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2. Coulomb’s law of failure

Hydraulic fracturing results from a pulling apart or tensile failure of the rock mass, but natural earthquakes are caused by sliding or shear failure along a plane. Many data on shear failure under compressive stress are available from the results of triaxail tests. (In the Earth below 100- to 200-m depth all stresses are compressive). In triaxial tests a piston apparatus is used to place a cylindrical volume of rock under a directed compressive stress that defines σ1, while the value of σ3 is controlled by the fluid pressure in a surrounding vessel. For any given value of σ3, the value of σ1 can be increased until the sample fails along a plane located at some angle θ to the axis of compression (Figure 5.2a). For many geologic media θ ~ 30°.

For a uniform confining pressure σ3 it is possible to plot the stress conditions at failure on a two-dimensional Mohr diagram, a graphic representation of the state introduced by the German engineer Otto Mohr in 1882. The Mohr circle defines the normal (σn) and shear (τ) stresses on the failure plane itself, provided that σ1, σ3, and θ are known, as they are in the case of failure in triaxial tests (Figure 10.2b). A Mohr circle with radius (σ13)/2 is centered on the abscissa at (σ1+σ3)/2. A line is drawn from the center of the circle at an angle of 2θ relative to the abscissa. The intercept between this radial line and the circle defines σn and τ on the failure plane, that is,

(5.5)

and

(5.6)

Under compression the values σ1 and σ3 are both taken as positive, as shown on Figure 10.2b. Under pure tension, σ1 is positive and σ3 is zero. Under pure shear, σ1 is positive and σ3 is negative.

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Thus, the position of the Mohr circle along the abscissa indicates the type of stress state. The size of the circle indicates the magnitude of the difference between σ1 and σ3 and is a measure of the differential stress.

For numerous experiments, conditions at failure are well described by Coulomb’s law of failure,

, (5.7)

where φ is called the angle of internal friction and is often about 30°. Thus tan φ, which is also known as the coefficient of friction, typically has a value of about 0.6. The French military engineer and physicist Charles Augustine de Coulomb predicted this relationship in the 1770s. At that time it was already known that

, (5.8)

described the behavior of noncohesive materials such as sand; Coulomb’s insight was to add the constant τ0 to represent the intact shear resistance of a cohesive material. The Coulomb failure line described by Eq. (5.7) bounds a region of stability on Figure 5.2b Mohr circles that touch the failure line describe conditions required to induce failure.

Although Coulomb’s law of failure describes many experimental results well, it remains a fundamentally empirical relation, because it is not yet possible to predict macroscopic failure behavior from molecular-scale behavior or from first principles (e.g., Scholz, 1990; Marder and Fineberg, 1996).

An apparent discrepancy between the failure behavior of drained and undrained fluid-saturated samples troubled early students of rock mechanics. In “drained tests” on saturated material, applied stresses are increased slowly and water is allowed to escape from the sample, and the results were similar in most respects to those obtained for dry samples. “Undrained tests”, in which the contained water is retained by an impermeable jacket, gave apparent φ values of ~0° (i.e., the failure criterion of Eq. (5.7) was defined by a horizontal line). By the 1950s it was recognized that the apparent discrepancy between drained and undrained behavior disappeared if, in the case of saturated samples, effective stresses were plotted on the abscissa of the Mohr diagram (i.e., σ1 Pf , σ3 Pf).

-28-

To summarize, then, in triaxial tests any sample can eventually be made to fail by increasing σ1 with σ3 held constant (Figure 10.3a) and/or by decreasing σ3 with σ1 constant (Figure 10.3b). Fluid-saturated samples can also be brought to failure by increasing the internal fluid pressure Pf . Varying σ1 or σ3 can induce failure by increasing the differential stress on the sample, an effect expressed on the Mohr diagram as an increase in the size of the Mohr circle. Increasing fluid pressure does not affect the shear stress but induces failure by decreasing the effective strength of the sample. This is expressed by shifting the circle toward the origin without changing its size (Figure 5.3c).

Figure 5.3 Mohr diagrams showing failure conditions induced by (a) increasing the greatest principal stress σ1, (b) decreasing the least principal stress σ3, and (c) increasing the internal pore-fluid pressure Pf. In each case the σ1 and σ3 values plotted on the abscissa are actually the effective stresses, that is stress σ1 - Pf and σ3 - Pf.

-29-

Glossary ” Relationship between hydrogeology and seismic activity”.

effective stress

действительное напряжение, эффективное напряжение

to credit

приписывать (кому-л. совершение какого-л. действия)

Coulomb's law

закон Кулона

downward force

сила, направленная вниз

tensile strength

предел прочности на разрыв

parting

поверхность стыка, отделение; разделение; разветвление; междупластье; тонкий прослой породы, пропласток

overburden weight

давление покрывающих пластов

tensile failure

разрушение при растяжении; разрыв

mutually orthogonal

взаимно ортогональный

orthogonal

ортогональный, прямоугольный

principal stresses

главные напряжения

thrust-fault

надвиг

deviator stress

девиаторное напряжение

arbitrary

произвольный, случайный

aligned

выровненный, ориентированный

off-diagonal

недиагональный

vigorous

сильный, энергичный; решительный

indistinguishable

неотличимый ( from)

-30-

shear failure

разрушение при сдвиге, разрушение при срезе

triaxial

трёхосный

piston

поршень

vessel

1) сосуд (для жидкости); 2) корабль, судно; летательный аппарат

abscissa

абсцисса; ось абсцисс

relative

относительный, сравнительный, взаимный (о расположении)

intercept

пересечение

insight

проницательность; способность проникновения в суть ( into)

intact

нетронутый; незатронутый, неповрежденный, невредимый, целый Syn: entire

region of stability

область стабильности

discrepancy

разница; различие, несходство, отличие (between; in) Syn: difference

disclosed

раскрытый

annual

ежегодный; годичный, годовой

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