freespan-120822234657-phpapp01.pdf
TRANSCRIPT
� Seabed irregularities (unevenness) during installation (residual tension on span creation is closely linked to the pipe weight).
� Subsequent scouring(sand wave) and movement.
�Seabed topography and composition (type of soil), wave and current action and pipe properties.
End Condition Using in Free Span� Fixed- Pinned end condition may be assumed for
single spans. Fixed- Fixed may only be assumed ifvalidated be observed support condition.
� "Fixed/Pinned" in this case is assumed to be theaverage of "Fixed/Fixed“ and "Pinned/Pinned"bending moments, on the basis that the endfixities of a span are somewhere between the twocases but it is difficult to determine exactly where.
� When calculating permissible span lengths, theassumed end conditions have a large impact onthe results.
� The fixed/pinned assumption may not be accuratewhen, for example, a pipeline spans between tworock ridges. The support conditions might then becloser to pinned/pinned; though the adjacentsections of pipe will provide some restraint so thatthe pipe section is not truly pinned/pinned.
� Analytically, it is only possible to accuratelydetermine these effects with the use of anadvanced finite element analysis to accuratelymodel the span support conditions and axialeffects.
� It is obviously impractical to perform this type ofanalysis on every span along the pipeline route.However, it may be possible to build a "typical" FEmodel to determine the magnitude of theseeffects and modify the limiting span criteria.
II. Criteria for Span Condition
Static StressVortex Shedding
Induced Vibration:
In Line; Cross Flow;
Bar Buckling Fatigue.
A. DNV-1981
1. Static Stress� Checked individual stress components, and the total
combined stress condition is also limited to maximumpercentage of the material SMYS (percentage isvariable according to pipeline loading condition).
2. Vortex Induced Vibration � VIV dependent upon the pipe and span characteristics,
fluid flow around a pipeline span can result in vorticesoccurring on the wake side of the pipe. If vortices areof sufficient frequency, they can produce significantpipeline oscillations.
� The parameter assessment VIV is “ Reduced Velocity”(Vr ).
�0 < Vr < 2.2 symmetric vortex shedding producing "In-Line" oscillations, i.e. parallel to fluid flow.
�2.2 < Vr < 3.5 alternate vortex shedding causing "In-Line"oscillations (unstable);
�4.8 < Vr < 12.0 alternate vortex shedding causing “Cross
Flow" oscillations i.e. perpendicular to fluid flow.
�4.8 < Vr < 12.0 alternate vortex shedding causing “Cross
Flow" oscillations i.e. perpendicular to fluid flow.
3. Bar Buckling� For a restrained pipeline, the pressure and
temperature induced axial force (compressive), ifof sufficient magnitude, may lead to beam modebuckling of the pipeline
� For a restrained pipeline, the pressure andtemperature induced axial force (compressive), ifof sufficient magnitude, may lead to beam modebuckling of the pipeline
4. Fatigue� As mentioned previously, vortex shedding induced
span vibrations may be broadly divided into two categories:
� In-line;
� Cross-flow.
� Cross flow vibrations by their nature are almost always high amplitude and consequently their occurrence should be avoided at all costs, while in-line vibrations are generally of smaller amplitude and may be permissible. The criteria for permitting in-line vibrations fall within assessment of the pipeline fatigue and fatigue usage requirements.
III. CalculationPermissible span lengths for a pipeline
are calculated based on each of the following criteria:
Static stress
Vortex shedding (in-
line vibrations)
Vortex shedding (cross flow vibrations)
Bar buckling.
For each of these criteria the permissible span length should generally be calculated for each of the following four load cases:
Empty
Water filled
Hydrotest
Operation
III. Calculation
2. Static stress� Due to its self-weight and lateral hydrodynamic
loading.
� The combined stresses should be checked againstthe allowable levels of stress given in the relevantcodes, i.e. is not to exceed thepermissible value.
� What are “a” and “b” ?
η .ep = usage factory as defined table below δ .F = specified minimum yeild strength
III. Calculation
� Effective mass (me) is function of Ca (add mass coefficient).
� Submerged Weight(Wsub)
� The relationship between VR and the stability parameter, KS
� 1<Vr<3.5 and Ks<1.8 : resonant in-line vortex shedding include oscillationsmay occur.
• The possibility of fatigue damage from in-line VIVs may therefore be
ignored if this criteria is violation.� Vr > 4.7 and Ks <16 crow-flow oscillation may occur.
• Cross-flow VIVs may be assumed not to occur if this criteria is violation.
III. Calculation
� The Reduced Velocity for In-line Vortex Shedding as figure A.3
� The calculation In-Line Vortex Shedding method is now the same as for the Cross Flow. i.e.
Other Method� The natural frequency based on document “ANALYSIS OF SPANS FOR SUBMERGED
PIPELINES (Shell)”:
Methodology1. The fundamental natural frequency (first Eigen
frequency) may be approximated by
2. The reduced velocity, VR, is defined as:
Methodology3. Onset Span Lengths :
Given(for In Line Onset spanLength)� finding Leff:
Given(for Cross flow Onset span Length)� finding Leff
What is this mean “Onset” ?Check all the MathCAD file , the span length due to onset span length is bigger/smaller span length due to Screening criteria.
Finding Vr (Reduced Velocity) ?.�Reduced Velocity for In Line Flow is defined in section 4.3.5 DNV RP F105� Reduced Velocity for Cross Flow is defined in section 4.4.4 DNV RP F105
Methodology
4. Screening Fatigue CriteriaThe In-line natural frequencies fn,IL must fulfill:
The Cross-Flow natural frequencies fn,CF must fulfill:
5. Given f =f finding maximum 5. Given f1=fnIL finding maximum free span length due to Inline flow. Given f1=fnCL finding maximum free span length due to CrossFLow.
Methodology
2. Fatigue Criterion
� ??????????
3. ULS Criterion(Ultimate Limit State)
Local buckling check for a pipeline free span shall be in compliance with thecombined loading – load controlled condition criteria in DNV-OS-F101, Sec.5 orsimilar stress-based criteria in a recognised code. Functional and environmentalbending moment, axial force and pressure shall be accounted for. Simplifications areallowed provided verification is performed by more advanced modeling / analyses incases where the ULS criteria become governing.
a) Input Data
�Hoop Stress:
Methodology
Section D505
Section D505
�Axial Force
Where: H = Effective (residual) lay tension
Δ pi = Internal pressure difference relative to as laid
ΔΤ = Temperature difference relative to as laid
�Characteristic plastic axial force resistance:
�Characteristic plastic moment resistance:
�Drag Force:
Where:
Other parameter is defined in DNV RP F105 , from section 5.4.4 to 5.4.8
Methodology�Inertial Force :
Where:
Other parameter is defined in DNV RP F105 , from section 5.4.10 to 5.4.13
: �The pressure containment resistance: F101-Eq5.8
�Characteristic collapse pressure is finding as: Eq. 5.10
�Plastic Collapse Pressure: F101-Eq5.12
�Elastic collapse pressure, see Eq. 5.11
MethodologyLoad-Controlled Combined Loading Check b) Load-Controlled Combined Loading Check
� Pipe members subjected to bending moment, effective axial force and external overpressure shall be designed to satisfy the following equation:
Applies for D/t2 <45, Pi>Pe
Where: Msd : The design moment is sum of maximum environmental bending moment due to in-line and cross-flow VIV (Dynamic) and static bending moment
Submerged Weight
Pcr Critical buckling load (positive sign)
The stiffening effect of concrete (CSF)coating may be accounted for by:
Methodology� Normalised Moment
� Design effective axial force
� Normalised Effective Force
�Which calculation using Check?
γ.F=Functional Load factor (S4 G201)
γ.c=Condition Load factor (S4 G203)
Applies for D/t2 <45, Pi<Pe
c) Validity Check
Maximum length for response model validity
Cross flow deflection
a
Methodology and Summary
C. COMPARE TWO METHOD CALCULATION FREE SPAN LENGTH
Coefficient DNV 1981 DNV RP F105
1. ReducedVelocity
� Interpolate for figure (notaccurate)
� Equation (accurate)
2. StaticStress
�Comparison with Yielding Criteria,Von Misses Stress included allparameters as:�Bending Stress�Hoop Stress�Hydrodynamic Load�Longitudinal Stress�Thermal Stress�Poisson Stress
�ULS check (Combined LoadingCheck) based on parameters as:�Bending Moment�Hoop Stress�Hydrodynamic Load�Axial Force
SummaryCoefficient DNV 1981 DNV RP F105
3. Dynamic Stress � Maximum span length based on theexcitation frequency (due to Vr-Interpolatefor figure )
� Maximum span length based on Screeningand Onset criteria
4. Bar Buckling � Maximum span length based on axial force � Not required, summary in ULS checks.
5. Fatigue Check � Required (but the sequence calculation ofmethod is not finding)
� Required when Screening Criteria isviolated.
6. Validity Check � Not required � Check the free span length is smaller140.D, deflection is invalid/Ok, Bucking isnot influence the response/ buckled(Onset Criteria).
7. Result �Bigger (see example free span length 40m) �Smaller (i.e the number is smaller <40m
Supplementary(wave)1. Analytic wave theories
Wave Theories are developed for constant water depth d. The objective of a wave theory is to determinethe relationship between T and λ and the water particle motion throughout the flow.
Supplementary (wave)
1. The different of wave theory
o if Ur<48.35, Airy theory / Airy Lagrange / Stocker 1st using sin/cos function
o Ur≥48.35 ,Cnoidal theory using Jacoby Eliptic function/ Stocker 2nd ,3rd ,4th ,….n
o Ur=∞ ,Limit solitary wave.
Fig 1:Ranges of validity for various wave theories.
Detail of the wave theory ref DNVRP C205
Supplementary (wave)
2. Defined Deep Water
� Deep water waves can be defined as those for which or more usefully:
� Shallow water waves can be defined as or
� Intermediate water as other section.
Supplementary (wave)
� All the wave theory: Airy, stocker, Cnoidal and Solitary are regular kinematics wave and waveperiod T remains constant but reality wave always random field.
I. Classification wave spectrum following specific characteristics wave
� Frequency spectrum;
� Direction spectrum;
� Energy Spectrum ;
� Height Spectrum.
II. Classification wave spectrum following geographical name or famous man� Pierson –Mosskowitz spectrum first time (P-M);
� Pierson –Mosskowitz spectrum second time;
� Bretschneider – Mitsuyasu spectrum (B-M);
� Jonswap spectrum (Joint North Sea Wave Observation Project);
� Neumann spectrum;
� Roll Fisher spectrum;
� Storckelov spectrum;
� Burling spectrum;
� Krulov spectrum;
� Bretschneider spectrum;
� Davidan spectrum.
III. Classification wave spectrum following water depth
� Deep water;
� Shallow water;
3. Wave spectrum classification