Recall: Recall: State of stress surrounding anState of stress surrounding anarbitrarily deviated wellarbitrarily deviated well
© Cambridge University Press (Fig. 8.1b, pp. 237)Zoback, Reservoir Geomechanics
Stresses in the wellbore coordinate systemStresses in the wellbore coordinate system
=RB
⎡
⎣⎢⎢
cos δ cosϕ
− sin δ
cos δ sinϕ
sin δ cosϕ
cos δ
sin δ sinϕ
− sinϕ
0
cosϕ
⎤
⎦⎥⎥
=SB RBSGRTB
= ( S )SB RB RTG RG R
TB
Stress at wellbore wallStress at wellbore wall
σzz
σθθ
τθz
σrr
= − 2ν( − ) cos 2θ − 4ν sin 2θσ33 σ11 σ22 σ12
= + − 2( − ) cos 2θ − 4 sin 2θ − ΔPσ11 σ22 σ11 σ22 σ12
= 2( cos θ − sin θ)σ23 σ13
= ΔP
Principal e�ective stresses around thePrincipal e�ective stresses around thewellborewellbore
σtmax
σtmin
= ( + + )1
2σzz σθθ ( − + 4σzz σθθ)2 τ2
θz‾ ‾‾‾‾‾‾‾‾‾‾‾‾‾‾‾‾√
= ( + − )1
2σzz σθθ ( − + 4σzz σθθ)2 τ2
θz‾ ‾‾‾‾‾‾‾‾‾‾‾‾‾‾‾‾√
Example: Reverse faultingExample: Reverse faulting
Find the minimum and maximum tangential stress for an open hole well that is oriented from North and deviated from vertical at a depth of km. Assume a hydrostatic porepressure gradient, a Poisson ration of , and a balanced drilling operation.
S =
⎡
⎣⎢⎢
30
0
0
0
25
0
0
0
20
⎤
⎦⎥⎥
α
β
γ
= 90∘
= 0∘
= 0∘
Azimuth of SHmax
=S1 SHmax
=S2 Shmin
20∘
20∘ 2
0.2
© Cambridge University Press (Fig. 8.1a, pp. 237)Zoback, Reservoir Geomechanics
Lower hemisphere projectionLower hemisphere projection
© Cambridge University Press (Fig. 8.1a, pp. 237)Zoback, Reservoir Geomechanics
Examples: Breakout initiationExamples: Breakout initiation
Normal Strike-slip Reverse
© Cambridge University Press (Fig. 8.2a,b,c, pp. 240)Zoback, Reservoir Geomechanics
Examples: Drilling induced tensile fractureExamples: Drilling induced tensile fracture
Normal Strike-slip Reverse
© Cambridge University Press (Fig. 8.3a,b,c, pp. 240)Zoback, Reservoir Geomechanics
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