shallow seismic refraction interpretation

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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

    shallow refraction travel-time curves: Geophysics, 51, 223–23

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    Gebrande, H., and Miller, H., 1985, Refractionsseismik, in Be

    Geowissenschafen II : Ferdinand Enke, 226–260.

    Hagedoorn, J.G., 1959, The plus-minus method of interpretin

    Geophysical Prospecting, 7, 158–182.

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    Hofmann, T., and Schrott, L., 2003, Determining sediment th

    fill deposits using seismic refraction – a comparison of 2D int

    Hordt, A., and Dikau, R. (eds), Geophysical Applications in G

    Geomorphology, Supp. Vol. 132, Gebruder Borntraeger, 71–8

    Leung T.M., 1995, Examination of the optimum XY value by

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    Palmer, D., 1980, The generalized reciprocal method of seism

    Society of Exploration Geophysics, 104p.

    Redpath, B., 1973, Seismic refraction for engineering site inv

    Research Lab., TR E-73-4, 51p.

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    Schuster, G.T., and Quintus-Bosz, A., 1993, Wavepath eikon

    58, 1314–1323.

    Sjogren, B., 2000, A brief study of the generalized reciprocal

    method: Geophysical Prospecting, 48, 815–834.

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    Whiteley, R.J., 1990c, Advances in engineering seismics: Key

    Geophysical Techniques, Theme 2, Proceedings of the 6 

    th

     IAE

    Whiteley, R.J., 1994, Seismic refraction testing - a tutorial: in

    Geophysical Characterization of Sites: Oxford & IBH Publish

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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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