Dynamic response and limit analysis of buried gas pipeline under ground consolidation load
Taolong Xu^{1} , Jian Mao^{2} , Yanhua Liu^{3} , Anlin Yao^{4}
^{1, 4}College of Petroleum Engineering, Southwest Petroleum University, Chengdu, 610500, China
^{2, 3}WestEast Gas Pipeline Branch Company, PetroChina Pipeline Company Limited, Shanghai, 200122, China
^{1}Corresponding author
Journal of Vibroengineering, Vol. 19, Issue 7, 2017, p. 49895008.
https://doi.org/10.21595/jve.2017.18405
Received 29 March 2017; received in revised form 18 June 2017; accepted 18 July 2017; published 15 November 2017
JVE Conferences
Currently, the significant dynamic plastic deformation of a buried gas pipeline frequently occurs due to the ground construction process that acts as a direct threat to the operation security of a buried gas transmission system. In this study, the pipesoil interaction structure under a dynamic consolidation load, such as high energy dynamic compaction load, was considered as a nonconservative system in the work. Two parts of structure dissipation energy were introduced into the Lagrange function, and the elastoplastic dynamic equations of a nonconservative system based on the Hamilton Variation Principle (HVP) and the finite element (FE) theory were established. Implicit solution schemes were proposed based on the dynamic equations, and a steel weightsoilburied pipeline finite element model was developed by performing a dynamic analysis in the LSDYNA software with an explicit format. Vivid impact responses of an underground pipeline associated with the buried depth, wall thickness, and tamping energy were simulated. The plastic failure criterion of high toughness pipeline steel indicates that treated pipeline buried depth, wall thickness, and tamping energy corresponded to the generalized loads, and limit state of a specific case. So, they were recognized via the relationship of generalized load in relation to the total strain of pipelines. This was performed by using tangent intersection criteria, two elastic slope criteria, and zero curvature criteria. Additionally, the von Mises yield stress criterion was also applied as a traditional approach. The study potentially offers significant references on the quantitative preevaluation of a buried gas pipeline that poses as a threat due to the occurrence of thirdparty damage such as extreme strong ground interference.
Keywords: dynamic consolidation loading, buried gas pipeline, Hamilton variation principle, dynamic response, limit analysis.
1. Introduction
Recently, ground construction activities including drilling exploration, foundation construction, and underground facilities installation are increasingly more frequent, and this leads to a threat with respect to the “area of opportunity” [1] where a buried pipeline is threatened by the expansion of thirdparty damage. Pipeline accident statistics from the U. S. Department of Transportation (DOT) indicate that approximately 2040 % of pipeline failures are caused by thirdparty damages. In Europe, the thirdparty damage accounts for approximately 50 % of all gas pipeline failure [2]. In China, with the trunk line in the Sichuan province as an example, approximately 14.2 % of the damages were caused by thirdparty interferences from 1969 to 1990, and this rate increased to 52.9 % after 2000. The statistical data shows that the third party damage accident ratio continuously increases, and thus the quantitative analysis of thirdparty interference is a key and difficult part of pipeline risk evaluation [3].
The dynamic consolidation (or dynamic compact) method was first used by Menard L. in 1969 for the treatment of abandoned stone foundation in the area of Napoule near Cannes. As shown in Fig. 1, dynamic consolidation is a complex nonlinear dynamic ground construction which makes a huge impact load by using the falling steel weight within very short time. Thus, it is considered as one of the main thirdparty threats of buried gas pipelines where it is possible to detect obvious dynamic characteristics. Many extant studies involving numerical analyses and experimental studies were performed on the problem of dynamic compaction kinetics. Theoretical studies examining boundary contact stress of dynamic compaction were performed by Kong et al. [4] and Tong et al. [5]. A dynamic contact finite element method was applied by Jiang et al. [6] to analyze the impact of dynamic compaction on foundation soil. Additionally, explicit transient nonlinear finite element analysis technology and a large deformation problem analysis method were employed in a study by Shui et al. [7]^{}to examine impact response during a dynamic compaction operation on the foundation soil. Furthermore, numerical modeling methods were developed by Song et al. [8], Li et al. [9] and Y. K. Chow et al. [10] to investigate the characteristics of dynamic compaction. Several insitu tests were made by Brandl et al. [11] and He et al. [12] to examine the subgrade compaction as well as the dynamic stress distribution of a hammer influence area.
Fig. 1. Impact of dynamic consolidation operation on buried gas pipeline
General phenomena and basic laws of rammer and soil during the dynamic compaction process were analyzed in most of existing studies but seldom researchers analyzed a force on the damage response of underground facilities such as a buried steel gas pipeline. In the present study, dissipated energy was introduced into a Lagrange function for a nonconservative system. The finite element scheme for the governing equations of the elastic plastic body with energy dissipation was derived based on the Hamilton Variation Principle (HVP). During this process, the dynamic control equation of an element (including kinetic energy, strain energy, damping dissipation work, and external force potential energy) was transformed into a dynamic control equation of an element (including a stiffness matrix, mass matrix, damping matrix, and load matrix). Based on the explicit scheme, the rammersoilburied pipeline interaction model under dynamic contact conditions was constructed by using the finite element method. It was assumed that the rammer corresponded to the rigid body. The DruckerPrager constitutive model was selected as the elasticplastic state of soil under the shock load and X70 buried steel pipe with strain rate effects which were reflected by the CowperSymonds model. In the semiinfinite soil medium, reasonable dynamic parameters and a contact algorithm were set to analyze the extreme stress, strain, and vibration velocity of a pipe with respect to three variables including buried depth, pipe wall thickness, and compact energy. Finally, the critical status was calculated by four limit analysis methods, namely the tangent intersection criterion, double elastic slope criterion, zero curvature criterion, and stress intensity criterion.
2. Elastoplastic dynamic governing equations
2.1. Implicit derivation based on HVP
Undoubtedly, it is necessary to consider the damping dissipation of a structure in practical dynamic impact processes such as the dynamic compaction. In the present study, the dissipation energy was introduced into the Lagrange function, and the dynamic governing equations for finite element scheme of elastoplastic body that account for the energy dissipation were derived based on the HVP. First, a unit body with kinetic energy $T$, strain energy $U$, and external force potential energy ${W}_{e}$ is considered. With respect to the conservative system, the Lagrange function is expressed as follows [13]:
The plastic dissipation function ${W}_{d}$ is embedded into the nonconservative system of the elastoplastic medium, and thus Eq. (1) is written as follows:
Thus, the elastoplastic dynamic governing equations are described as shown in Eq. (3), and the details of the derivation process based on HVP are given in the Appendix:
where ${K}^{e}$, ${M}^{e}$, ${C}^{e}$, ${F}_{ext}$ and ${F}_{p}$ represent stiffness matrix, mass matrix, damping matrix, external load matrix, and generalized load matrix produced by plastic deformation of the unit body. Eq. (3) is reexpressed in an incremental form as shown in Eq. (4):
where, $\mathrm{\Delta}{F}_{ext}$ and $\mathrm{\Delta}{F}_{p}$ represent the matrix incremental of external load and the generalized load matrix incremental produced by plastic deformation, respectively, and $\mathrm{\Delta}{F}_{p}=\underset{v}{\iiint}{B}^{T}D\mathrm{\Delta}{\epsilon}_{p}dV$ and $\mathrm{\Delta}{F}_{ext}=\underset{v}{\iiint}{N}^{T}\mathrm{\Delta}fdV+\underset{S}{\iint}{N}^{T}\mathrm{\Delta}\stackrel{}{t}dS$. The details of each symbol are given in Appendix.
The finite element program of dynamic compaction involves solving a dynamic equation by using the stepbystep time integration. It is necessary to select an appropriate loading time step to control the solution stability. If the selected load time step $\mathrm{\Delta}t$ is too low, then it increases the calculation time. And conversely, the calculation accuracy is affected if the selected time step $\mathrm{\Delta}t$ is too high. With respect to the compaction and other dynamic impact load, the time step is determined by the following expression [14]:
where $\mathrm{\Delta}l$ denotes characteristic size of the smallest element in the structure; and $c$ denotes the longitudinal wave velocity.
The method is used in conjunction with the Newmark method and the plastic iterative method for the solution of the incremental form of a control equation in each time step. The solution process is shown in Fig. 2.
2.2. Damping definition in explicit finite element code
The explicit analysis of dynamic finite element program is based on a dynamic control equation [15]. In the ANSYS/LSDYNA finite element software, a Hamilton control equation is achieved through the damping settings as shown in Fig. 3. The commands including EDDAMP, PART, LCID, and VALDMP can be selected in Damping Options. The element group number for the damping load is defined via PART. The Load curve ID (LCID) identifies the damping coefficient versus time curve, and an LCID is required if timedependent damping is defined. Additionally, VALDMP is used to specify the mass damping with respect to time, and VALDMP is a constant system damping coefficient or a scale factor applied to the curve to define the damping coefficient relative to time. Thus, the massweighted (Alpha) or stiffnessweighted (Beta) damping is defined by using the EDDAMP command [16].
Fig. 2. Flow chart for solving governing equations of elastoplastic dynamic process
Fig. 3. Damping option box in ANSYS
In addition to the Damping Option command, the massweighted (Alpha) or stiffnessweighted (Beta) damping is expressed in the LSDYNA input file as *DAMPING_GLOBAL, *DAMPING_PART_MASS, and *DAMPING_PART_STIFFNESS.
3. Finite element modeling
3.1. Material parameters
Currently, pipelines with extreme strength and ductility that are composed of X70 and X80 grade steels are widely used in a longdistance natural gas transmission system. A kinematic hardening bilinear model that obeys the von Mises yield criterion can easily identify the strength and deformation of a steel pipeline under dynamic impact conditions as follows:
where ${S}_{ij}$ denotes the partial stress tensor; ${\alpha}_{ij}$ denotes the back stress tensor; and ${\sigma}_{y}$ denotes the yield stress.
The strain rate effect should not be ignored due to the high speed impact of dynamic consolidation. In this study, the strain rate is considered during the usage of the CowperSymonds (CS) [17] model that scales the yield stress rate dependent factor as shown below:
where ${\sigma}_{0}$ denotes the static yield strength or initial yield stress, $C$ and $P$ denote the CS strain rate parameters, ${\dot{\epsilon}}_{eff}$ denotes the equivalent strain rate, ${\dot{\epsilon}}_{eff}=\sqrt{\left(2/3\right){\dot{\epsilon}}_{ij}{\dot{\epsilon}}_{ij}}$, $\beta $ denotes the hardening parameter between 0 (kinematic hardening only) and 1 (isotropic hardening only), ${\epsilon}_{p}^{eff}$ denotes the effective plastic strain, and ${E}_{p}$ denotes the plastic hardening modulus that is given by ${E}_{p}=\frac{{E}_{\mathrm{t}\mathrm{a}\mathrm{n}}E}{E{E}_{\mathrm{t}\mathrm{a}\mathrm{n}}}$, and ${E}_{tan}$ and $E$ denote the tangent modulus and elastic modulus, respectively. If only kinematic hardening is involved, then Eq. (7) is expressed as Eq. (8) as follows:
The material parameters of CS model can be determined based on the related test results of high strength steel [18] as listed in Table 1 (keyword *MAT_PLASTIC_KINEMATIC in LSDYNA).
Table 1. Material parameters of pipeline steel
Density (kg/m^{3})

Elastic modulus (GPa)

Poisson’s ratio

Tangent modulus (GPa)

Yield stress (MPa)

CS strain rate parameter


C/s^{1}

$P$


7900

210

0.3

13.5

540

5946

1.75

The DruckerPrager (DP) model was selected as the constitutive law of soil (keyword *MAT_DRUCKER_PRAGER in LSDYNA). The DP model is a reasonable law to model the elasticplastic state of soil under an impact load during which the instability in the large deformation calculation is available [19]. The expression of DP model is given below:
where ${J}_{2}={s}_{ij}{s}_{ij}/2$, and ${s}_{ij}$ denote the second invariant of stress deviation, ${I}_{1}={\sigma}_{kk}/3$, and ${\sigma}_{kk}$ denotes the first invariant of stress tensor, $\alpha $ and $k$ denote the constants determined by cohesion value c and angle of friction $\varphi $ as follows:
Table 2. Soil material parameters
Soil type

Density
(kg/m^{3})

Elastic shear
modulus (MPa)

Poisson’s ratio

Cohesion
value (kPa)

Angle of
friction (rad)

Clay

1500

5.38

0.3

42

0.471

Sand

1840

20

0.25

5

0.611

Collapsible loess

1380

7.25

0.38

14.9

0.414

Gravel

2200

25

0.2

55

0.698

Four different soil types were applied to analyze the buffering effect under different soil properties (as listed in Table 2), which are especially necessary for a longdistance pipeline. Specifically, when the rammer collided with the soil by surfacetosurface contact, the free surface vibration caused soil and buried pipeline turbulence. In order to save computing time, the steel weight was approximately regarded as a rigid body with a density of 7640 kg/m^{3}.
3.2. Model design
It is assumed that the soil is an elasticplastic material that is composed of horizontal layers, and each layer is homogeneous and isotropic. Thus, the process of dynamic consolidation can be simplified as a semiinfinite system that is impacted by a rammer with the short cylinder shape [19]. In this study, the diameter ${D}_{s}$ of rammer corresponds to 2 m, and the steel weight impacts immediately the soil above the pipeline (with an outer diameter ${D}_{p}$, thickness $T$, and buried depth $h$). Fig. 4 schematically describes the relative position and size of each part. The surfacetosurface contact mode with a pure penalty method was selected as the contact schemes between hammer, soil, and buried pipeline. An artificial boundary referred to as the nonreflective boundary condition was applied to the pipeline perimeter boundaries and the bottom boundary, which corresponded to the semiinfinite earth in reality. A solid164 hexahedral element was selected in the explicit FEA model, which included the steel rammer, soil, and buried pipelines. As shown in Fig. 5, a half model was developed due to the symmetry of the model. This was performed by using the Lagrange element where a total of 15,379 nodes and 12,792 elements were divided.
Fig. 4. Geometric model
Fig. 5. Finite element model
Fig. 6. Interface of objectoriented program
In order to enhance the simulation efficiency, an objectoriented program was designed as shown in Fig. 6, and it includes the material parameters of the soil and pipeline steel as well as the working conditions of pipeline and consolidation behavior. The function of the FEA model and its calculation and postprocess in the interface triggered the corresponding software. Thus, the material parameters and working conditions could be modified conveniently.
3.3. Calculation results and discussion
3.3.1. Soil buffer mechanism
As mentioned above, in order to obtain the solution of the dynamic problem, it is necessary to gradually integrate the dynamic governing Eq. (4). Specifically, the LSDYNA uses the explicit central difference method for time integration. The buffer mechanism of the soil above the pipe is expressed by a damping part in the dynamic governing equation, and the soil damping is divided into two terms as follows:
where $a$ and $b$ denote the constants with values that are associated with the lumped mass matrix ${M}^{e}$ and global stiffness matrix ${K}^{e}$, and $a=$ 0.7 and $b=$ 0.002.
Four soil models (Table 2) were employed in the present study to identify the damping effect relative to the steel weight. Fig. 7 visually depicts the depression of the collapsible loess surface under impact during which the tamping energy corresponds to 1000 kJ. It ensures that other conditions remain unchanged as follows: ${D}_{p}=$ 1016 mm, $h=$ 1 m, $T=$ 21 mm, $P=$ 10 MPa, and ${D}_{s}=$ 2 m. Fig. 8 shows the duration traces of the vertical displacement of steel weight penetrated into the soil, and it was possible to obtain a clear intuitive judgment of the strength of each soil. The most significant compaction depth that corresponded to 0.246 m appeared on the collapsible loess. The clay and gravel mediums were characterized by the obvious rebound phenomenon that was distinguished from those of the other types. Thus, a visual impression was obtained where the gravel corresponded to the most rigid medium. But it had significant flexibility that directly affected the response intensity of the buried pipeline due to the buffer mechanism. Fig. 9 shows a comparison of the von Mises stress of the pipetop element 12165 and the maximum resultant node velocity of pipeline. The gravel medium with the highest density and elastic shear modulus always created the highest interference on pipeline. In contrast, the clay played a much better cushion role as well as a vibration mitigation effect with respect to an underground structure than with respect to the other mediums. Additionally, it is observed that clay is widely found in developed areas with active ground construction. Thus, clay is considered as the covering layer, and the dynamic response and limitation analyses of the buried gas pipeline under multiple working conditions are performed in the following sections.
Fig. 7. $Y$displacement contours of collapsible loess under consolidation load
Fig. 8. $Y$displacement of four different soil types under a consolidation load
Fig. 9. Comparison of dynamic responses of a pipetop
3.3.2. Distance attenuation analysis
With respect to the ground dynamic compaction, the soil buffer mechanism is always closely related to the energy attenuation due to the increase in a construction distance, and this is illustrated by the interference of pipeline under different impacting distances. This includes both vertical and horizontal orientations. The former case is discussed here while the latter is calculated in section 3.3.3.
Fig. 10 shows the von Mises stress reduction of pipetop element 12165 by using a timehistory curve. There a significant decrease occurred when the distance exceeded 3 m. Since then the inner pressure was a major contributor of the equivalent stress of the pipeline, and its value approximately corresponded to 214 MPa. The maximum value of pipeline approximately corresponded to 216 MPa. Clearer distancedependences regularities are observed in Fig. 11 in which maximum equivalent stresses of pipeline under five distances are calculated and indicated by open red circles, and the maximum resultant node velocities are denoted with solid blue circles. As observed in the figure, there is a high reduction in the slope between 1 m and 3 m in both responses, and they are fitted by the solid lines. The tendencies of the distance attenuation law for pipeline’s dynamic response are accurately described by the Gauss function as given below:
where $f\left(d\right)$ denotes the modeling result including maximum von Mises stress and maximum resultant node velocity as shown in Fig. 11; ${f}_{min}$ denotes estimated minimum values; $d$ denotes distance from the pipeline to the loading position in this study; and $A$, $w$, and ${d}_{c}$ correspond to constants determined by different conditions. Thus, the fit curve for stress and velocity is analyzed by Origin 8.0, and the Gauss functions are described as follows:
With respect to the maximum von Mises stress $\sigma \left(d\right)$:
With respect to the maximum resultant node velocity $v\left(d\right)$:
In order to verify the applicability of Eqs. (13) and (14), the simulation of a 2 m distance was performed. The stress and velocity results corresponded to 233.51 MPa and 1.0081 m/s, respectively, by modeling, and the stress and velocity results corresponded to 233.01 MPa and 1.41 m/s, respectively, when Eq. (13) and Eq. (14) were used. As shown in Fig. 11, the fit curves with a Gauss function indicate good prediction ability for a relative dynamic response. Thus, the predictive trending by Gauss functions is extremely similar to the timehistory character as shown in Fig. 10.
Fig. 10. Distance attenuation with respect to equivalent stress of a pipetop element
Fig. 11. Distance attenuation law of dynamic response of buried pipeline (positive and negative distances indicate two opposite directions from the impacting point)
3.3.3. Multicondition analysis
The security of a longdistance buried gas pipeline under dynamic compaction is always influenced by multiple variables, such as buried depth, wall thickness inner pressure, soil type, and tamping energy, which should be considered as the main risk factors of thirdparty damage. Although the inner pressure and soil type factors were discussed above, it is necessary to further clarify the relevance of other factors. Three conditions (A, B and C) containing a total of 21 cases (listed in Table 3) were investigated by using an explicit code in the following sections. It was assumed that the pipeline was always in the worst status, and this indicated that an additional protective structure was not present above the pipeline. The impact distance was assumed as 0 m, and it was assumed that the pipeline directly contacted the clay in all cases.
In condition A, the dynamic responses of the gas pipeline were analyzed under the following different buried depths: 0.5 m, 0.8 m, 1.0 m, 1.5 m, 2.0 m, 2.5 m, and 3.0 m. The following parameters were used in each case: pipeline diameter ${D}_{p}=$ 1016 mm, wall thickness $T=$ 21 mm, inner pressure $P=$ 10 MPa, tamping energy $E=$ 2500 kJ. The effective stress was considered as an example, and Fig. 12 shows the maximum effective stresstime response of the pipeline under different buried depths. Qualitatively, an obvious stress attenuation phenomenon was obtained with an increase in the buried depth $h$ (horizontal impact distance), and the time consumption of the stress curve peak also increased. It should be noted that significant fluctuations existed with respect to both stress and time when $h>$1 m. The quantitative assessment in Fig. 13 indicated that the maximum stress decreased from 517.33 MPa to 416.12 MPa when the buried depth increased from 1.0 m to 1.5 m. This indicated that the sensitivity of the horizontal impact distance as well as the loading propagation duration existed when the pipeline was buried at a depth exceeding 1.0 m. Thus, the appropriate increase in the overlying soil can effectively protect the pipeline, especially the pipeline laid through high consequence areas.
Slopeillustrated embedded fit curves demonstrated in Fig. 13 can articulate the feature descriptions mentioned above. A doseresponse curve with a variable Hill slope was used to identify the tendency of maximum von Mises stress $\sigma \left(h\right)$ under different buried depths $h$ as follows:
With respect to the loading propagation time $t\left(h\right)$, the Allometric power function was applied to describe the influence of the buried depth $h$ of the pipeline as follows:
Table 3. Multiconditions in simulation (X70 pipeline, ${D}_{p}=$ 1016 mm)
Condition

Case

Inner pressure $P$ (MPa)

Depth $h$ (m)

Wall thickness $T$ (mm)

Tamping energy $E$ (kJ)

A

1

10

0.5

21.0

2500

2

10

0.8

21.0

2500


3

10

1.0

21.0

2500


4

10

1.5

21.0

2500


5

10

2.0

21.0

2500


6

10

2.5

21.0

2500


7

10

3.0

21.0

2500


B

1

10

1.0

14.6

2500

2

10

1.0

17.5

2500


3

10

1.0

21.0

2500


4

10

1.0

26.2

2500


5

10

1.0

28.0

2500


C

1

10

1.0

21.0

1000

2

10

1.0

21.0

1500


3

10

1.0

21.0

2000


4

10

1.0

21.0

2500


5

10

1.0

21.0

3000


6

10

1.0

21.0

3500


7

10

1.0

21.0

4000


8

10

1.0

21.0

4500


9

10

1.0

21.0

5000

Fig. 12. Timehistory of effective stress maxima with respect to different buried depths
Fig. 13. Stress magnitude and loading propagation characters with respect to different buried depths
The thicknessstress response was simulated in condition B where the following other parameters were considered as constant: pipeline diameter ${D}_{p}=$ 1016 mm, inner pressure $P=$ 10 MPa, buried depth $h=$ 1.0 m, and tamping energy $E=$ 2500 kJ. Fig. 14 shows the effective stress maxima under the following five different wall thicknesses: 14.6 mm, 17.5 mm, 21.0 mm, 26.2 mm, and 28.0 mm. The maximum von Mises stress increased with decreases in the wall thickness. Higher residual stress fluctuations due to inner pressure were observed in these cases as compared with those in the other conditions. An increase in the wall thickness increased the reliability of the state for the pipeline operation.
Fig. 14. Timehistory of effective stress maxima under different wall thickness
However, the extreme stress response was less insensitive to the wall thickness than expected. Thus, it is necessary to appropriately increase the wall thickness to a certain level that can enhance the ability to resist external interference in addition to considering a reasonable relationship between construction cost and system integrity with respect to a failure analysis.
In condition C, eight tamping energy levels (1500 kJ, 2000 kJ, 2500 kJ, 3000 kJ, 3500 kJ, 4000 kJ, 4500 kJ, and 5000 kJ) were imposed by the steel weight to explore the response of the pipeline with ${D}_{p}=$ 1016 mm, $T=$ 21.0 mm, $P=$ 10 MPa, and $h=$ 1.0 m. As shown in Fig. 15(a), the maximum von Mises stress exceeded the yield strength of the pipeline when the energy exceeded 2500 kJ. Thus, the sensitivity of the energy magnitude was motivated when the value was less than 2500 kJ. The bilinear law fitted in Fig. 15(b) distinctly proved the energystress characteristic via relative slopes. However, the bilinear law exhibits a close connection with the inner pressure, and this may offer an inherent interference on the pipeline resistance to the external force.
Fig. 15. Maxima of effective pipeline stresses with respect to multiple tamping energy levels
a) Timehistory curve
b) Bilinear law
In the pipeline system, pipeline vibrations cause loosening and breakage of the pipeline attachments as well as the pipeline connections [20]. This causes the pipeline to explode if the influence is significant and leads to serious accidents that compromise the safety [21]. From a vibration velocity viewpoint, the maximum resultant pipe velocities under a compacting load were calculated with four different soil types that could support more quantitative data for third party perturbations on the buried pipeline. Based on the results of the previous analysis, buried depth and tamping energy were selected as the variables as shown in Fig. 16 and Fig. 17.
Fig. 16. Pipe vibration velocity under different depths
Fig. 17. Pipe vibration velocity under different tamping energy
The general law for each case was similar and stated that a deeper buried depth led to a smaller vibration, and conversely that a higher load led to a stronger vibration. Each soil type with different parameters played a specific role of a different vibration damper. The damping effects due to different soil parameters were almost consistent especially when the depth exceeded 2.0 m as shown in Fig. 16, and this was not observed in Fig. 17. The prediction process was also performed by using the exponential function fit method, and the maximum resultant velocities of pipe $v\left(h\right)$ and $v\left(E\right)$ for each case was obtained by using five parameters, namely ${v}_{0}$, ${A}_{1}$, ${A}_{2}$, ${t}_{1}$ and ${t}_{2}$ as listed in Table 4. The simulation results of the pipe vibration velocity under different conditions provided a theoretical reference for the field monitoring of a thirdparty disturbance.
Table 4. Fitting parameters of maximum resultant velocity on pipeline under various depth and tamping energy
Parameter

Condition

Gravel

Clay

Loess

Sand

${v}_{0}$

Fig. 15

–1.556

0.776

–0.969

–1.645

Fig. 16

–0.873

10.194

11.404

151109.776


${A}_{1}$

Fig. 15

15.719

9.877

–0.969

14.976

Fig. 16

12.574

–5.097

0.238

–151097.186


${A}_{2}$

Fig. 15

15.719

9.877

12.002

14.976

Fig. 16

–11.700

–5.097

–11.642

–12.594


${t}_{1}$

Fig. 15

1.312

1.077

1.492

1.401

Fig. 16

–13455.090

1275.713

–1786.724

2.050E8


${t}_{2}$

Fig. 15

1.312

1.077

1.492

1.401

Fig. 16

615.517

1275.712

872.844

756.890

4. Limit state analysis
4.1. General engineering limit analysis method
Plastic failure is recognized as a common failure mode for high grade pipeline steel, and thus plastic limit load is an important parameter to determine the bearing capacity of a pipeline and to evaluate the integrity of the structure [22]. In actual working conditions, the stressstrain response exhibits strong nonlinear characteristics when the material is in a plastic deformation stage. In order to avoid computational difficulties caused by a large deformation, the limit analysis method is widely adopted in engineering, and the following three limit analysis methods correspond to general options:
1) Tangent Intersection (TI) criterion was proposed by Save [23], and as shown in Fig. 18(a), the ultimate load ${P}_{lt}$ is defined as the intersection of two tangent lines that are drawn based on the elastic stage and plastic flow stage of the load  strain ($P\epsilon $) response by testing.
2) Double Elastic Slope (DES) criterion is accepted as an approximate criterion by multiple versions for boiler and pressure vessel code of ASME [24], and the ultimate load ${P}_{l\phi}$ is determined by the intersection of the experimental loadstrain ($P\epsilon $) response and double elastic slope line as shown in Fig. 18(b).
3) Zero Curvature (ZC) criterion was proposed by Zhang et al. [25] who improved the ZC criterion based on the TI criterion, and defined the ultimate load ${P}_{lc}$ as the load value at the separation points of the load  strain ($P\epsilon $) curve and the tangent of the plastic stage as shown in Fig. 18(c).
5. Limit analysis of pipeline under dynamic consolidation load
In order to determine the extreme state for a pipeline under a consolidation load, the load in Fig. 18 is converted into the relevant variables in Table 3, and the strain is considered as the maximum total stain under various conditions. Thus, it is necessary to postprocess the relationship between extreme total strain ε and buried depth $h$, wall thickness $T$, and tamping energy $E$. The strain results for specified operating conditions are listed in Table 5.
Fig. 18. Three common limit load criteria
a) TI criterion
b) DES criterion
c) ZC criterion
Table 5. Total strain for different conditions for buried gas pipeline with respect to tamping load
(1): Clay soil type, X70 pipeline, ${D}_{p}=$ 1016 mm, $P=$ 10 MPa, $T=$ 21 mm, $E=$ 2500 kJ


Buried depth $h$ (m)

0.5

0.8

1.0

1.5

2.0

2.5

3.0


Total strain $\epsilon $ (×10^{3})

3.6482

2.4103

2.135

1.7173

1.4257

1.2126

1.105


(2): Clay soil type, X70 pipeline, ${D}_{p}=$ 1016 mm, $P=$ 10 MPa, $h=$ 1.0 m, $E=$ 2500 kJ


Wall thickness $T$ (mm)

14.6

17.5

21.0

26.2

28.0


Total strain $\epsilon $ (×10^{3})

3.4748

2.729

2.2074

2.0141

1.9072


(3): Clay soil type, X70 pipeline, ${D}_{p}=$ 1016 mm, $P=$ 10 MPa, $T=$ 21 mm, $h=$ 1.0 m


Tamping energy $E$ (kJ)

1000

1500

2000

2500

3000

3500

4000

4500

5000


Total strain $\epsilon $ (×10^{3})

1.6884

1.7986

2.074

2.2449

2.4838

2.9448

3.1002

3.6665

3.8718

Based on three conditions listed in Table 5, straindepth ($\epsilon h$) curve, strainthickness ($\epsilon T$) curve, and strainenergy ($\epsilon E$) curve are composed as shown in Fig. 19(a), 19(b), and 19(c), respectively. The limit buried depth (${h}_{lt}$ by TI criterion, ${h}_{l\phi}$ by TES criterion, ${h}_{lc}$ by ZC criterion), limit wall thickness (${T}_{lt}$ by TI criterion, ${T}_{l\phi}$ by TES criterion, ${T}_{lc}$ by ZC criterion), and limit tamping energy (${E}_{lt}$ by TI criterion, ${E}_{l\phi}$ by TES criterion, ${E}_{lc}$ by ZC criterion) of a buried gas pipeline under a tamping load were obtained by applying three limit analysis methods as described in Section 4.1. For example, with respect to the clay medium, the limit value by the TI criterion are as follows: ${h}_{lt}=$ 0.943 m (Fig. 19(a)) and ${T}_{lt}=$ 19.073 mm (Fig. 19(b)), and they were more conservative than the other limit criterions (${h}_{l\phi}={h}_{lc}=$ 0.785 m, ${T}_{l\phi}=$ 16.927 mm, and ${T}_{lc}=$ 17.500 mm). With respect to the limit tamping energy, the conservative ordering corresponded to ${E}_{l\phi}>{E}_{lc}>{E}_{lt}$ as shown in Fig. 19(c), which was contrary to the depth and thickness.
Fig. 19. Limit analysis of buried gas pipeline with respect to tamping load (cases in Table 5)
a) Total strain vs. depth
b) Total strain vs. wall thickness
c) Total strain vs. tamping energy
Fig. 20 shows more limit analysis results of a pipeline under multiconditions where additional von Mises yield stress criteria were used. With respect to the limit of the buried depth of pipeline shown in Fig. 20(a), the results with open blue squares by the TI criterion depict relatively conservative characteristics. In contrast, the yield stress criterion prediction with a solid pink inverted triangle is observed more clearly. Additionally, the buffer capacity of clay exceeds those of the other mediums, with the mean limit depth sequence that corresponds to Gravel > Loess > Sand > Clay, and clay also exhibited the lowest standard deviation as shown in the performed descriptive statistics plots. With respect to the limits of the wall thickness of the pipeline in Fig. 20(b), the results with respect to the yield stress criterion were more conservative than the others. The ZC criterion with an open green triangle exhibited a relatively smaller limit prediction value in gravel and sand. The lowest values of the TES criterion were observed for clay and loess. The order of the mean limit wall thickness corresponded to Gravel > Sand > Loess ≈ Clay. With respect to the limit of the tamping energy of the consolidation process as shown in Fig. 20(c), the TES criterion with a conservative property was only suitable for clay, and null for other soil types. The shock resistance of clay was also reflected by the mean energy limit values, which followed the order of Clay > Loess > Gravel > Sand. Thus, a higher value increased the buffer capability. The energy limitation data exhibited significant fluctuation as compared with those of the depth and thickness and especially with respect to the gravel and clay analysis.
Fig. 20. Limit analysis results under multiconditions
a) Limits of buried depth
b) Limits of wall thickness
c) Limits of tamping energy
6. Conclusions
1) In this study, it is considered that the damping dissipation of a structure, such as buried gas pipeline, can be divided into a mass point movement part and strain rate related part, which are imported into the Lagrange function. Additionally, an implicit finite element scheme based on the Hamilton principle is established for the dynamic control equation of a nonconservative system composed of an elastoplastic material.
2) The finite element model of a compaction process with multiconditions is developed and simulated by a LSDYNA explicit solution method. The buffer mechanism of different soil types is assessed by using a onetoone comparison where a significant role is played by clay in cushioning a steel weightsoilpipeline system while gravel exhibits poor buffer performance. A total of 84 cases are investigated to identify the specific response law with respect to pipeline overload on the ground. The following results are obtained: 1) the magnitude on the covered soil thickness and tamping energy produced increased turbulence on pipeline as compared with that created by the wall thickness and that for the vibration velocity characteristic; 2) a significant residual stress appears under various wall thicknesses, and this barely affects the maxima of vibration velocity of a pipeline with different wall thicknesses; 3) a clear sensitivity and insensitivity boundary are statistically illustrated in both depthstresstime response and energystress response where the former is located at approximately 1.0 m, and the latter has approximately 2500 kJ.
3) Based on the parametric analysis, four failure criterions are applied to determine the limit status of high toughness pipeline in specific cases. Generally speaking, clay supports increased damping ability with respect to an underground structure as compared with the other three soil types. With respect to the limit depth and limit wall thickness viewpoint, gravel soil exhibits the worst resistance capability with respect to external forces while sand performs the worst from the limit tamping energy viewpoint. The results indicate that the chat TI criterion, von Mises yield stress criterion, and ZC criterion always achieve relatively conservative results with respect to limit buried depth, limit wall thickness, and limit tamping energy, respectively. Thus, it is necessary to carefully inspect the applicability of TES criterion and especially for the limit tamping energy analysis.
Acknowledgements
The authors appreciate the financial support provided by “The Young Scholars” Development Fund of Southwest Petroleum University of China. The authors declare that there is no conflict of interest regarding the publication of this paper.
References
 Kent Muhlbauer W. Pipeline Risk Management Manual: Ideas, Techniques, and Resources. 3rd Edition, Gulf Professional Publishing, 2004. [Search CrossRef]
 Gas Pipe Line Incident: 19702001 5th Report of The European Gas Pipe line Incident Date Group, 2002. [Search CrossRef]
 Xu T. L., Yao A. L., Jiang H. Y., et al. Key techniques of risk assessment of oil and gas pipelines damaged by thirdparty. Journal of Oil and Gas Technology, Vol. 33, 2011, p. 150154. [Search CrossRef]
 Kong L. W., Yuan J. X. Study on surface contact stress and settlement properties during dynamic consolidation. Chinese Journal of Geotechnical Engineering, Vol. 20, 1998, p. 8692. [Search CrossRef]
 Tong X. D., Jiang Y. S., et al. A new method for dynamic contact analysis. Engineering Mechanics, Vol. 17, 2000, p. 8286. [Search CrossRef]
 Jiang P., Li R. Q., Kong D. F. Numerical analysis of large deformation impact and collision properties during dynamic compaction. Chinese Journal of Geotechnical Engineering, Vol. 22, 2000, p. 222226. [Search CrossRef]
 Tian S., Wang Z. Explicit nonlinear numerical analysis of dynamical performance of dynamic compaction. Rock and Soil Mechanics, Vol. 29, 2008, p. 15801584. [Search CrossRef]
 SongXiuguang Dynamic Analysis of Consolidation. Hehai University, Nanjing, 1997. [Search CrossRef]
 Li Benping Consolidation Mechanism Analysis by Finite Element Method. Zhejiang University, Hangzhou, 1993. [Search CrossRef]
 Chow Y. K., Yong D. M., et al. Dynamic compaction analysis. Journal of Geotechnical Engineering, Vol. 118, Issue 8, 1992, p. 11411157. [Search CrossRef]
 Brandl H., Sadgorski W. Dynamic stresses in soil caused by falling weights. Proceedings of the Ninth International Conference on Soil Mechanics and Foundation Engineering, Vol. 2, 1977, p. 187194. [Search CrossRef]
 He C. M., Zou J. F., Li L. Field tests on measurement of dynamic stress of dynamic compaction. Chinese Journal of Geotechnical Engineering, Vol. 29, 2007, p. 628632. [Search CrossRef]
 Dunne F., Petrinic N. Introduction to Computational Plasticity. Oxford University Press, 2005. [Search CrossRef]
 Fan T. Study on the Elastic Mechanics QuasiVariational Principles of Nonlinear NonConservative Systems. Harbin Engineering University, 2007. [Search CrossRef]
 Fan J. H., Gao Z. H. Nonlinear Continuum Mechanics Foundation. Chongqing University Press, Chongqing, 1987. [Search CrossRef]
 LSDYNA Keyword User’s manual (970V). Livermore Software Technology Corporation, Livermore, 2003. [Search CrossRef]
 Cowper G. R., Symonds P. S. Strain Hardening and Strain Rate Effects in the Impact Loading of Cantilever Beams. Brown University, Applied Mathematics Reports, 1958. [Search CrossRef]
 Chen Z. J., Yuan J. H., Zhao Y. Impact experiment study of ship building steel at 450MPa level and constitutive model of CowperSymonds. Journal of Ship Mechanics, Vol. 11, 2007, p. 933941. [Search CrossRef]
 Zhao S. P., Zeng X. G., Yao A. L., et al. Dynamic response numerical simulation of buried gas pipeline during thirdparty interference. Sichuan Building Science, 2009, p. 138139. [Search CrossRef]
 Tian Jialin, Yuan Changfu, Yang Lin, et al. Vibration analysis model of pipeline under action of gas pressure pulsation coupling. Engineering Failure Analysis, Vol. 66, 2016, p. 328340. [Search CrossRef]
 Wang C. Q., Chai J. S., Niu W. W. Research on consequence assessment system of natural gas pipeline leakage accidents. Applied Mechanics and Materials, Vols. 295298, 2013, p. 744748. [Search CrossRef]
 Liang W. J., Chen P., Sheng S. P., et al. Limit Load Numerical Analysis of Pressure Pipe with Incomplete Welding Defects. Light Industry Machinery, 2008. [Search CrossRef]
 Save M. Experimental verification of plastic limit analysis of torispherical and toriconical heads, pressure vessels and piping: design and analysis. Pressure Vessels and Piping – Design and Analysis, Vol. 1, 1972, p. 382416. [Search CrossRef]
 ASME, 2004, Boiler and Pressure Vessel Code Section VIII, Division 2. American Society for Mechanical Engineers, New York, USA. [Search CrossRef]
 Zhou Z. H. A Method of Hamiltonian System for Fracture Problems and Its Applications. Dalian University of Technology, 2011. [Search CrossRef]
Cited By
Ocean Engineering
M. Ezzati, M. Naghipour, M. Zeinoddini, A.P. Zandi, M. Elyasi

2020
