2014
DOI: 10.1190/tle33060640.1
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Seismic attenuation in partially saturated rocks: Recent advances and future directions

Abstract: The large amount of data collected with the broadband attenuation vessel (BBAV) and other laboratory devices and analyzed in the last five years sheds light on the physics of wave-induced fluid flow in Berea Sandstone. However, the knowledge is insufficient to fully exploit the physics of seismic wave attenuation in partially saturated rocks. In particular, some technical challenges have limited the depth of research. Soon these challenges will be overcome by the use of fluid-pressure sensors capable of measur… Show more

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Cited by 29 publications
(8 citation statements)
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“…Waves generate fluid flow in the pores and energy losses that can be observed in field and laboratory experiments [2][3][4]. Recent laboratory experiments performed in the seismic range have shown the frequency dependence of anelasticity in sandstones with partial gas or oil saturations [5][6][7], while experiments conducted in Reference [8] show a significant attenuation in the extensional and bulk deformation modes, as well as numerical simulations in close agreement with laboratory data.…”
Section: Introductionsupporting
confidence: 64%
“…Waves generate fluid flow in the pores and energy losses that can be observed in field and laboratory experiments [2][3][4]. Recent laboratory experiments performed in the seismic range have shown the frequency dependence of anelasticity in sandstones with partial gas or oil saturations [5][6][7], while experiments conducted in Reference [8] show a significant attenuation in the extensional and bulk deformation modes, as well as numerical simulations in close agreement with laboratory data.…”
Section: Introductionsupporting
confidence: 64%
“…Nevertheless, wave attenuation characteristics at sonic and ultrasonic frequencies cannot be simply extrapolated to the field‐scale data due to the expected frequency dependency. To make laboratory measurement more closely related to the frequency range of field seismic data, the forced‐oscillation technique was devised to dynamically measure the frequency‐dependent elastic moduli within a broad frequency range (i.e., 10 −3 to kHz) (e.g., Batzle et al, 2006; Fortin et al, 2005, 2014; Madonna et al, 2011; Mikhaltsevitch et al, 2011; Piane et al, 2019; Pimienta et al, 2015a; Quintal et al, 2013; Spencer, 1981; Tisato et al, 2014; Zhao et al, 2013).…”
Section: Introductionmentioning
confidence: 99%
“…∼5 cm in length) than that in the resonance bar technique (e.g. ∼50 cm in length) (Fortin et al ., 2005, 2007; Batzle et al, 2006; Madonna et al ., 2011; Mikhaltsevitch et al ., 2011; Quintal et al ., 2013; Subramaniyan et al ., 2014; Tisato et al ., 2014; Pimienta et al ., 2015a). Basically, the induced strain amplitude of the forced‐oscillation device should be less than 10 −6 to achieve the elastic response of far‐field seismic waves, with the coverage of a wide frequency band (e.g.…”
Section: Introductionmentioning
confidence: 99%