Geophysical Information Adewoyin, O. O., Joshua, E. O. Akinyemi, M. - - PowerPoint PPT Presentation

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Analysis of Geotechnical Parameters from Geophysical Information Adewoyin, O. O., Joshua, E. O. Akinyemi, M. L., Joel, E. S. and Omeje, M. from Covenant University, Ogun State, Nigeria Content of Presentation Introduction Methodology


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Analysis of Geotechnical Parameters from Geophysical Information

Adewoyin, O. O., Joshua, E. O. Akinyemi, M. L., Joel, E. S. and Omeje, M. from Covenant University, Ogun State, Nigeria

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Content of Presentation

Introduction Methodology Results and discussion Conclusion

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Introduction

 The high cost of geotechnical investigation is a major factor

that discourages many building developers from carrying out site characterization.

 Especially, when there is no legislation that enforces it.  One of the consequences of this is its significant contribution

to the incessant building collapse experienced in many developing countries, including Nigeria of late.

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Introduction Cont’d

 Geophysical investigations are usually less expensive and much

easier to conduct (Anderson and Croxton, 2008; Mohd et al., 2012).

 This approach does not affect the natural state of the

environment.

 One of such methods is the seismic refraction method (Tezcan et

al., 2009; Atat et al., 2013).

 This involves the generation of seismic energy (seismic waves or

elastic stress waves) that travels through the soil and interact with soil particles and interstitial fluids.

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Introduction Cont’d……..

 The effect of soil texture and structure affect the responses of soil

to seismic waves. These variations in responses are the interest of the geophysicist (Sayeed et al., 2007; Uyanik, 2010).

 Based on the above, seismic refraction method can be used to

estimate and observe internal changes of soil properties,

 which can be used as a measure of seismic parameters that may

be useful in subsurface characterization (Altindag, 2012; Bery and Saad, 2012).

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Methodology

 Seismic refraction survey was conducted using a 24-Channel

Terraloc MK 6 seismogram (ABEM Instrument, 1996).

 The length of the surveyed profiles ranges between 100 and

200 m, 2 m geophone spacing was used for proper coverage of the refractor layer (Mohd et al., 2012).

 A 15 kg sledge hammer was used as the energy source and data

were acquired

 The data acquired were interpreted using seisImager software

package (SeisImager, 2009).

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Fig 1: schematic diagram of seismic refraction method (Subsurface geotechnical, 2016).

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Methodology Cont’d…….

 The results obtained from the software interpretation were

subjected to some equations in theory in order to determine basic geotechnical parameters (Tezcan et al., 2009; Nastaran, 2012; Atat et al., 2013).

 Statistical analysis was applied to the raw data set.  The analysis used in this study was based on the relationship

between the primary wave velocity and other geotechnical parameters derived from the study (Altindag, 2012)

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Methodology Cont’d…..

 The raw data set was subjected to least square regression

analysis,

 Different curve fitting approximations were executed.  The polynomial regression of order 2 was found to give the

highest correlation coefficient in most cases.

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Methodology Cont’d

 Empirical correlation equations were obtained that related

both the p-wave velocities with basic geotechnical parameters.

 The graphs of the different geotechnical parameters were

plotted against the primary wave velocity.

 The graphs obtained are as presented below

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Results and discussion

E= 3E-06Vp2 - 0.0024Vp + 1.4289 R² = 0.9999

5 10 15 20 25 30 500 1000 1500 2000 2500 3000 3500 4000

Young's modulus, E (GPa) Primary wave velocity, Vp (m/s) Fig 2: The graph of Young’s modulus (GPa) against the primary wave velocity (m/s)

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Results and discussion Cont’d…….

Fig 3: The graph of Bulk modulus (GPa) against the primary wave velocity (m/s)

B = 2E-06Vp2 - 0.0015Vp + 0.9163 R² = 0.9999

2 4 6 8 10 12 14 16 18 500 1000 1500 2000 2500 3000 3500 4000

Bulk modulus, B (GPa) Primary wave velocity, Vp (m/s)

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Results and discussion Cont’d………..

Fig 4: The graph of shear modulus (GPa) against primary wave velocity (m/s)

μ = 1E-06Vp2 - 0.001Vp + 0.5754 R² = 0.9999

2 4 6 8 10 12 500 1000 1500 2000 2500 3000 3500 4000 Shear modulus, μ (GPa) Primary wave velocity, Vp (m/s)

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Results and discussion Cont’d………

Fig 5: The graph of Oedometric modulus (GPa) against primary wave velocity (m/s)

Ec = 2E-06Vp2 - 0.001Vp + 0.3606 R² = 1 1 2 3 4 5 6 7 8 9 500 1000 1500 2000 2500

Oedometric modulus, Ec (GPa) Primary wave velocity, Vp (m/s)

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Results and discussion Cont’d……

Fig 6: The graph of ultimate bearing capacity (MPa) against the primary wave velocity

qf = 1E-07Vp2 + 0.0009Vp - 8E-05 R² = 1 0,5 1 1,5 2 2,5 500 1000 1500 2000 2500

ultimate bearing capacity, qf (MPa) Primary wave velocity, Vp (m/s)

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Results and discussion Cont’d…….

 The empirical correlation equations were obtained

4289 . 1 0024 . 10 3

2 6

   

 p p

V V E 9163 . 0015 . 10 2

2 6

   

 p p

V V B

5754 . 001 . 10 1

2 6

   

 p p

V V 

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Results and discussion Cont’d…….

3606 . 001 . 10 2

2 6

   

 p p c

V V E

5 2 7

10 8 0009 . 10 1

 

    

p p f

V V q

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Results and discussion Cont’d….

 The coefficient of determination for the various parameters

ranged between 0.99 and 1.00.

 This indicates a high degree of correlation.  Thus, from these equations the geotechnical parameters of

interest can be determined by obtaining information on either the compressional wave velocity of the different layers of the subsurface.

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Results and discussion Cont’d…..

 It is important to state at this point that the results obtained in this

study correlated with the results of Altindag (2012) and Bery and Saad (2012).

 The correlation coefficient in Altindag (2012) differed from the present

study by 0.22 while in Bery and Saad (2012) the correlation coefficient varied from the present study by a factor of 0.06.

 This variation in results could be as a result of the different curve

fitting approximation used or the variation in the geological formation

  • f the areas of study.
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Results and discussion cont’d…….

 For instance, in Altindag (2012), power curve fitting approximation

was found to give the highest correlation coefficient and the geomaterials studied were of sedimentary geological composition.

 In Bery and Saad (2012) linear curve fitting approximation was

used for the study and the geologic formation is microcline granite, which is quite different from the present study.

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Conclusion

 In conclusion, this study revealed that geotechnical

parameters can be determined from the p-wave velocity, which can be used to easily characterize the subsurface condition of a site.

 Also, the empirical equations obtained can be used to

evaluate and predict the geotechnical parameters of a site.

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Conclusion Cont’d………..

 Finally, this study has the potential to reduce the cost and the

difficulty of conducting geotechnical investigations before embarking on building development.

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Acknowledgements

 The authors would like to appreciate the management of

Covenant University for providing financial support for this research.

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References

 ABEM Instrument AB, 1996. Equipment Manual for TERRALOC MK6 Software Version 2.21,

Bromma, Sweden

 Altindag, R. “Correlation between P-wave velocity and some mechanical properties for

sedimentary rocks”, The Journal of the Southern African Institute of Mining and Mettalurgy, 2012, vol. 112, pp. 229-237.

 Anderson, N and Croxton, N Geophysical methods commonly employed for geotechnical site

characterization, Transportation Research Circular 2008, pp.1-13

 Atat, J. G., Akpabio, I. O. and George, N. J. “Allowable bearing capacity for shallow

foundation in Eket Local Government area, Akwa Ibom State, Southern Nigeria”, International Journal of Geosciences, 2013, vol. 4, pp. 1491-1500

 Bery, A. A. and Saad, R. “Correlation of seismic p-wave velocities with engineering

parameters (N value and rock quality) for tropical environmental study”, International Journal of Geosciences, 2012, vol. 3, pp. 749-757.

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References Cont’d……..

 Mohd, H. Z. A., Rosli, S., Fauziah, A. Devapriya, C. W. and Mohamed, F

. T . B “Seismic refraction investigation in near surface landslides at the Kindasang area in Sabah, Malaysia”, Sciverse Science Direct, Procedia Engineering, 2012, vol. 50, pp. 516-531

 Nastaran, S. Correlation between geotechnical and geophysical properties of soil. A thesis

submitted in partial fulfilment of the requirement of Birmingham University for the degree

  • f Master of Philosophy. Stoke-on-trent: University of Birmingham, 2012

 Sayeed, S. R. M. Adel, M. E. M. and Abd El-Aal, A. K. ” Applicability of near surface seismic

refraction technique to site characterization of south Marsa Matrouh and Sedi Abd El- Rahman, Western desert, Egypt,” Journal of Applied Geophysics, 2007, vol. 6, no. 2, pp. 77-85

 SeisImager, 2009. SeisImager/2DTM Manual Version 3.3  Soupios, P

. M., Papazachos, C. B., Vargemezis, G. and Fikos, I. “Application of seismic methods for geotechnical site characterization”, International Workshop in Geoenvironment and Geotechnics, 2005, pp. 1-7

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References Cont’d……

 Subsurface Geotechnical [sourced on 3/02/2016] @ www.geophysical.biz/seisrf1.htm  Tezcan, S. S., Ozdemir, Z. and Keceli, A. “Seismic technique to determine the allowable

bearing pressure for shallow foundations in soils and rocks”, Acta Geophysica, 2009,

  • vol. 57 no. 2, pp. 1-14

 Uyanik, O. “Compressional and shear wave velocity measurements in unconsolidated

top-soil and comparison of the results”, International Journal of the Physical Sciences, 2010, vol. 5 no. 7, pp. 1034-1039.

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Thank You for Listening