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reservoir geomecanics

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280 Reservoir geomechanics<br />

Methods for approximating S hmin in normal faulting areas<br />

In Chapter 7 we discussed how mini-frac and leak-off tests can be used to accurately<br />

determine the magnitude of the least principal stress, S hmin . Knowledge of the least principal<br />

stress is not only a critical step in determining the full stress tensor (as discussed<br />

at length in Chapters 7 and 8), it also provides important information for drilling stable<br />

wells. During drilling, mud weights must be kept below S hmin to prevent accidental<br />

hydraulic fracturing and lost circulation, but above both the pore pressure (to avoid taking<br />

a kick) and the minimum mud weight required to prevent excessive wellbore failure<br />

(i.e. the collapse pressure) as discussed in Chapter 10. Because of this, a number of<br />

empirical techniques have been proposed for estimating the least principal stress in the<br />

absence of direct measurements. This issue is particularly important in normal faulting<br />

areas (such as the Gulf of Mexico) where overpressure is present at depth. As illustrated<br />

in Figure 1.4d, in overpressured normal faulting regions, there can be extremely small<br />

differences between P p and S hmin , which define the mud window, orthe safe range of<br />

pressures to use while drilling.<br />

In the sections below, the techniques summarized in Table 9.1 for estimating the<br />

least principal stress (or least principal effective stress) in the Gulf of Mexico are<br />

briefly discussed.<br />

In their classic paper on hydraulic fracturing, Hubbert and Willis (1957) proposed<br />

an empirical expression for the magnitude of the least principal stress as a function of<br />

depth in the Gulf of Mexico region,<br />

S hmin = 0.3(S v − P p ) + P p (9.1)<br />

where the constant 0.3 was empirically determined from the analysis of hydraulic fracturing<br />

data. The scientific basis for this constant can be understood in terms of frictional<br />

faulting theory (Zoback and Healy 1984), as equation (4.45) produces essentially the<br />

same equation for a coefficient of friction of 0.6. However, as additional data became<br />

available for the offshore Gulf of Mexico area, Hubbert and Willis later adopted an<br />

empirical coefficient of 0.5 indicating that observed values for the least principal stress<br />

in the Gulf of Mexico generally exceed the values predicted using equation (4.45) with<br />

a coefficient of friction of 0.6.<br />

Matthews and Kelly (1967) proposed a similar relation for the fracture pressure,<br />

or the magnitude of the pore pressure at which circulation is lost. As this requires<br />

propagation of a hydraulic fracture away from the wellbore, this value is essentially<br />

equivalent to the least principal stress. Thus, they proposed<br />

S hmin = K i (S v − P p ) + P p (9.2)<br />

where K i is a function of depth, z. Using this relation, functions for the Louisiana gulf<br />

coast and south Texas gulf coast region were proposed that varied in a non-linear fashion

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