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World Stress Map Conference - International Lithosphere Program ...

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Wednesday, October 15 th<br />

Oral Session I: <strong>Stress</strong> and rock strength measurements – techniques and results<br />

Constraining the magnitude of the maximum horizontal stress<br />

in the Taiwan Chelungpu-fault Drilling Project (TCDP) from<br />

borehole breakout dimensions and rock true triaxial strength<br />

Bezalel Haimson and Haruyuki Oku<br />

University of Wisconsin, Madison, WI, USA<br />

bhaimson@wisc.edu<br />

Weiren Lin<br />

Japan Agency for Marine-Earth Science and Technology, Kochi, Japan<br />

Sheng-Rong Song<br />

Department of Geoscience, National Taiwan University, Taiwan<br />

Borehole breakout traces identified on geophysical logs have been primarily used as an important in<br />

situ stress direction indicator. They provide indispensable data required for the construction of the<br />

<strong>World</strong> <strong>Stress</strong> <strong>Map</strong>. In addition, cross sections of breakout angular spans at vertical borehole perimeters<br />

have been shown to be directly related to the magnitudes of the in situ principal stresses (Song and<br />

Haimson, IJRMMS, 1997). However, the explicit relationship requires knowledge of the rock strength<br />

criterion, because of the reasonable assumption that the points of intersection between breakout and<br />

borehole wall cross section represent the boundary between stable rock on the outside of the breakout<br />

and failed rock on the inside. Equating the correct strength criterion to the state of stress at the points<br />

of intersection, one obtains an equation in terms of the three in situ principal stresses. Two of the in<br />

situ principal stresses are typically determined from the gravitational gradient (σv) and from leak-off<br />

or hydrofracturing tests (σh). Thus, the only unknown variable is the maximum horizontal in situ stress<br />

σH. Vernik and Zoback (JGR, 1992) showed that the commonly used Mohr-Coulomb strength<br />

criterion, which ignores the effect of the intermediate principal stress, was not applicable to borehole<br />

walls, where the local principal stresses are widely differential. Rather, a true triaxial compressive<br />

strength criterion that takes in consideration all three principal stresses is necessary. At the University<br />

of Wisconsin, we had designed and fabricated an apparatus for determining the true triaxial strength of<br />

rectangular prismatic specimens subjected to three unequal principal stresses and used it originally to<br />

obtain a generalized strength criterion for the amphibolite in the KTB scientific ultra deep well,<br />

Germany. Equating the criterion to the state of stress at the points of borehole-breakout intersections<br />

yielded the magnitudes of σH between 3200-6800 m depth (Haimson and Chang, JGR, 2002). The<br />

present paper describes the computation of the σH magnitude in the vicinity of the Chelungpu Fault,<br />

Taiwan, host of the slip zone during the Chi-Chi earthquake (Mw 7.6; 1999). The TCDP scientific<br />

hole B intercepts the Fault at 1136 m. Within the depths of logged breakouts (930-1300 m), the<br />

vertical stress σv as estimated from density logs varied between 22 and 30 MPa. Within the same<br />

depth range, two pairs of leak-off tests, one above and one below the fault, yielded σh magnitudes<br />

between 16 and 24 MPa (Hung et al., Tectonophysics, 2007). A series of true triaxial tests on the<br />

Chinshui siltstone straddling the 30°-east dipping Fault yielded a strength criterion relating the<br />

octahedral shear stress to the mean normal stress on the failure plane:<br />

[ ] 49 . 0<br />

0.<br />

5 ( σ<br />

1 2<br />

2<br />

2<br />

3 ( σ 1 − σ 2)<br />

+ ( σ 2 −σ<br />

3)<br />

+ ( σ 3 −σ<br />

1)<br />

= 5.<br />

66 3 + σ 3)<br />

. The principal stresses σ1>σ2>σ3 at the<br />

breakout-borehole wall intersection are represented by σθ > σz > σr, and these are related to the in situ<br />

principal stresses σH, σh, and σv by the well-known Kirsch solution. By substituting the known σh and<br />

σv at each breakout depth, a non-linear equation was obtained in terms of one unknown: σH. Solving<br />

the equation using Newton’s numerical method yielded estimates of σH varying between 48 and 56<br />

MPa, indicating that the stress condition presently prevailing along the Chelungpu Fault favors strikeslip<br />

faulting, bordering on thrust faulting.<br />

22 3 rd <strong>World</strong> <strong>Stress</strong> <strong>Map</strong> <strong>Conference</strong>, 15.-17. October 2008 in Potsdam

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