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reservoir geomecanics

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102 Reservoir geomechanics<br />

Drucker–Prager criterion<br />

The extended von Mises yield criterion, or Drucker–Prager criterion, was originally<br />

developed for soil mechanics (Drucker and Prager 1952). The von Mises criterion may<br />

be written in the following way<br />

J 2 = k 2 (4.25)<br />

where k is an empirical constant. The yield surface of the modified von Mises criterion in<br />

principal stress space is a right circular cone equally inclined to the principal stress axes.<br />

The intersection of the π-plane with this yield surface is a circle. The yield function<br />

used by Drucker and Prager to describe the cone in applying the limit theorems to<br />

perfectly plastic soils has the form:<br />

J 1/2<br />

2<br />

= k + α J 1 (4.26)<br />

where α and k are material constants. The material parameters α and k can be determined<br />

from the slope and the intercept of the failure envelope plotted in the J 1 and (J 2 ) 1/2<br />

space. α is related to the internal friction of the material and k to the cohesion of<br />

the material. In this way, the Drucker–Prager criterion can be compared to the Mohr–<br />

Coulomb criterion. When α is equal to zero, equation (4.26) reduces to the von Mises<br />

criterion.<br />

The Drucker–Prager criteria can be divided into an outer bound criterion (or circumscribed<br />

Drucker–Prager) and an inner bound criterion (or inscribed Drucker–<br />

Prager). These two versions of the Drucker–Prager criterion come from comparing<br />

the Drucker–Prager criterion with the Mohr–Coulomb criterion. In Figure 4.6 the two<br />

Drucker–Prager criteria are plotted in the π-plane. The inner Drucker–Prager circle<br />

only touches the inside of the Mohr–Coulomb criterion and the outer Drucker-Prager<br />

circle coincides with the outer apices of the Mohr–Coulomb hexagon.<br />

The inscribed Drucker–Prager criterion is obtained when (Veeken, Walters et al.<br />

1989; McLean and Addis 1990)<br />

3sin φ<br />

α = √ (4.27)<br />

9 + 3sin 2 φ<br />

and<br />

3C 0 cos φ<br />

k =<br />

2 √ q √ 9 + 3sin 2 φ<br />

(4.28)<br />

where φ is the angle of internal friction, as defined above.<br />

The circumscribed Drucker–Prager criterion (McLean and Addis 1990; Zhou 1994)<br />

is obtained when<br />

6 sin φ<br />

α = √ (4.29)<br />

3 (3 − sin φ)

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