shallow seismic refraction interpretation
TRANSCRIPT
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Comparison of shallow seismic refraction interpretatio
Robert J Whiteley and Peter J Eccleston
Coffey Geotechnics Pty. Ltd.
8/12 Mars Road Lane Cove West
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ABSTRACT
A number of shallow refraction interpretation method
conditions using synthetic and published field data. The sy
velocity zone in a depression at the base of the regolith. Ind
Reciprocal Method was in reasonable with this model. The
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While our comparisons are not definitive and all the in
compared have deficiencies and limitations they do offer so
refraction interpretation for regolith mapping. This is achie
methods and involves the Reciprocal Method, Wavepath Ei
and Visual Interactive Ray Tracing. Interesting subsurface
highlighted by joint use of ray path displays and wave path
various statistical goodness-of-fit measures to the field data
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INTRODUCTION
Shallow seismic refraction is the “work-horse” of eng
widely applied to regolith mapping in geotechnical enginee
interpretation developments have led to this method being i
conventional mineral exploration technique for deeper targe
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With the routine acquisition of increased volumes of d
focus of effort is now on the quality and applicability of an
approaches and methods. These are still currently 2D but a
sensitivity of the refraction method to regolith variations is
We have chosen to compare some refraction interpretation m
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more sophisticated refractor velocity analysis via line-segm
(i.e., minus-times). With the RM, depth errors caused by la
regolith and by incompletely defined shallower refractors ar
interpolation of composite velocity terms between source po
been identified. The RM can also be enhanced to evaluate t
velocity analyses (e.g., Dampney and Whiteley, 1980) and o
sparse in constrained field conditions (e.g., Wright, 2006).
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The absence of a theoretical and reliable practical bas
migration distances has meant that the performance of the G
media being questioned by a number of authors (e.g., Hathe
Sjogren, 2000; Leung, 1995, 2003; Whiteley, 2002). The p
GRM is examined in our comparison.
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refraction interpretation on a PC screen using Visual Interac
VIRT is one of the interpretation methods used in this comp
As available PC power has increased, other approache
interpretation have been developed including various forms
Zhang and Toksöz, 1998). Sheehan et al. (2005) recently e
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SYNTHETIC DATA
The 3-layer synthetic model (Model 3L01, from Whit
of many similar models that were examined. This contains
below the deeper interface representing a variable regolith b
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wide with a velocity of 1500 m/s. The RM has identified a
26 m wide, extending from about 58 m to 84 m with a veloc
somewhat narrower than the actual low velocity zone. The
violation as an unacceptably high velocity zone on the right
This so-called “fictitious” velocity region is uncertain in the
used. Such model violations often occur when first arrivals
refracted waves are combined in the RM and GRM velocity
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layers of this model it is quite difficult for WET inversion.
interpretation has represented significant features of the syn
deepening near the centre of the model being apparent in th
other features of the model are less obvious. The approxim
model is close to the specified velocities for the upper layer
approximately follows the 2400 m/s velocity contour althou
are not reached until much deeper. However, the left margi
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Figure 6. This interpretation has identified a wide low velo
refractor, possibly representing a fault and a substantial cha
this structure. This is represented mainly by the thickening
assigned a uniform velocity of 1600 m/s in the GRM interpr
VIRT was independently applied to this data set and a
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The WET model obtained after 20 iterations using a s
shown in Figure 7, with the corresponding wave path densit
fitted the field data with a maximum unsigned error of 2.2 m
change across the structure with very different velocity grad
with different lithologies and weathering characteristics. A
indicated in the WET interpretation at the structure. The w
7 shows a concentration within the higher velocity shallowe
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refracted arrivals that occur over abrupt structures. These e
obtained with both the RM and GRM over the thicker regol
poorly for this model, both smoothing and underestimating
the depression and greatly narrowing the low velocity zone.
WET inversion allowed a major feature of the synthet
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approaches to shallow refraction interpretation for regolith m
approach is summarised in Table 1.
Firstly, this involves applying the RM that incorporate
of redundant, single direction first-arrival data sets. This al
quality and limitations to be quickly assessed and provides
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ACKNOWLEDGEMENTS
Maung Aung Win interpreted the synthetic model dat
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REFERENCES
Ackermann H.D., Pankratz, L.W., and Dansereau, D., 1986, R
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Gebrande, H., and Miller, H., 1985, Refractionsseismik, in Be
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Hofmann, T., and Schrott, L., 2003, Determining sediment th
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Leung T.M., 1995, Examination of the optimum XY value by
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Palmer, D., 1980, The generalized reciprocal method of seism
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Schuster, G.T., and Quintus-Bosz, A., 1993, Wavepath eikon
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Sjogren, B., 2000, A brief study of the generalized reciprocal
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Whiteley, R.J., 1990c, Advances in engineering seismics: Key
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Whiteley, R.J., 1994, Seismic refraction testing - a tutorial: in
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TABLE
Table 1:
Shallow Refraction Interpretation System for Detailed Rego
Interpretation Method App
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FIGURE CAPTIONS
Fig. 1:
Synthetic Model 3L01 with t - x plots and first arrival ray pat
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(a) GRM interpretation, after Palmer (1980), and (b) VIRT
Fig. 7:
WET interpreted model and wavepath density diagram.
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