Using refraction method to find depth to bedrock
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| Series | Geophysical References Series |
|---|---|
| Title | Problems in Exploration Seismology and their Solutions |
| Author | Lloyd P. Geldart and Robert E. Sheriff |
| Chapter | 14 |
| Pages | 497 - 503 |
| DOI | http://dx.doi.org/10.1190/1.9781560801733 |
| ISBN | ISBN 9781560801153 |
| Store | SEG Online Store |
Problem 14.1
To find the depth to bedrock in a damsite survey, 12 geophones were laid out at 15-m intervals from 15 to 180 m. Determine the overburden depth from the data in Table 14.1a assuming a single layer above the refractor. By how much does the depth differ if we assume two layers above the refractor?
Background
The refraction method is discussed in problem 4.18.
| $ x({\rm {m}}) $ | $ t({\rm {s}}) $ |
|---|---|
| 15 | 19 |
| 30 | 29 |
| 45 | 39 |
| 60 | 50 |
| 75 | 59 |
| 90 | 62 |
| 105 | 65 |
| 120 | 68 |
| 135 | 72 |
| 150 | 76 |
| 165 | 78 |
| 180 | 83 |

Solution
Figure 14.1a shows the plotted data. The single layer interpretation (fine lines) gives $ V_{1}=1120\ {\mbox{m/s}} $, $ V_{2}=4120\ {\mbox{m/s}} $, $ t_{i}=0.084\ {\rm {s}} $. The critical angle $ \theta _{c}=\sin ^{-1}(1120/4120)=15.8^{\circ } $. Equation (4.18a) gives the depth to bedrock as
$ {\begin{aligned}h=V_{1}t_{i}/2\cos \theta _{c}=1120\times 0.084/2\cos 15.8^{\circ }=49{\mbox{ m}}.\end{aligned}} $
The three-layer solution (heavy lines) gives $ V_{1}=790\ {\mbox{m/s}}, $ $ V_{2}=1490\ {\mbox{m/s}} $, $ V_{3}=4120\ {\mbox{m/s}} $, $ t_{i1}=0.020\ {\rm {s}} $, $ t_{i2}=0.084\ {\rm {s}} $. Note that $ V_{1} $ is not reliable; it could be any smaller value. If it were smaller, the first-layer values would change slightly, but it would not significantly change the values for the other layers.
For the first interface, $ \theta _{c1}=\sin ^{-1}(790/1490)=32.0^{\circ } $,
$ {\begin{aligned}h_{1}=V_{1}t_{i1}/2\cos \theta _{c1}=790\times 0.020/2\times \cos 32.0^{\circ }=9.3\ {\rm {m}}.\end{aligned}} $
For the second interface, $ \sin \theta _{1}/V_{1}=\sin \theta _{c2}/V_{2}=1/V_{3} $, so
$ {\begin{aligned}\sin \theta _{1}/790=\sin \theta _{c2}/1490=1/4120;\quad \theta _{1}=11.1^{\circ },\quad \theta _{c2}=21.2^{\circ }.\end{aligned}} $
Thus we get from equation (4.18d)
$ {\begin{aligned}t_{i2}=2h_{1}\cos \theta _{1}/V_{1}+2h_{2}\cos \theta _{c2}/V_{2},\end{aligned}} $
so $ 0.084=2\times 9.3\times 0.981/790+2\times h_{2}\times 0.932/1490 $,
$ {\begin{aligned}h_{2}=(0.084-0.023)\times (1490/2\times 0.932)=49\ {\rm {m}}.\end{aligned}} $
The total depth is $ h_{1}+h_{2}=58\ {\rm {m}} $.
The difference between the two interpretations is 9 m or about 17%.
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| Specialized techniques | Introduction to Problems in Exploration Seismology and their Solutions |
Also in this chapter
- Using refraction method to find depth to bedrock
- Interpreting engineering refraction profiles
- Interpretation of four-shot refraction data