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25th International Meeting on Organic Geochemistry IMOG 2011

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P-325<br />

Origin of abnormal s<strong>on</strong>ic resp<strong>on</strong>se in the shale interval of<br />

Northern S<strong>on</strong>gliao Basin, China<br />

Huo Qiuli, Zeng Huasen, Fu Li, Ren Zhigao, Fan Qinghua, Zhang Xiaochang<br />

Explorati<strong>on</strong> and Development Research Institute, Daqing Oilfield Company Ltd., PetroChina, Daqing, China<br />

(corresp<strong>on</strong>ding author:yjydh206@yahoo.com.cn)<br />

The deviati<strong>on</strong> of s<strong>on</strong>ic transit time log from normal<br />

trend in the shale interval has been widely interpreted<br />

as overpressure since Magara (1978). The<br />

prerequisite for the relati<strong>on</strong>ship between s<strong>on</strong>ic transit<br />

time and overpressure is that overpressure is induced<br />

by undercompacti<strong>on</strong> or disequilibrium. The origin of<br />

overpressure is still in c<strong>on</strong>troversial, however. Aplin et<br />

al.(1995) suggested that the relati<strong>on</strong>ship of porosity<br />

vs. depth was influenced by lithology heterogeneity.<br />

Another example is that overpressure can exist in the<br />

shale interval of normal pressure (e.g. Teige et al.,<br />

1999, Hao et al., 2007). It seems that overpressure<br />

and the deviati<strong>on</strong> of s<strong>on</strong>ic transit time log from normal<br />

trend are not necessary closely correlated. The<br />

deviati<strong>on</strong> of s<strong>on</strong>ic transit time log from normal trend is<br />

widespread in the shale interval of Qingshankou<br />

formati<strong>on</strong> at the basin scale, especially <strong>on</strong> the bottom<br />

of Qingshankou 1st member (K2qn1) which is the<br />

main source rock in the S<strong>on</strong>gliao Basin. In most of<br />

past studies (e.g. Wang, 1984, Chi et al., 2000, Xiang<br />

et al., 2006), those deviati<strong>on</strong>s of s<strong>on</strong>ic transit time are<br />

c<strong>on</strong>sidered to be induced by overpressure of shale<br />

based <strong>on</strong> undercompacti<strong>on</strong> or disequilibrium<br />

mechanisms, and as the main force that migrated the<br />

oil generated from K2qn1 downward to the underlying<br />

Fuyang reservoirs. However, our recent studies<br />

showed that the deviati<strong>on</strong>s of s<strong>on</strong>ic transit time may<br />

be more closely correlated to the organic carb<strong>on</strong><br />

c<strong>on</strong>tent in the shale interval which has never been<br />

noticed before. Profiles of s<strong>on</strong>ic log and total organic<br />

carb<strong>on</strong> c<strong>on</strong>tent (TOC) of three representable wells<br />

with different organic maturities, which excludes the<br />

hydrocarb<strong>on</strong> generati<strong>on</strong> origin of overpressure, show<br />

that the s<strong>on</strong>ic log nearly traces the TOC profile in<br />

each well (see Fig. 1). It is accordingly believed that<br />

the deviati<strong>on</strong> of s<strong>on</strong>ic log is induced by organic<br />

c<strong>on</strong>tent heterogeneity in the shale interval (i.e.<br />

lithology heterogeneity). The s<strong>on</strong>ic transit time of<br />

shale in K2qn1 with different burial depths was then<br />

plotted by depth in Fig. 2 to decrease the effect of<br />

lithology heterogeneity. The result is obvious and the<br />

s<strong>on</strong>ic transit time decreases as the depth increases<br />

without any deviati<strong>on</strong>, which corroborated that the<br />

s<strong>on</strong>ic transit time deviati<strong>on</strong> in the shale interval is<br />

most likely the result of lithology heterogeneity<br />

(organic c<strong>on</strong>tent) instead of overpressure induced by<br />

undercompacti<strong>on</strong> or disequilibrium.<br />

Fig. 1 S<strong>on</strong>ic transit time and TOC profiles by depth in the<br />

S<strong>on</strong>gliao Basin. TOC log were calculated using method<br />

described by Passey et al.(1990) while calibrated by<br />

measured data (solid circle). SK-I is a scientific drilling well<br />

from ICDP project. Ro is the reflectance of vitrinite.<br />

Depth(m)<br />

0 60 120 180<br />

0<br />

Du 401<br />

500<br />

1000<br />

1500<br />

2000<br />

2500<br />

Jin 37<br />

Gu 302<br />

S<strong>on</strong>icTransit Time(us/ft)<br />

Shengshen 2<br />

Si 103<br />

Shuang 11<br />

Fig. 2 S<strong>on</strong>ic transit time (of shale) profile by depth in the<br />

K2qn1. Short horiz<strong>on</strong>tal lines are the s<strong>on</strong>ic transit time<br />

ranges.<br />

References<br />

1.Aplin, A.C., Yang, Y., Hansen, S., 1995. Assessment of<br />

[beta] the compressi<strong>on</strong> coefficient of mudst<strong>on</strong>es and its<br />

relati<strong>on</strong>ship with detailed lithology. Marine and Petroleum<br />

Geology 12, 955-963.<br />

2.Magara, K., 1978. Compacti<strong>on</strong> and Fluid Migrati<strong>on</strong>.<br />

Elsevier Science & Technology.<br />

458

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