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Home Civil Engineering Foundation Engineering

Seismic Refraction Survey – Determine Classification and Thickness of Various Soil Layer

Arjun Barman,CE by Arjun Barman,CE
December 2, 2023
in Foundation Engineering
Reading Time: 7 mins read
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Seismic Refraction Survey is a part of the geotechnical investigation. In this article, you will find seismic refraction method and its procedure for the classification of soil and determining the soil layer thickness.

Table of Contents

  • Seismic Refraction Survey
    • Seismic Reflection Survey Method
    • Seismic Refraction Survey Limitations:
    • Example:
      • Solution:
    • Velocity Calculation
    • Thickness of Layers
    • Reference:
    • FAQ
      • What is seismic refraction survey?

Seismic Refraction Survey

Seismic refraction survey is useful in obtaining preliminary information about the thickness of the various soil layers and the depth of rock or hard soil at a large site. Seismic refraction surveys are conducted by impacting the soil surface, such as at point A in Figure 3.45a, and observing the first arrival of the stress waves (disturbance) at several other points (e.g., B, C, D, ….). The impact can be created by a small explosion or hammer blow. Geophones can record the first arrival of disturbance waves at several points.

The impact on the ground surface creates two types of waves, one is P-waves (plane waves or compression waves) and another called S-waves (or shear waves). P-waves are faster than S-waves that’s why the first arrival of disturbance waves will be related to the velocities of the P-waves in various soil layers.

Seismic Refraction Survey
Figure 3.45a Seismic Refraction Survey

The velocity of the P-wave:

\upsilon \text{ }=\text{ }\sqrt{\frac{{{E}_{s}}}{\left( \frac{\gamma }{g} \right)}\frac{\left( 1-{{\mu }_{s}} \right)}{\left( 1-2{{\mu }_{s}} \right)\left( 1+{{\mu }_{s}} \right)}} \tag{3.79}

Where

Es = modulus of elasticity of the medium
γ = unit weight of the medium
g = acceleration due to gravity
μs = Poisson’s ratio

Seismic Reflection Survey Method

Step 1:  Obtain the times of the first arrival, t1, t2, t3, t4,. . . ., at various distances x1, x2, x3, x4,. . . , from the point of the impact.

Step 2: Plot a graph of time t against distance x. The graph will look like the below Figure 3.45b.

Step 3: Calculate the slopes of the lines 0a, ab, bc, ….., :

Slope\text{ }of\text{ }0a=\frac{1}{{{\upsilon }_{1}}}
Slope\text{ }of\text{ }ab=\frac{1}{{{\upsilon }_{2}}}
Slope\text{ }of\text{ }bc=\frac{1}{{{\upsilon }_{3}}}

    Here, {{\upsilon }_{1}},\text{ }{{\upsilon }_{2}},\text{ }{{\upsilon }_{3}}, . . . . , are p-wave velocities in layers I, II, III, . . . . ., respectively (see figure 3.45a).

Seismic Refraction Survey
Figure 3.45b Seismic Refraction Survey

Step 4: Determine top layer thickness:

\tag{3.80}{{Z}_{1}}=\frac{1}{2}\sqrt{\frac{{{\upsilon }_{2}}-{{\upsilon }_{1}}}{{{\upsilon }_{2}}+{{\upsilon }_{1}}}}{{x}_{c}}

The value of {{x}_{c}} can be obtained from the plot which is shown in Figure 3.45b.

Step 5: Determine the second layer thickness:

\tag{3.81}{{Z}_{2}}=\frac{1}{2}\left[ {{T}_{i2}}-2{{Z}_{1}}\frac{\sqrt{\upsilon _{3}^{2}-\upsilon _{1}^{2}}}{{{\upsilon }_{3}}{{\upsilon }_{1}}} \right]\frac{{{\upsilon }_{3}}{{\upsilon }_{2}}}{\sqrt{\upsilon _{3}^{2}-\upsilon _{2}^{2}}}

Note: If you have trouble viewing the equation then view the page in desktop mode in your mobile browser.

Here, {{T}_{i2}} is the time intercept of the line cd in Figure 3.45b, extended backward.

(For detailed derivations of this equation and other related information, see the research paper “Dobrin, 1960, and Das, 1992”.)

P-waves velocities indicate the types of soil or rock in various layers that are present below the ground surface. The range of the p-wave velocity that is encountered in different types of soil and rock at shallow depths is given below in Table 3.12.

Table 3.12: Range of P-Wave Velocity in Various Soil and Rocks

P-Wave Velocity in Various Soil and Rocks
Range of P-Wave Velocity in Various Soil and Rocks

In Seismic refraction survey there have two limitations and that must be kept in mind when analyze the results.

Seismic Refraction Survey Limitations:

  1. The general equation for the survey – that is eq. (3.80) and eq. (3.81) – are base on the assumption that the P-wave velocity {{\upsilon }_{1}}<{{\upsilon }_{2}}<{{\upsilon }_{3}}<.....
  2. When a soil is saturated below the water table, the p-wave velocity may be incorrect. Through water, P-wave can travel with a velocity of about 1500 m/s. For dry soil, loose soil, the velocity may be well below 1500 m/s. However, in a saturated soil condition, the waves will travel through water that is present in the void space with a velocity of about 1500m/s. If the presence of groundwater has not been detected, then the p-wave velocity may be erroneously interpreted that indicating a stronger material like sandstone is actually present in situ. In general, geophysical results should always be verified by the result obtained from the soil boring test.

Now, at the end of this session, an example problem is given below for perfect understanding.

Example:

The result of a seismic refraction survey at a site are given below:

Distance of geophone from the source of disturbance (m)Time of first arrival (t x 10­­­-3)
2.511.2
523.3
7.533.5
1042.4
1550.9
2057.2
2564.4
3068.6
3571.1
4072.1
5075.5
seismic refraction survey site data

Solution:

Velocity Calculation

Seismic refraction survey site data
first arrival time of P wave versus distance of geophone from source
of disturbance

In Figure 3.46, the time of the first arrival of p-waves is plotted against the distance of the geophone from the source of disturbance (explosion or hammering). The plotted graph has three straight-line segments. The velocity of the top three layers can be calculated as:

Slope of segment:

0a=\frac{1}{{{\upsilon }_{1}}}=\frac{\text{time}}{\text{distance}}=\frac{23\times {{10}^{-3}}}{5.25}
{{\upsilon }_{1}}=\frac{5.25}{23\times {{10}^{-3}}}=228\text{ m/s (top layer)}

Slope of segment:

ab=\frac{1}{{{\upsilon }_{2}}}=\frac{13.5\times {{10}^{-3}}}{11}
{{\upsilon }_{2}}=\frac{11}{13.5\times {{10}^{-3}}}=814.8\text{ m/s (middle layer)}

Slope of segment:

bc=\frac{1}{{{\upsilon }_{3}}}=\frac{3.5\times {{10}^{-3}}}{14.75}
{{\upsilon }_{3}}=\frac{14.75}{3.5\times {{10}^{-3}}}=4214\text{ m/s (third layer)}

After analysis of the results given in Table 3.12, it indicates that the third layer is a Rock Layer.

Thickness of Layers

From Figure 3.46, {{x}_{c}}=10.5m , So

{{Z}_{1}}=\frac{1}{2}\sqrt{\frac{{{\upsilon }_{2}}-{{\upsilon }_{1}}}{{{\upsilon }_{2}}+{{\upsilon }_{1}}}}{{x}_{c}}

Thus,

{{Z}_{1}}=\frac{1}{2}\sqrt{\frac{814.8-228}{814.8+228}}\times 10.5=3.94m

Again, from (Eq. 3.81),

{{Z}_{2}}=\frac{1}{2}\left[ {{T}_{i2}}-2{{Z}_{1}}\frac{\sqrt{\upsilon _{3}^{2}-\upsilon _{1}^{2}}}{{{\upsilon }_{3}}{{\upsilon }_{1}}} \right]\frac{{{\upsilon }_{3}}{{\upsilon }_{2}}}{\sqrt{\upsilon _{3}^{2}-\upsilon _{2}^{2}}}

The value of {{T}_{i2}} (from figure 3.46) is 65 x 10-3 s. Hence,

{{Z}_{2}}=\frac{1}{2}\left[ 65\times {{10}^{-3}}-2\times 3.94\frac{\sqrt{{{4214}^{2}}-{{228}^{2}}}}{4214\times 228} \right]\frac{4214\times 814.8}{\sqrt{{{4214}^{2}}-{{814.8}^{2}}}}=12.66m

Thus, the rock layer lies from the surface of the ground at a depth of:

{{Z}_{1}}+{{Z}_{2}}=3.94+12.66=16.60m

Note: Equations and the number of equations which used in this article are taken from reference section source.

See this video to learn more about “what is seismic reflection?”

What is seismic reflection?

Watch this video for how to do seismic reflection surveys practically on the site.

seismic reflection surveys practically on the site

Reference:

Principles of Foundation Engineering (Ninth edition, 2019), “Braja M. Das, University Sacramento”, “Nagaratnam Sivakugan, College of Science & Engineering James Cook University”

FAQ

What is seismic refraction survey?

Seismic refraction survey is a method of determining the classification of soil (e.g. clay, silt, sandstone, granite, etc.) and the thickness of various soil layers by using an artificial seismic such as a small explosion or hammering.

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Arjun Barman,CE

Arjun Barman,CE

Meet Arjun Barman, a civil engineering enthusiast on a mission to become a structural engineering maestro. With an unwavering passion for the art of building, Arjun shares his expertise and love for civil engineering through his engaging writing. Join him on his exciting journey through the world of structures, as he simplifies the complexities and makes the wonders of civil engineering come to life, one article at a time. Direct contact: [email protected]

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