetry are presented. The coefficients have a form of a nl
m of a well-known approximate PP reflection/transmission coefficient for a
weak contrast interface separating two background isotropic halfspaces and
a correction due to weak anisotropy. The correction is controlled, linearly
, by the so-called weak anisotropy (WA) parameters. The coefficients are de
fined with respect to an arbitrary isotropic background. The formulae are c
onvenient for description of coefficients of reflection and transmission in
low symmetry weakly anisotropic media as well as in media with higher symm
etry (orthorhombic, hexagonal) with arbitrarily oriented axes of symmetry.
For anisotropies of higher symmetry for which approximate formulae of other
authors exist, we discuss the differences between these and our formulae a
nd effects of these differences on the accuracy of approximate coefficients
. performance of the approximate formulae for Rpp coefficients is tested on
models with weak anisotropy and weak contrast interfaces as well as on mod
els whose anisotropy and velocity contrast are in no way weak. Even in the
latter case, the formulae yield satisfactory results. Accuracy of the appro
ximate Rpp coefficient depending on the choice of the background is then in
vestigated. It is shown that the Rpp coefficient can be described approxima
tely by a formula, whose correction term due to anisotropy is independent o
f the S-wave background velocity and depends only slightly on the choice of
the P-wave background velocity. The formulae for the Rpp coefficients comm
only used in literature for higher symmerty anisotropies are obtained by li
nearization of the above mentioned formula. Linearization lead to the depen
dence of the Rpp coefficient on the choice of the S-wave background velocit
y and, generally to a slight decrease of accuracy. Presented formulae are c
onvenient for solving an inverse problem determination of contrasts of para
meters of anisotropic media surrounding an interface. Sensitivity of the ap
proximate Rpp coefficient to basic weak anisotropy parameters is presented.