Modern seismic recording instruments allow precise measurements of the amplitude of reflected signals. Intuitively we would expect that this amplitude information could be used to increase our knowledge of the physical properties of the reflecting earth. The relevant factors defining the amplitude of a reflection signal are: spherical divergence, absorption, the reflection coefficient of the reflecting interface, the cumulative transmission loss at all interfaces above this, and the effect of multiple reflections. Of these factors, three—spherical divergence, the reflection coefficient and the transmission loss—are reasonably clear concepts (though the estimation of transmission loss from acoustic logs caused some difficulties in the hey-day of synthetic seismograms). Absorption still presents considerable problems of detail, but our understanding has increased significantly in recent years. The factor least well understood is undoubtedly the effect of multiple reflections. Multiple paths having an even number of bounces can have the effect of delaying, shaping and magnifying the pulse transmitted through a layered sequence. Simple demonstations of this phenomenon can be made using elementary thin plates, and these can be presented for various synthetic and real sequences of layers. Such demonstrations lead one to explore the relation between the spectrum of the transmitted pulse and the spectrum of the reflection coefficient series. If it were possible to isolate the amplitude and shape variations imposed by absorption within a layer, there would be a chance that this measure of absorption would be useful as a correlatable or diagnostic indication of rock properties. If it were possible to isolate the amplitude and shape variations imposed by multiple reflections, there would be a chance that this measure would be useful as an indication of cyclic sedimentation and of the dominant durations of the sedimentary cycles. However, the separation of these two effects constitutes a formidable challenge. The very difficulty of this separation suggests that it may be opportune to review the quantitative estimates of absorption made by field experiments.
[1]
P. Bois,et al.
ETUDE STATISTIQUE DE LA CONTRIBUTION DES MULTIPLES AUX SISMOGRAMMES SYNTHETIQUES ET REELS
,
1963
.
[2]
P. O'brien,et al.
SOME EXPERIMENTS CONCERNING THE PRIMARY SEISMIC PULSE
,
1969
.
[3]
N. Anstey.
ATTACKING THE PROBLEMS OF THE SYNTHETIC SEISMOGRAM
,
1960
.
[4]
J. Sherwood,et al.
Minimum-phase and related properties of the response of a horizontally stratified absorptive Earth to plane acoustic waves
,
1965
.
[5]
SUR L'INFLUENCE D'UN EMPILEMENT DE COUCHES MINCES EN SISMIQUE*
,
1963
.
[6]
A. W. Trorey.
THEORETICAL SEISMOGRAMS WITH FREQUENCY AND DEPTH DEPENDENT ABSORPTION
,
1962
.
[7]
R. Bortfeld.
Seismic Waves in Transition LAYERS
,
1960
.
[8]
G. Kunetz,et al.
FILM SYNTHETIQUE AVEC REFLEXIONS MULTIPLES THEORIE ET CALCUL PRATIQUE
,
1960
.
[9]
J. Hagedoorn,et al.
A process of seismic reflection interpretation
,
1954
.
[10]
P. Bois,et al.
INFLUENCE DE LA LARGEUR DU PAS D'ECHANTILLONNAGE DU CAROTTAGE CONTINU DE VITESSES SUR LES SISMOGRAMMES SYNTHETIQUES A MULTIPLES*
,
1965
.