The trends and variance in amplitude variation with offset (AVO) observatio
ns caused by near-surface structure, attenuation, and scattering are numeri
cally synthesized by pseudospectral viscoelastic 2-D modeling. Near-surface
structure produces amplitude focusing and defocusing that significantly di
stort AVO observations in offset windows at a scale comparable to that of t
he lateral variations in the structure. Attenuation and scattering decrease
absolute amplitudes at all offsets. Scattering and wave interference incre
ase the variance associated with AVO measurements.
Depending on the relative influence of intrinsic attenuation, apparent atte
nuation associated with scattering, and geometrical focusing, a normalized
AVO response can increase or decrease with offset (relative to that for the
associated elastic, nonscattering, 1-D solution), and so mimic the behavio
r predicted as a function of contrasts in density, velocity, porosity or Po
isson's ratio. If only relative (normalized) amplitudes are available, it i
s difficult to distinguish between effects of parameters whose main contrib
utions are to absolute amplitude; for example, a trend of decreasing amplit
ude (relative to that for an elastic flat-layered model) produced by intrin
sic attenuation may be counteracted by focusing/scattering or anisotropic e
ffects over wide aperture ranges. Diagnostic information on AVO effects of
scattering and attenuation is lost when the noise level is sufficiently hig
h. Interpretations of AVO observations based on homogeneous layered elastic
models must therefore be used with caution as they are, in general, nonuni
que. Lateral variations in AVO parameters are the key to detecting hydrocar
bons, so lateral changes in AVO produced by lateral changes in the overburd
en properties have potential for being misinterpreted, especially if the re
cording aperture is small.