PETROLEUM EXPLORATION AND DEVELOPMENT, 2021, 48(2): 460-468 doi: 10.1016/S1876-3804(21)60037-X

Hydraulic fracturing induced casing shear deformation and a prediction model of casing deformation

LU Qianli1, LIU Zhuang1, GUO Jianchun,1,*, HE Le2, LI Yanchao3, ZENG Ji4, REN Shan5

1. State Key Laboratory of Oil & Gas Reservoir Geology and Exploitation in Southwest Petroleum University, Chengdu 610500, China

2. Downhole Service Company, CCDC, CNPC, Chengdu 610052, China

3. Shale Gas Exploration & Development Project Department, CNPC Chuanqing Drilling Engineering Co., Ltd., Chengdu 610052, China

4. Research Institute of Engineering and Technology, PetroChina Southwest Oil & Gas Field Company, Chengdu 610052, China

5. Chengdu Learn-Practices Technology Co., Ltd., Chengdu 610000, China

Corresponding authors: *E-mail: guojianchun@vip.163.com

Received: 2020-05-18   Online: 2021-04-15

Fund supported: Supported by National Natural Science Foundation of China51904258
Supported by National Natural Science Foundation of China51874250
Project of Science and Technology of Shale Gas Exploration & Development of CCDC2019-JS-941
National Major Project of Science and Technology2016ZX05048-004-006

Abstract

To study the casing deformation (CD) in shale gas well fracturing caused by natural fracture slip, a fracture face stress model is built based on stress analysis, and a CD prediction model is established based on complex function to analyze factors affecting wellbore shear stress and CD. (1) The fracture and wellbore approach angles have significant impacts on the wellbore shear stress. In Weiyuan shale gas field, Sichuan Basin, under the common wellbore approach angle of nearly 90°, the wellbore is subjected to large shear stress and high risk of CD at the fracture approach angle range of 20° to 55° or its supplementary angle range. (2) When the fracture is partially opened, the wellbore shear stress is positively correlated with the fluid pressure, and negatively correlated with the fracture friction coefficient; when the fracture is fully opened, the wellbore shear stress is positively correlated with the natural fracture area. (3) The lower the elastic modulus and the longer the fracture length, the more serious the CD will be, and the Poisson's ratio has a weak influence on the CD. The deformation first increases and then decreases with the increase of fracture approach angle, and reaches the maximum when the fracture approach angle is 45°. (4) At a given fracture approach angle, appropriately adjusting the wellbore approach angle can avoid high shear stress acting on wellbore, and reasonable control of the fluid pressure in the fracture can reduce the CD risk. The shear stress acting on casing is usually much greater than the shear strength of casing, so increasing casing strength or cementing quality have limited effect on reducing the risk of CD. Caliper logging data has verified that the CD prediction model is reliable, so the model can be used to establish risk analysis chart and calculate deformation value, to provide a reference for quick CD risk prediction in fracturing design.

Keywords: shale gas well ; hydraulic fracturing ; natural fracture ; fracture slippage ; casing deformation mechanism ; casing deformation ; risk control

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Cite this article

LU Qianli, LIU Zhuang, GUO Jianchun, HE Le, LI Yanchao, ZENG Ji, REN Shan. Hydraulic fracturing induced casing shear deformation and a prediction model of casing deformation. [J], 2021, 48(2): 460-468 doi:10.1016/S1876-3804(21)60037-X

Introduction

Volume fracturing of horizontal well has become the key technology in shale gas development, and core techniques, represented by "slick water at high pumping rate+soluble bridge plug" and "intensive staged clustering+temporary plugging and diverting", have been widely used[1,2,3]. However, casing deformation (CD) is likely to occur in volume fracturing of horizontal wells[4]. By the end of 2019, 187 wells had been fractured in Changning- Weiyuan area (C-W area), of them, 75 had CD, accounting for 40.1%. Consequently, fracturing was unable to implement in 174 stages[5]. CD will affect the wellbore integ-rity, hinder running down of tools, and even cause some invalid stages, greatly affecting the stimulation efficiency[6,7].

Some studies suggest that the main factors inducing CD in shale gas horizontal wells include natural fracture slippage, casing yield collapse and thermal stress damage[8]. In terms of research on CD caused by natural fracture (NF) slippage shear, Liao et al. analyzed CD characteristics of wells in C-W area based on field stimulation data, and concluded that NF slippage shear was the main cause of CD[9,10,11]. Gao et al. analyzed the influences of fracturing zone, formation slippage, cementing quality, natural fracture and other factors on CD with simulation software[12,13,14,15,16]. Fu et al. analyzed the influence of NF parameters on CD through large-scale physical modeling experiments[17,18]. In general, the previous researches on NF slippage shear induced CD mostly focused on the analysis of the phenomenon and laws of CD, but few studies on NF slipage, stress on casing, deformation mechanism, CD rapid prediction, and response to CD risk during fracturing have been conducted. In this work, in light of NF slip shear induced CD, a formation-fracture-casing stress unit has been established to analyze the mechanical mechanism of CD, a CD calculation model based on the complex function has been worked out to analyze influence factors of CD. The research results can provide an analytical tool for rapid prediction of the deformation position and deformation severity of horizontal well in fracturing engineering design.

1. Stress analysis of CD wellbore

1.1. Stress model of formation-fracture-casing

High-angle natural fractures are common in shale reservoirs of southern Sichuan Basin[11, 19-21]. During the fracturing process of shale reservoir, due to the existence of flow channels such as hydraulic fractures or voids in cement, fracturing fluid may flow into the NF intersecting with the wellbore and make the fluid in fractures rise in pressure[5]. When fluid pressure in fractures increases to a critical value, the resultant force of fracture surface friction and wellbore shear force (the shear force of the wellbore against fracture slippage) will be less than the shear force of formation slippage, and fracture will slip and cause casing deformation. Based on the above physical process, as shown in Fig. 1, the stress model of formation-fracture-casing system was established to study the mechanical mechanism of CD caused by the fracture slippage-shear. In the figure, the angle between the direction of the maximum horizontal principal stress (Oe direction) and the fracture surface in the clockwise direction (referred to as the fracture approach angle) is θ, and the angle between the Oe direction and the horizontal wellbore in the clockwise direction (referred to as the wellbore approach angle) is α. The model assumes that: (1) The horizontal wellbore (in the same horizontal plane) passes through a vertical NF, and fracturing fluid flows into the NF from the wellbore through a flow channel. (2) The horizontal wellbore is composed of casing and cementing sheath; the whole cementing sheath and casing bear the shear stress together, but damaged cementing sheath cannot bear the shear stress. (3) The NF is uncemented, the fluid fills natural fracture when it enters; (4) Fracturing fluid leak-off and fracture propagation are not considered, fluid pressure is equal everywhere in the NF.

Fig. 1.

Fig. 1.   Stress model of formation-fracture-casing system.


Since the NF in the model is assumed to be vertical, the formation vertical stress has no shear stress component on the fracture surface, and the effect of horizontal principal stress on the fracture surface is the main interest of the study. A horizontal square section of casing and formation (Fig. 1b) in the formation-fracture-casing system stress unit model (Fig. 1a) is selected for stress analysis, and 4 sides of the stress unit are indicated by the dotted lines a', b', c', and d' with the length equal to fracture length. In the figure, the x axis is perpendicular to the fracture surface, and the y axis is parallel to the fracture surface. According to the plane stress analysis, the normal stress in the x direction and shear stress in the y direction of the stress unit before fracturing operation can be expressed as follows:

$\left\{ \begin{align} & {{\sigma }_{x}}=0.5({{\sigma }_{\text{H}}}+{{\sigma }_{\text{h}}})-0.5({{\sigma }_{\text{H}}}-{{\sigma }_{\text{h}}})\cos \ 2\theta \\ & {{\tau }_{xy}}=0.5({{\sigma }_{H}}-{{\sigma }_{\text{h}}})\sin \ 2\theta \\ \end{align} \right.$

1.1.1. Partially opened fracture model

Fracturing fluid enters and supports NFs during hydraulic fracturing. When the fracture is partially opened, as shown in Fig. 2a, the fracture surface in the x direction is mainly subjected to the contact force of rocks and the fracture fluid pressure, and the main forces in the y direction are the fracture surface friction force and the wellbore shear force. Assuming that the stress unit is stable, the force balance established in the x direction can be expressed as:

${{\sigma }_{x}}{{A}_{\text{f}}}+{{\tau }_{yx}}{{A}_{\text{f}}}={{p}_{\text{f}}}{{A}_{\text{f}}}+{{\sigma }_{\text{n}}}{{A}_{\text{f}}}+{{\tau }_{yx}}{{A}_{\text{f}}}$

Fig. 2.

Fig. 2.   Stress analysis of the square stress unit.


The force balance in the y direction can be expressed as:

${{\sigma }_{y}}{{A}_{\text{f}}}+{{\tau }_{xy}}{{A}_{\text{f}}}={{\sigma }_{y}}{{A}_{\text{f}}}+f+{{\tau }_{c}}{{A}_{c}}$

Since the near-wellbore stress has been released before cementing, and the cement solidification stress is ignored, when the fracture surface friction force is greater than the shear force on formation in the y direction (b' surface), from Eq. (3), the actual friction force (f) on the fracture surface is equal to the shear force on formation, and the wellbore shear force is zero.

When the fracture surface friction force is less than the shear force on formation in the y direction, the formation will slip along the fracture surface if there is no wellbore in the formation. And if existing, the wellbore will bear part of the shear force to resist the formation slippage, in this case, f is the maximum static friction force (fmax). The shear stress of the wellbore against fracture slippage under current conditions (referred to as the wellbore shear stress) can be calculated from Eq. (3):

${{\tau }_{\text{c}}}=({{\tau }_{xy}}{{A}_{\text{f}}}-{{f}_{\max }})/{{A}_{\text{c}}}$

In the above equation, fmax can be calculated by the fracture surface friction coefficient μ, and the values of which can be 0.6-1.0[5]:

${{f}_{\max }}\text{=}\mu {{\sigma }_{\text{n}}}{{A}_{\text{f}}}$

Assuming that the stress unit is stable, fracture geometric parameters are fixed, the relationship between the fluid pressure inside fracture and the forces in the tangential direction of fracture is shown in Fig. 3. In the figure, with the increase of pf, fmax decreases linearly, f is equal to the shear force on formation in the y direction ${{\tau }_{xy}}{{A}_{\text{f}}}$, and the wellbore shear force is zero. When fmax decreases to ${{\tau }_{xy}}{{A}_{\text{f}}}$, the wellbore will support part of the shear force (${{\tau }_{\text{c}}}{{A}_{\text{c}}}$) to keep the stress unit static, and f is equal to fmax. When pf increases to${{\sigma }_{x}}$, the fracture is fully opened by the fracturing fluid, the rocks on both sides of the fracture are no longer in contact, and f is zero, at this point, the wellbore shear force is equal to${{\tau }_{xy}}{{A}_{\text{f}}}$.

Fig. 3.

Fig. 3.   Relationship between fluid pressure inside fracture and the forces in the tangential direction of fracture.


1.1.2. Model of fully opened fracture

When the NF is fully opened by fracturing fluid, the rocks on both sides of fracture are no longer in contact

(Fig. 2b), the fracture surface is only subjected to pf in the x direction, and f is zero in the y direction, and the shear force in this direction is borne by the wellbore. Therefore, the wellbore shear stress under current conditions can be calculated from Eq. (3):

${{\tau }_{\text{c}}}={{\tau }_{xy}}\frac{{{A}_{\text{f}}}}{{{A}_{\text{c}}}}$

Ac is the area enclosed by the cementing sheath on the section of wellbore and fracture:

${{A}_{c}}=\frac{\pi ({{R}^{2}}-r_{1}^{2})}{\left| \sin \left( \alpha -\theta \right) \right|}$

Ac is the area enclosed by the casing (${{{A}'}_{\text{c}}}$) when the cementing sheath is damaged:

${{{A}'}_{\text{c}}}=\frac{\pi (r_{\text{2}}^{2}-r_{1}^{2})}{\left| \sin \left( \alpha -\theta \right) \right|}$

1.2. Analysis of factors affecting wellbore shear stress

Tables 1 and 2 show the basic welllbore parameters and geological engineering parameters of shale reservoir stimulation in a block of Weiyuan area. In this area, the direction of ground stress is E-W, the maximum horizontal principal stress (σH) is about 75 MPa, the minimum horizontal principal stress (σh) is about 65 MPa, and the direction of horizontal wellbore is approximately parallel to the direction of σh. Comprehensive interpretation results of the ant-body and logging data show that NFs in this block are mostly in N-E strike and about 150 m long on average. The effects of factors, such as approach angle, fracture area, fracture fluid pressure, and fracture friction coefficient on wellbore shear stress were analyzed based on the above data.

Table 1   Basic parameters of horizontal well stimulation in a block of Weiyuan area.

ParameterValueParameterValue
Wellbore diameter215.9 mmCasing (P125 steel)
shear strength
178 MPa
Casing diameter139.7 mmCementing sheath
shear strength
11.5 MPa
Casing wall thickness12.7 mm

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Table 2   Geological engineering parameters of reservoir stimulation in a block of Weiyuan area.

Well
number
Elasticity modulus/
MPa
Poisson’s
ratio
σh/
MPa
σH/
MPa
σH
azimuth/
(°)
Wellbore approach
angle/(°)
Number
of NF
NF
azimuth/
(°)
Average NF
length/m
Number
of CD
Fracture approach
angle at CD
position/(°)
A133 2100.2461.674.3100110536.8-46.0125253.2
A234 1030.2260.771.610090425.8-44.0180245.5
A336 1040.2462.874.110090225.064
A434 1360.2362.073.510090268.031
B137 3340.2770.582.49585635-60.0120338.0-52.0
B230 8040.2265.978.6959040-10.0130
C135 1540.2269.583.89090630.0-65.0300335.0-56.0
C240 8520.2165.078.89090820.0-50.0220150.0

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1.2.1. The approach angle

Fig. 4 shows the relationship curves of fracture approach angle (θ), wellbore approach angle (α) and wellbore shear stress (τc) under the conditions of Af=10 m2, pf=75 MPa, cases of intact cementing sheath and damaged cementing sheath. When the fracture trend is parallel or perpendicular to the direction of the maximum horizontal principal stress (σH), τc is equal to zero, which is independent of α. In other cases, the value of τc is affected by both θ and α. Wellbores in Weiyuan area are along the minimum horizontal stress direction in general (α is approximately equal to 90°). The corresponding θ of high shear stress area (τc≥1 GPa) in this case is 20°-55° (or its supplementary angle) when α=90°, which is consistent with the NF approach angle at CD position in Table 2. Thus, the value of α can be appropriately adjusted according to the chart to avoid the impact of high shear stress on wellbore at a given θ.

Fig. 4.

Fig. 4.   Effect of fracture approach angle on wellbore shear stress under different wellbore approach angles.


Besides, the integrity of the cementing sheath has a significant impact on the wellbore shear stress. In this case, the maximum shear stress on wellbore (α=135°, θ=45°) with damaged cementing sheath is 5.97 times that with intact cementing sheath. Fig. 4a shows that the value of τc is much higher than the shear strength (Ss) of the cementing sheath. Thus, it can be inferred that the cementing sheath integrity will be difficult to maintain when the formation slips along the fracture surface, so the focus of the next analysis is the CD in the case with damaged cementing sheath. Moreover, high steel-grade and thick casing is used in this case, the τc value in the case of damaged cement sheath is compared with the casing shear strength (Sc). It is found that the τc value is much higher than the casing shear strength (Fig. 4b), which shows that enhancing casing strength or cementing quality has limited effect on reducing the risk of CD[22].

1.2.2. Fracture area

Fig. 5 shows the relationship curves between fracture area (Af) and τc under α in different values of a fully opened fracture with θ=30°. In the figure, the larger the Af, the larger the τc is; and the value of τc first increases and then decreases with the increase of α. From Eq. (6), at given τxy and Ac, τc is mainly affected by Af, namely, the larger the NF area, the higher the risk of CD.

Fig. 5.

Fig. 5.   Influence of NF area on wellbore shear stress.


1.2.3. Fluid pressure in fractures

Fracture fluid pressure will affect natural fracture slippage when the fracture is partially opened. Fig. 6 shows the relationship curves between θ and τc under different pf conditions when α=90°, μ=0.6, and Af=50 m2. When the pf value is higher than σx, τc reaches the maximum, and when pf is lower than σx-μ-1τxy, τc becomes zero at any θ conditions. Taking the case of θ=30° as an example, σx is calculated to be 67.5 MPa and σx-μ-1τxy is 60.3 MPa. In the figure, τc increases with the increase of pf, the τc curves at pf of 70, 75, and 80 MPa overlap at the position of θ=30°, and τc reaches the maximum value when the pf value is higher than 67.5 MPa. In contrast, when the pf value is lower than 60.3 MPa, τc is zero.

Fig. 6.

Fig. 6.   Influence of fracture fluid pressure on wellbore shear stress.


1.2.4. Fracture friction coefficient

Fig. 7 shows the relationship between θ and τc under different fracture friction coefficient (μ) conditions of a partially opened fracture when α=90°, pf=65 MPa, and Af=50 m2. It can be seen at given ground stress and fracture geometric parameters, fmax increases with the increase of μ, resulting in decrease of τc. However, because of the limited range of μ, the influence of the variation of μ on wellbore shear stress is not as significant as that of pf.

Fig. 7.

Fig. 7.   Influence of fracture friction coefficient on wellbore shear stress.


Based on the above analysis, it is believed that NF is the main factor inducing CD in horizontal wells. Therefore, strengthening the monitoring and identifica-tion of NF in the block will help prevent CD in engineering: (1) Placing the wellbore parallel or perpendicular to the trend of natural fractures and avoid large NFs can reduce the wellbore shear force and lower the risk of CD based on a deep understanding of the geological conditions of the block; (2) Reducing net pressure in the fracture through engineering measures is an effective method to reduce the risk of CD[9].

“Multi-cluster perforation+temporary plugging and diverting” technology applied in the horizontal well fracturing in Weiyuan area has achieved good results in reducing the risk of CD. The proportion of CD wells treated by this technology is 21%, which is far less than that of wells treated by the coventional technology of 48%. In blocks with known geological engineering parameters, the method proposed in this paper can be used to establish a chart and quickly estimate the risk of CD. Fluid pressure in the fracture can be reasonably controlled through engineering measures, such as optimizing the wellbore azimuth, controlling pumping rate, and applying temporary plugging, to reduce the risk of CD.

2. Calculation of CD induced by fracture slippage

2.1. Casing deformation calculation model

The rapid determination of CD is of great significance to the engineering design of CD well. Since the fracture slip shear stress is much greater than wellbore shear strength, it can be assumed that the CD is approximately equal to the fracture slippage in the tangential direction. Meanwhile, assuming that: (1) NF is the “I+II” composite type fracture[23] (the opened fracture with tensile stress is defined as type I, and the slip fracture with shear stress is defined as type II), as shown in Fig. 8, and the fluid pressure in the fracture is pf; (2) the fracture is fully opened under pf, fluid pressure is equal everywhere inside the fracture, and fluid leak-off and fracture propagation are ignored. Based on the above assumptions, a CD calculation model is established based on the complex function method.

Fig. 8.

Fig. 8.   Plane strain model of “I+II” type fracture.


The Westergaard stress function of “I+II” type fracture can be expressed as[23]:

$\left\{ \begin{align} & Z\left( z \right)=\sqrt{\frac{{{d}^{2}}}{{{d}_{1}}{{d}_{2}}}}\left( {{\sigma }_{\text{b}}}\cos \ \psi +\tau \sin \ \psi \right)+\frac{{{\sigma }_{\text{a}}}-{{\sigma }_{\text{b}}}}{2}+ \\ & \ \ \ \ \ \ \ \ \ i\sqrt{\frac{{{d}^{2}}}{{{d}_{1}}{{d}_{2}}}}\left( {{\sigma }_{\text{b}}}\sin \ \psi -\tau \cos \ \psi \right) \\ & \psi =\beta -\frac{{{\beta }_{1}}+{{\beta }_{2}}}{2} \\ \end{align} \right.$

Based on the Muskhelishvili fracture displacement calculation method[23], the displacement field of the “I+II” type fracture can be calculated by Eq. (10):

$\left\{ \begin{align} & u=\frac{1}{{{E}'}}\left\{ 2\operatorname{Re}\widetilde{Z}\left( z \right)-\left( 1+{\upsilon }' \right)\left[ \frac{1}{2}\operatorname{Re}\bar{z}Z\left( z \right)-\begin{matrix} {} \\ {} \\\end{matrix} \right. \right. \\ & \ \ \ \left. \left. \begin{matrix} {} \\ {} \\\end{matrix}\frac{1}{2}\operatorname{Re}zZ\left( z \right)+\operatorname{Re}\widetilde{{{Z}_{\text{I}}}}\left( z \right) \right] \right\} \\ & v=\frac{1}{{{E}'}}\left\{ 2\operatorname{Im}\widetilde{Z}\left( z \right)-\left( 1+{\upsilon }' \right)\left[ \operatorname{Im}\widetilde{Z}\left( z \right)-\begin{matrix} {} \\ {} \\\end{matrix} \right. \right. \\ & \ \ \ \left. \left. \begin{matrix} {} \\ {} \\\end{matrix}\frac{1}{2}\operatorname{Im}\bar{z}Z\left( z \right)-\frac{1}{2}\operatorname{Im}zZ\left( z \right)-\operatorname{Im}\widetilde{{{Z}_{\text{I}}}}\left( z \right) \right] \right\} \\ \end{align} \right.$

The fracture relative displacement can be derived from Eq. (9) and Eq. (10):

$\left\{ \begin{align} & \Delta u=4\left( 1-{{\upsilon }^{2}} \right)\frac{\tau }{E}a\sqrt{1-{{\left( \frac{{{k}'}}{a} \right)}^{2}}} \\ & \Delta v=4\left( 1-{{\upsilon }^{2}} \right)\frac{{{\sigma }_{\text{b}}}}{E}a\sqrt{1-{{\left( \frac{{{k}'}}{a} \right)}^{2}}} \\ \end{align} \right.$

And the fracture relative displacement under the additional fluid pressure in fracture can be derived as:

$\left\{ \begin{align} & \Delta {{u}_{\text{p}}}=0 \\ & \Delta {{v}_{\text{p}}}=4\left( 1-{{\upsilon }^{2}} \right)\frac{{{p}_{\text{f}}}}{E}a\sqrt{1-{{\left( \frac{{{k}'}}{a} \right)}^{2}}} \\ \end{align} \right.$

Thus, the fracture relative displacement of “I+II” type fracture can be derived from Eq. (11) and (12) as:

$\left\{ \begin{align} & \Delta {{u}_{\text{f}}}=4\left( 1-{{\upsilon }^{2}} \right)\frac{\tau a}{E}\sqrt{1-{{\left( \frac{{{k}'}}{a} \right)}^{2}}} \\ & \Delta {{v}_{\text{f}}}=4\left( 1-{{\upsilon }^{2}} \right)a\frac{{{\sigma }_{\text{b}}}-{{p}_{\text{f}}}}{E}\sqrt{1-{{\left( \frac{{{k}'}}{a} \right)}^{2}}} \\ \end{align} \right.$

2.2. Model validation

During the perforation operation of Well HX-1 in Wei 202 block, the bridge plug was obstructed when pumped to 3090 m downhole. The result of ant-body interpretation showed that a NF (150 m long, 50° N by E in azimuth) across the wellbore at the sticking point, the wellbore was about 30 m away from the fracture midpoint. Well temperature logging data showed that the temperature at the sticking point dropped greatly, and caliper logging data showed that grade-3 CD occurred at the sticking point (Tables 3 and 4). As shown in Fig. 9, the calculated CD (Δuf, relative displacement in tangential direction of “I+II” type fracture) of Well HX-1 is 33.5 mm based on the above data. And the caliper logging data showed that the maximum CD of this well is 31.8 mm. The relative error of calculated CD is 5.3%, indicating that the calculation model is applicable.

Table 3   Geological engineering parameters of Well HX-1.

ParameterValueParameterValue
NF length150 mPoisson’s ratio0.22
Wellbore diameter215.9 mmElasticity modulus43.5 GPa
Casing diameter139.7 mmσH60 MPa
Casing thickness12.7 mmσh72 MPa

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Table 4   CD detection logging parameters of Well HX-1.

ParameterValueParameterValue
Deformation length10 mMaximum CD31.8 mm
Average inner diameter112.7 mmCD grade3
Maximum inner diameter141.4 mm

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Fig. 9.

Fig. 9.   Calculated CD of Well HX-1.


2.3. Analysis of factors affecting CD

2.3.1. Rock mechanical parameters

Fig. 10 shows the relationship curves of k'/a and Δuf under different elasticity moduli at θ=45°, υ=0.25, and a=50 m. The figure shows the calculated CD varies in parabolic shape, and the maximum CD occurs at the fracture midpoint; under the same stress, the higher the elasticity modulus, the smaller the rock strain, so the larger the elasticity modulus, the smaller the CD will be.

Fig. 10.

Fig. 10.   Influence of rock elasticity modulus on CD.


With θ and a fixed, the influence of rock Poisson’s ratio on CD at E=30 GPa is shown in Fig. 11. The figure shows the CD is negatively correlated with Poisson’s ratio, but Poisson’s ratio has a limited effect on CD.

Fig. 11.

Fig. 11.   Influence of rock Poisson’s ratio on CD.


2.3.2. Fracture geometric parameters

Fig. 12 shows the influence of fracture half-length on CD at θ and υ with fixed values, and E of 30 GPa. The figure shows fracture half-length has a great impact on CD. This is because the larger the a, the larger the fracture area, the greater the shear force on formation, and the greater the formation displacement will be, resulting in larger CD.

Fig. 12.

Fig. 12.   Influence of fracture half-length on CD.


With υ and a fixed, the influence of fracture approach angle on CD at E of 30 GPa is shown in Fig. 13. Since the shear stress is a sine function of θ, only the variation of the CD at θ∈[0°, 90°] is discussed. The calculation results show that the CD first increases and then decreases with the increase of θ, and the maximum value appears at θ of 45°.

Fig. 13.

Fig. 13.   Influence of fracture approach angle on CD.


3. Conclusions

The fracture and wellbore approach angles have significant impacts on the wellbore shear stress. Under the condition of common wellbore approach angles in the Weiyuan shale gas field, under fracture approach angles of 20° to 55° (or supplementary angles), the wellbore is subjected to large shear stress and high risk of CD.

When the fracture is partially opened by fracturing fluid, the wellbore shear stress is positively correlated with the fluid pressure in fracture, and negatively correlated with the fracture friction coefficient. When the fracture is fully opened, the wellbore shear stress is positively correlated with the natural fracture area.

The lower the rock elasticity modulus and the longer the fracture length, the more serious the CD will be. Poisson's ratio has a weak influence on the CD. The CD first increases and then decreases with the increase of the fracture approach angle, and reaches the maximum at the fracture approach angle of 45°.

For a given fracture approach angle, appropriately adjust the wellbore approach angle can avoid high shear stress on the wellbore. Reasonable control of the fluid pressure in fracture can reduce the CD risk. The shear stress on casing is usually much greater than casing shear strength, increasing casing strength or cementing quality has limited effect on reducing the risk of CD.

Caliper logging data has verified the CD prediction model, and the model can be used to establish risk analysis charts and calculate CD, which provides reference for quick CD risk prediction in fracturing design.

Nomenclature

a—NF half length, m;

a', b', c', d'—the 4 sides of the stress unit;

Ac,${{{A}'}_{\text{c}}}$—the area enclosed by the cementing sheath and casing on the section of wellbore and fracture, m2;

Af—NF area, m2;

d, d1, d2—the distance from z point to the midpoint and two endpoints of the long axis of the fracture in “I+II” type fracture plain stress model, m;

E—rock elasticity modulus, MPa;

E'—rock elasticity modulus under the plain strain condition, MPa;

f—actual friction force on fracture surface, 106 N;

fmax—the maximum static friction force on fracture surface, 106 N;

h—NF half height, m;

Im—imaginary part of complex function;

k—any point on the X axis;

k°—X coordinate value of k point, m;

pf—fluid pressure in fracture, MPa;

r1, r2—inner diameter and outer diameter of casing, m;

R—wellbore diameter, m;

Re—real part of complex function;

Sc—casing shear strength, MPa;

Ss—cementing sheath shear strength, MPa;

u, v—tangential and normal displacement of “I+II” type fracture, m;

x, y—the direction perpendicular and parallel to the fracture surface;

X—1D coordinate axis along the major axis of “I+II” type fracture;

z—the complex variable at any point in the “I+II” type fracture plain strain model;

$\bar{z}$—conjugate complex number of complex variable z;

Z(z),${{Z}_{\text{I}}}\left( z \right)$—Westergaard stress function of “I+II” type fracture and I type fracture;

$\widetilde{Z}\left( z \right)$,$\widetilde{{{Z}_{\text{I}}}}\left( z \right)$—integral of$Z\left( z \right)$, ${{Z}_{\text{I}}}\left( z \right)$ with respect to z;

α— wellbore approach angle, (°);

β, β1, β2—the angles between the line from z point to the midpoint and two endpoints of the long axis of the fracture with fracture long axis, (°);

Δu, Δv—relative displacement in tangential and normal directions of “I+II” type fracture, m;

Δup, Δvp—relative displacement in tangential and normal directions of fracture with the influence of fluid pressure, m;

Δuf, Δvf—relative displacement in tangential and normal directions of “I+II” type fracture with influence of fluid pressure, m;

θ—NF approach angle, (°);

μ—fracture friction coefficient, dimensionless;

σa, σb—normal stress components of ground stress on the long and short axis of “I+II” type fracture, MPa;

σH, σh—the maximum and minimum horizontal principal stress, MPa;

σn—contact normal stress of matrix on fracture surface, MPa;

σv—vertical stress, MPa;

σx, σy—the normal stress component of ground stress in the x and y direction of the stress unit, MPa;

τ—the shear stress component of ground stress of the stress unit, MPa;

τc—wellbore shear stress, MPa;

τyx, τxy—the shear stress component of ground stress in the x and y direction of the stress unit, MPa;

υ—rock Poisson’s ratio, dimensionless;

υ°—rock Poisson’s ratio under plain strain condition, dimensionless;

Ψ—intermediate variables, (°).

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