In-field flowlines transfer production among subea wells to the production facilities. The processed hydrocarbons will be transferred to the shore through the export pipelines. The subsea flowline or pipeline is installed on the seabed and is subjected to wave and current loading.
The main scope to design a pipeline system is presented below.
Pipeline design begains with material selection and pipe sizing to withstand the inernal or external overpressure. When the pipe diameter is selected for the flow consideration, the pipe wall thickness is designed for internal pressure containment, which is to prevent the pipe burst failure due to the internal pressure. Pipe should also be designed to prevent the collpase and propagating buckling failure due to the external over pressure.
30 CFR 250 has the following formulation for internal pressure design: \[P = {2\cdot S\cdot t \over D}F\cdot E\cdot T \tag{1}\label{eq1} \] where
30 CFR 250 uses Barlow's Equation to calculate the internal design pressure that a pipe can withstand to its dimensions and the strength of its material. The design factor of 0.6 indicates the the hoop stress due to the internal design pressure should be limited to 60% of yield strength for riser component.
The Federal Regulations codes and industrial standards employ Barlow's Equation to calculate the internal design pressure that a pipe can withstand, considering its dimensions and material strength. A constant hoop stress along the wall thickness is calculated, which should be less than 72% of the yield strength. The required wall thickness based on ASME codes is typically less than that required by CFR codes. ASME codes use the differential pressure, whereas CFR codes consider the internal design pressure only. The formula for riser wall thickness internal pressure design (burst) is presented below in Table 1.
Pipeline | Code | Formula | Design Factor F | Pressure |
---|---|---|---|---|
DOI Pipelines | 30 CFR 250.1002 | t=PD/(2SEFT) | 0.72 | Internal |
API RP 1111 | pb=k(S+U)ln(D/Di), p<F*pb | 0.72 | Differential | |
DOT Pipelines (Liquid) | 49 CFR 195.106 | t=PD/(2SEF) | 0.72 | Internal |
30 CFR 250.1002 | t=PD/(2SEFT) | 0.72 | Internal | |
B31.4 A402.3.2 | t≥pD/(2FS) | 0.72 | Differential | |
API RP 1111 | pb=k(S+U)ln(D/Di), p<F*pb | 0.72 | Differential | |
DOT Pipelines (Gas) | 49 CFR 192.105 | t=PD/(2SEFT) | 0.72 | Internal |
30 CFR 250.1002 | t=PD/(2SEFT) | 0.72 | Internal | |
B31.8 A842.2.2 | t≥pD/(2FST) | 0.72 | Differential | |
API RP 1111 | pb=k(S+U)ln(D/Di), p<F*pb | 0.72 | Differential |
API RP 1111 presents the formula to calculate the pipe burst pressure and set up the 72% of the burst pressure as the limit of the design pressure. The burst pressure formula from pipe testing or can be verified using finite element analysis method (von Mises stress at the outfer reaches the yield strength). It's worth noting that calculations based on CFR using Barlow's Equation are often conservative for thick-walled pipes. A request to use API RP 1111 to determinethe wall thickness is an alternate compliance from requirment of 30 CFR 250 per BSEE NTL 2009-G28.
Pipe collpase pressure are calculated based on pipe material and size. API RP 1111 utilizes a collapse factor of 0.7 (limiting the external overpressure to 70% of the collapse pressure) for seamless or ERW pipe, while applies a collapse factor of 0.6 for cold expanded pipe, such as DSAW pipe.
Pipeline is also checked for propagating buckling due to the external hydrostatic pressure. The propagating buckling case is checked exclusively at the maximum water depth, where the maximum net external overpressure are located, assuming a minimum internal pressure of zero. As the pressure requried to start a propagating buckling is smaller than the pressure required to initiate collapse, it is often not economical to prevent the propagating buckling by increasing the pipe wall thickness, epsecially for deepwater pipelines. Instead, Buckle arrestors may be used if external overpressure exceeds 80% of propagating pressure per API RP 1111.
The pipeline is installed on the seabed and is subjected to wave and current loading. The assessement of on-bottom stability includes both vertical and lateral stability design. Three methods for lateral stability are considered:
Before pipeline stability is assessed, the following parameters, such as pipe weight, penetration, and enviromental loads must be determined.
The pipe weight calculation includes the pipe metal, coatings (anti-corrosion, insulation, or concrete weight coating), contents, and marine growth. The calculation is performed for three conditions: installation, embedment, and operation. The weight difference arises from varying fluid contents. Pipe metal loss due to corrosion is only considered at the operational stage.
The initial penetration, zpi, is due to the self-weight of the pipe prior to lateral movement. This value can either be provided or calculated using the following models. An iterative procedure is performed to determine the initial pipe embedment after laying, based on the equilibrium between the pipeline's contact force and the bearing capacity of the soil. The initial penetration in clay can be calculated using the Verley and Lund model, while the initial penetration in sand can be calculated using the Verley and Sotberg model.
The initial penetration will be added to the penetration caused by dynamics during laying, penetration due to pipeline movement under waves and current, and penetration due to piping to calculate the total pipeline penetration, zp.
The hydrodynamic load reductions due to pipeline penetration and trenching are applied to the absolute stability calculations. Load reduction due to a permeable seabed is not considered in this assessment.
Two basic wave parameters, significant wave height Hs and peak wave period Tp, are provided. The JONSWAP or other spectrum is applied as the appropriate spectral density function. The significant flow velocity amplitude \(U_s\) and the mean zero up-crossing period \(T_u\) of the oscillating flow at the pipeline level can be calculated using the spectral moment. The spectrally derived characteristics - oscillatory velocity, period and the associated steady current velocity V - are the main paramters for the generalized lateral stability assessment.
Stability design criteria provide methods and acceptance standards for the vertical and lateral stability of pipelines. Vertical stability ensures that flotation in water is avoided. The submerged weight of the pipeline must exceed the safety factor on buoyancy, which usually is a value of 1.1. If the pipeline's submerged weight does not satisfy this criterion, a concrete weight coating should be added to increase the pipeline's specific gravity to at least the safety factor.
An example is shown in the table below to check the pipe vertical stability in water (to avoid floatation). Initially, no concrete weight coating is specified. Since the pipe's specific gravity of 1.146 without the coating is greater than or equal to the required buoyancy safety factor of 1.1, the submerged weight of pipeline meets the vertical stability criterion to avoid floatation.
Concrete Weight Coating (CWC) | CWC Thickness, mm | Pipeline Specific Gravity |
---|---|---|
Existing | 0.0 | 1.146 |
Absolute static stability is a simplified and conservative approach based on the quasi-static equilibrium of forces, aimed at ensuring that the pipeline will experience no break-out under the design extreme single wave-induced oscillatory cycle in the sea state.
Virtual stability design allows for displacement of less than approximately half a diameter under the largest waves in a sea state. In this condition, the pipeline is considered virtually stable and will not experience break-out. This optimized approach may also benefit from the build-up of passive resistance.
Limited accumulated displacement design permits accumulated displacement of up to 10 hydrodynamic pipeline diameters. Under this design, the pipeline will break out of its cavity multiple times during the sea state, and the calculated displacement should be assumed to be proportional to time.
For a pipeline on sand, the minimum pipeline weights required to achieve virtual stability and to limit lateral displacement to 10D during a three-hour stormshould be determined using database solutions. For a pipeline on clay, the significant weight parameters that satisfy the virtual stability criterion and the 10D criterion are defined using emprical equations.
The stability utilization ratio (UR), defined as the ratio of the required submerged weight for stability to the actual submerged weight, should be less than or equal to 1.0 to meet the stability requirements. An example is shown in the table below to check the pipe absolute static stability & generalized stability. As illustrated in the previous table, no concrete weight coating is required to avoid floatation. However, the stability does not meet either the absolute static stability or generalized lateral stability requirements without concrete weight coating, as the URs exceed 1.0. The required concrete weight coating thickness is calculated to meet the stability criteria. For example, to reduce the 10D displacement stability UR of 1.515 to 1.0 and meet the limited displacement stability criterion, the required concrete weight coating thickness must be increased to 29.9 mm.
To Meet Stability Criterion | Required CWC Thickness, mm | Absolute Static Stability | Generalized Stability | |||
---|---|---|---|---|---|---|
Vertical UR | Lateral UR | Virtual Stability UR | 10D Disp. Stability UR | Generalized Stability Applicable? | ||
Vertical stability in water | 0.0 (Existing) | 1.501 | 1.961 | 1.636 | 1.515 | Yes |
Absolute static vertical | 31.6 | 1.000 | 1.961 | 1.636 | 1.515 | Yes |
Absolute static lateral | 323.4 | 0.437 | 1.000 | 0.277 | 0.372 | Yes |
Virtual stability | 32.3 | 0.994 | 1.702 | 1.000 | 0.976 | Yes |
10D Displacement | 29.9 | 1.017 | 1.718 | 1.028 | 1.000 | Yes |
To meet the stability requirements, the pipeline should be designed with a concrete weight coating thickness as summarized in the following table. The required CWC thickness for absolute static stability is not feasible since it exceeds the maximum applicable thickness, usually 150 mm.
To Meet Stability Criteria | Pipe Allowable Movement | Required Concrete Coating Thickness, mm |
---|---|---|
Absolute Static Stability | No movement | 323.4 (not feasible) |
Virtual Stability | Less than half the pipeline's diameter | 32.3 |
Limited Displacement Stability | Up to 10x pipeline's diameter | 29.9 |
The pipeline is installed on the seabed and may have the fee spans. The pipeline free spanning assessment addresses fatigue screening and ultimate limit state (ULS) design due to in-line and cross-flow VIV, as well as direct wave loading. Three key design considerations are evaluated based on the following criteria:
The pipe weight calculation for the free spanning assessment is similar to the weigth calculation for pipeline stability assessment. The submerged pipe weight and specific gravity for each phase are calculated and provided for the pipeline free spanning assessment.
The flow velocity at the pipe level is calculated similar to those calculated for pipeline stability assessment. The main wave parameters, including significant wave height Hs, peak wave period Tp, and wave direction θ, are provided. The spectrally derived significant wave velocity \(U_s\), wave period \(T_u\) and the current velocity \(U_c\) are key paramters for the pipeline free spanning assessment. The significant flow velocity amplitude and the mean zero up-crossing period of oscillating flow at the pipeline level can be calculated using the spectral moment. The sea state paramters (Hs, Tp, θ) are transformed into (Us,Tu) at the pipe level.
The pipe effective tension (axail force) is used to calculate the pipe fundamental natural frequency. The pressure and temperature difference from the installation phase is used to calculate the effective axial force. The effective axial force can be estimated using non-linear finite element analysis and input to this module, or by applying the simplified formulas for thin-walled pipes and thick wall pipe.
When the lowest (fundamental) natural frequencies in the in-line direction for a given free span exceed the VIV
onset frequencies, the onset of in-line VIV is not expected to occur.
When the lowest (fundamental) natural frequency in the in-line direction for a given free span
exceed the VIV screening frequency, a fatigue life of more than 50 years is expected. If the VIV screening
criteria are violated, a full fatigue analysis should be performed.
The following figure shows the pipe natural frequency and in-line VIV onset and screening for operation phase.
For operation phase, in-line VIV is not expected if the span length is less than the VIV onset length of 20.9m. If the span length is more than the VIV onset length of 20.9m, in-line VIV is possible. The fatigue life due to in-line VIV is in excess of 50 years if the span length is less than the VIV screening length of 22.1m. If the span length is more than the VIV screening length of 22.1m, the fatigue life due to in-line VIV is less than 50 years and more detailed fatigue analysis should be performed.
When the lowest (fundamental) natural frequencies in the cross-flow direction for a given free span exceed the VIV
onset frequencies, the onset of cross-flow VIV is not expected to occur.
When the lowest (fundamental) natural frequency in the cross-flow direction for a given free span
exceed the VIV screening frequency, a fatigue life of more than 50 years is expected. If the VIV screening
criteria are violated, a full fatigue analysis should be performed.
The following figure shows the pipe natural frequency and cross-flow VIV onset and screening for operation phase.
For a span in the effectve range shown in Figure 2, the minimum structural frequency is 1.94Hz when the span length is 18.8m. The cross-flow onset frequency is 0.96 Hz and the cross-flow screening frequency is 0.70 Hz, which are independent of the span length. Since the cross-flow onset frequency is less than the minimum structural frequency, no cross-flow VIV onset is expected. Since the cross-flow screening frequency is less than the minimum structural frequency, a fatigue life in excess of 50 years is exprected for cross-flow VIV.
The response model is applied to estimate the magnitude of the dynamic response in a free span.
For in-line VIV, the maximum steady-state amplitude response primarily depends on the reduced velocity and
the stability parameter. The amplitude response for cross-flow VIV is a function of the reduced velocity.
The cross-flow response model is also applied for low KC regimes under current-dominant conditions.
The response model is applied to estimate the magintude of dynamic response in a free span, which will be used for VIV-induced bending calculation.
One example of an in-line respsone model (normalized amplitdue as a fucntion of reduced velocity) is shown in Figure 3.
One example of an cross-flow respsone model is shown in Figure 4.
The design bending moment is the resultant of the two static moments (horizontal and vertical) and the two dynamic moments due to in-line and cross-flow VIV. The pipe, subjected to the design bending moment, effective axial force, and pressure, should satisfy the local buckling combined loading criteria.