Direct Measurements of Wave Dispersion at Seismic Frequencies and Gassmann Fluid Substitution

Author(s):  
X. Wei ◽  
S.X. Wang ◽  
J.G. Zhao ◽  
G.Y. Tang ◽  
H.J. Yin
2014 ◽  
Vol 2 (2) ◽  
pp. 106-114
Author(s):  
Sonny Inichinbia ◽  
◽  
Peter O. Sule ◽  
Aminu L. Ahmed ◽  
Halidu Hamza

2021 ◽  
Author(s):  
Ranjith Kunnath

<p>A model that explains the anomalies in the Love wave dispersion in the earth is presented. Conventionally, welded contact between the crust and the upper mantle is assumed, leading to Love wave generation when the earth is excited. However, the observations of SH wave dispersion at seismic frequencies is at variance with this model, at least for some crustal plates (Ekström, 2011). When frictional slip occurs at the crust-upper mantle interface, a new type of interfacial elastic wave called the antiplane slip wave can occur (Ranjith, 2017). It is shown that the antiplane slip waves can explain the observed anomalies in the Love wave dispersion. </p>


Geophysics ◽  
2010 ◽  
Vol 75 (3) ◽  
pp. N65-N78 ◽  
Author(s):  
Ida L. Fabricius ◽  
Gregor T. Bächle ◽  
Gregor P. Eberli

Elastic moduli of water-saturated sedimentary rocks are in some cases different from moduli derived using Gassmann fluid substitution on data for rocks in the dry state. To address this discrepancy, we use a data set representing 115 carbonate samples from different depositional settings and a wide range of porosity and permeability. Depositional texture is reflected in the effect of water on elastic moduli and in the porosity-permeability relationship. Depositional texture is taken into account when porosity and permeability are combined in the effective specific surface of pores, which is related for a given pore fluid to the reference frequency as defined by Biot. For a given frequency of elastic waves, we obtain Biot’s frequency ratio between measured ultrasonic wave frequency and Biot reference frequency. For mostsamples with a frequency ratio above 10, elastic moduli in the water-saturated case are higher than predicted from elastic moduli in the dry case by Gassmann fluid substitution. This stiffening effect of water in some cases may be described by Biot’s high-frequency model, although in heterogeneous samples, a squirt mechanism is more probable. For data representing frequency ratios of 0.01 to 1, Gassmann fluid substitution works well. For samples with frequency ratios below 0.001, elastic moduli in the water-saturated case are lower than would be expected according to Gassmann’s equations or to Biot’s theory. This water-softening effect becomes stronger with decreasing frequency ratio. Water softening or stiffening of elastic moduli may be addressed by effective-medium modeling. In this study, we used the isoframe model to quantify water softening as a function of frequency ratio.


2014 ◽  
Vol 40 (1) ◽  
pp. 181-193 ◽  
Author(s):  
Aamir Ali ◽  
Muhammad Kashif ◽  
Matloob Hussain ◽  
Jamil Siddique ◽  
Irfan Aslam ◽  
...  

Geophysics ◽  
2009 ◽  
Vol 74 (5) ◽  
pp. WB89-WB95 ◽  
Author(s):  
Vladimir Grechka

It is usually believed that Gassmann fluid substitution can be performed only for a fully interconnected portion of the pore space. While this is certainly true, the presence of disconnected porosity does not necessarily invalidate Gassmann’s predictions. This unconventional view is supported with an analytic proof of the equivalence of Gassmann theory and the noninteraction approximation for the effective elasticity of solids with isolated self-similar pores. Numerical tests for more realistic microgeometries, where pores have diverse shapes and the pore space is partially disconnected, demonstrate that errors in Gassmann-type infill substitution are typically small and unlikely to exceed a few percent as long as the aspect ratios of pores are greater than approximately 0.2. If the fracture-like pores are aligned or elasticities of the substituted infills are close, Gassmann theory remains accurate for isolated pores with smaller aspect ratios.


2021 ◽  
pp. 1-8
Author(s):  
Ranjith Kunnath

Abstract Conventional models of the structure of the earth, such as the Preliminary Reference Earth Model (PREM), assume a bonded interface between the crust and the upper mantle. The bonded contact model is consistent with the observation of Love waves during an earthquake. However, anomalies in the Love wave dispersion have been reported in the literature. When slip occurs at the crust-mantle interface, another kind of an interfacial wave, called the slip wave can exist. It is shown that the dispersion relation of the slip wave, with a slip weakening friction law, appears to be in agreement with the observations at seismic frequencies. This suggests that slip could occur at the crust-mantle interface.


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