TECHNISCHE UIUVERSITEIT Laboratodwn or Scheepshydromechanîca Archief Mekelweg 2, 2628 CD Deift Tel.: 015- 786873-Fax: 015-781836
WEGEMT SCHOOL
DESIGN AND ANALYSIS OF SLENDER MARINE STUCTURES
- RISERS AND PIPELINES
CONTRIBUTION BY PROFESSOR D GARETH OWEN
HERIOT- WA lT UNIVERSITY
MARINE RISERS
CONTENTS
CHAPTER 1 INTRODUCTION
CHAPTER 2 RIGID TENSIONED MARINE RISERS 2.1 Description of System
2.3 Riser Components
2.4
Design Considerations2.5
Inspection and Maintenance2.6
Static and Dynamic Analysis of Vertical Tensioned Marine Risers2.7 Model Tests of Tensioned Risers
CHAPTER 3 FLEXIBLE RISERS
3.1 Description of Systems and Components 3.2 Riser Configurations
3.3
Design Considerations for Flexible Marine Risers
3.4
Installation and Inspection3.5 Dynamic Analysis of Flexible Marine Risers
3.6
Mechanical Behaviour of Flexible Marine Risers
3.7
Experimental Studies3.8
Future Prospects
1. INTRODUCTION
A marine riser is essentially a conductor pipe connected between a fixed offshore platform, a floating platform or a vessel and the welihead at the seabed. The. purpose of
the marine riser is to, provide a conductor for the
conveyance of fluids or drilling hardware between the
platform and the well. In the first sense (viz conductor
for the conveyance of fluids) the conductor is
categorised as a "production riser", while in the second
sense it is categorized as a "drilling riser". There are essentially three kinds of risers
- the rigid integral riser
- the rigid non-integral riser
- the flexible (dynamic) riser
The integral riser design utilizes a structural pipe to support flow-carrying tubulars. The riser is fabricated in 15m joints with mechanical connectors in both ends of
the structural pipe. When the connector is made up, all
the tubular flow paths are made, up simultaneously. This is the concept applied in modern drilling risers.
The non-integral rigid riser design consists of a central
structural pipe supporting vertically spaced guide
funnels or other means of guiding tubulars. Flowline
tubulars are individually run down the riser through the
funnels and latched to the template or manifold. The
structural pipé must be installed and tensioned before
the f lowline tubulars are run. The concept has been
employed successfully in the Argyll and Buchan Fields in
the North Sea.
A flexible dynamic riser design consists of a continuous
flexible pipe or a bundle of flexible pipes, with 'a
specific structure adapted to the production
requirements, connected at the surface (together with the possibility for quick disconnection) and on the seabed.
Flexible risers have some significant technical and
economic advantages, probably the most important one
being their capability to survive a loo .yèar storm
without disconnection: this saves time and miminimises
loss of production.
The original use of marine risers for oil and gas
developments goes back to the early days of the industry.
As oil and gas developments moved offshore, drilling
activities required the use of a conductor between the
drill floor and the sea-bed to act as a conduit for'the
drill-pipe and also to provide an annular space for the
return of the drilling mud. When drilling from fixed
platforms the problem is relatively easily solved by
employing rigid riser pipe that is clamped at intervals
to structural members of the platform along their
vertical run up to the surface. The problem is a more complex one when drilling from a floating or compliant
offshore structure. Since the risers in such circumstances cannot be supported along their- length and--.
only supported at their upper ends at the drilling rig, a number of issues, have to be addressed. In the first
place the riser needs to be maintained under sufficiently
high
tension
at their top to prevent buckling due to self weight of their very slender geometry. In addition, to accommodate the motions of the rig (particularly those inheave), slip joints and flexible jumpers have to be
provided at the upper
endof the
riser.Also the
required tension has to be maintained within acceptable limits by means of a tension compensation system. These
features will be described in more detail at a later
stage in these notes. To prevent overstressing at the
sea-bed a ball-joint is provided. The design of such
rigid tensioned risers was initially dominated by static
considerations. However, in recent years (say the past
two decades) greater attention has needed to be given to the dynamic behaviour of risers. This has been mainly
due to the fact that risers have been increasingly
exposed to more severe conditions (deeper waters, severe wave climates) and this has meant that dynamic effects
have tended to be more important than hitherto.
Furthermore, in the case of production risers, the
operational performance of the floating facility is
critically dependent
on the performance of the riser
system. Thus it had become increasingly important to
predict reliably the maximum riser stresses and
deflections, so that riser designs are compatible with
the anticipated operating and environmental conditions.
As an attractive alternative to the rigid tensioned
production riser, the flexible riser concept has been
developed in recent years. The flexible riser can
accommodate large motions of the surface platform without
the need for the special hardware associated with
tensioned systems (eg flexible jumpers, slip joints, tension compensation, ball-joints etc).
Palmer (1985) has listed the advantages of the flexible riser in comparison with rigid risers, as
follows:-A flexible riser system can accommodate large
motions of the floater.
A flexible riser is generally lighter than a rigid riser, and does not require large axial
tension to keep the bending stress to an
acceptable level. This makes it possible to
eliminate the weight and space needed by riser
tensioning and heave compensation devices.
Since there is less tension in a flexible
riser, its lower end can be simpler, and it
does not need to be so strongly anchored as a
There is more freedom of choice in where to
attach a flexible riser to the floater compared with a rigid system. It does not need to run
through a moonpool, and thus the moonpool is left free for other activities such as well
workovers.
-Because a flexible riser is light and can be
deformed, it can be installed (and if necessary
replaced) by light equipment, based on DP
(dynamically positioned) vessels with minimal
weather dependence and interference with other
vessels.
(vi) The flexibility of the system makes it easier
to alter the configuration and tie in
additional wells during the operating life of
the field.
'While flexible risers are a relatively recent
development as compared to rigid risers, their history
can still be traced as far back as the early 1940's when, during World War II, a long flexible pipe reinforced with braided steel wire was laid across the English Channel to
provide the allies' beach head in France with fuel, as
part of the "Pluto Operation" ' (Chen (1990)).
Flexible risers have been extensively used in connection
with SPM offshore loading and off loading operations since
the late 1950's. Although these hoses should not be confused with flexible marine risers they exhibit many
features that are similar in relation
to both their
construction and design. 'In the early 1970's flexible
marine risers were progressively introduced into the
offshore oil and gas industry. In 1972, flexible pipes produced by COFLEXIP were depolyed as f lowlines in the Emeraude Field (Congo). The next significant mile stone
in the development of flexible pipes was their
application in
1975 as risers in the Poleng Field in
Indonesia. This was followed with the successful
introduction of flexible risers in 1978 in the Enchora
Field in Brazil and later in 1979 at Chevron's Casablanca
Field in the Spanish Mediterranean. Into the 1980's,
with the fall in oil price and the discovery and
exploitation of oil in deeper waters, the past decade has
seen rapid developments and innovative designs for
flexible pipes and pipe systems. Today, flexible pipes
have been used in various parts of the world and have
become more and more important in the offshore oil
industry (from Chen (1990))'. Flexible marine risers, are
progressively replacing rigid tensioned riser systems for
all operations with the exception of those associated
with drilling activities from a floating rig.
(iv)
2 RIGID TENSIONED MARINE RISERS
2.1 Description of System
In fact the term 'rigid' is somewhat ambiguous in that such risers have a considerable degree of movement due to
their stiffness over the length.
As has already been mentioned,
marine risers can be
categorized as either being 'drilling risers' or
'production risers'. Rigid tensioned marine risers can
be used for both areas of application, whereas flexible
risers can only be used as production risers. The
diagram (Figure 2.1) shows schematically the location of the major components of a tensioned riser used within a
drilling riser system. These components comprise
- a connector and flexible joint at the base
- a riser structure in segmented joints
- a tensioning system
- flow connectors at the vessels
Rigid tensioned risers can be further distinguished as
being either 'integral' or 'non-integral' in relation to the structural layout of f lowlines. Such a distinction only really applies to production risers. The nature,
advantages and disadvantages of 'integral' and
'non-integral' riser types is indicated below.
Integral Riser
-
This is built and installed in sections orjoints similar to a drilling riser
- Individual f lowlines cannot be installed or
removed separately
- Internal: tubular f lowlines in this case are
continued wholly within the riser pipe itself
- External: in this case f lowlines are arranged
externally to the central structural pipe that
supports them similar to choke and kill lines
in a drilling riser
Advantages of Integral Riser
These are:
- speed of deployment and retrieval
- they behave well under severe environments
- Internal variety: these can contain and
quickly monitor a leak in a flowing tubular
through the pressure increase in the riser bore
- External variety: these are less expensive in
variety due to difficulties with internal configurations
Non-Integral
RiserThis consists of a central structural pipe supporting
arms with guide funnels which support f lowlines laterally
preventing them from buckling. With regard to
installation, the main structural riser is deployed first
in standard lengths and tensioned, then the f lowlines are run one at a time through the guide funnels.
The advantages of a non-integral riser include the
ability to pull individual f lowlines without disturbing
the entire riser.
Amongst its disadvantages are its relatively slow
installation and retrieval. Also,
in the case of a
weather-related shut-down, the operation to pull the
riser must be commenced well in advance thus
substantially increasing the downtime as compared to an
integral riser.
2.2 Sources of Failure of Tensioned Riser Systems
In general the riser can fail under the following
circumstances:
-When the material at a particular section fails due to overloading or due to load cycles giving rise to a fatigue failure
Local or global buckling, caused by compression
in the riser
Failure due to excessive internal or external
pressure causing 'bursting' (radial outward
stresses) or 'crushing' (radial inward
stresses)
Types of Riser System Failure Modes (see Figure 2.2)
Figure 2.2 refers to the wide variety of failure modes
that can occur in a tensioned riser system. These seven types of failure mode are briefly described below.
1. Distortion of the cylinder cross-section
which can be caused by
-- the existence of a double curvature
bend radii, producing high bending R2(la)
(buckling)
with small moments at
- a lack of buoyancy in the riser producing
collapse of the lower section and excessive
tensioning devices which do nt respond quickly enough for vessel heave may cause the failure
illustrated in ic
- on raising the riser after disconnection,
failure could occur due to insufficient weight
existing in the lower section to
maintain
tension and thereby reduce bending Cid)
Ball Joint Damage may occur due to incorrect
monitoring of th base angle, or vessel wrongly
positioned for current conditions (2 and 3 diagram)
Drill String Fatigue Failure (due tO bending stress reversals) or damage to the BOP causing blowout may occur due to the same reasons as cited in 2. above
(2 and 3 diagram)
4, Riser pipe and/or Conductor Pipe ailures due to
- vertical loads being transmitted through
peripheral shear action at the conductor. The
conductor length is determined by the shear
resistance of the seabed, or
= large bending movements being induced on the
conduôtor column due to the horizontal
component of the riser tension and the weight
of the BOP and horizontal deflection (4) The Emergency Disconnect Fails to Function (5)
Ecçe5sve stress may occur in the riser connection
tO the supplementary buoy.
In most cases of
a
productioñ system with a srf ace vessel and a
submerged buoy, there is a phase difference in
response due to wave loading This may introduce
excessive stress and fatigue conditions at the, buoy
and in the riser segment above the buoy (6)
The conductor pipe may fail and the BOP would
consequently collapse oñto the seabed. This could
ccur due to either
4above or due tO resonant
response of the BOP mass on the elastic column
support, excited by the sea state forming function
2.3 RISER COMPONENTS
The components of a riser system must be strong enough to
withstand high tension and bending moments1 and have
enough flexibility to resist fatigue, yet be as light as practicable to minimize tensioning and f loatation
requirements.
Some detailed information on important riser components
is given below (as presented in Sheffield (1980)).
Riser Joints
A 'riser joint' is constructed of seamless pipe with
mechanical connectors welded on the ends. Kill/choke
lines are attached to the riser by extended flanges of
the connector. The riser can be run in a manner similar
to driilpipe: by stabbing one stalk at a time into the
string and tightening the connector. Ball Joints
'Ball joints' or 'flexible joints' allow limited angular
motion of the riser. In some cases, these flexible
joints may be a series of ball joints. 'Pressure
compensated' ball joints should be used to decrease the torque required to deflect the joint. The forces acting
on the joint push the inner ball against the outer
casing, causing the joint to bind. To decrease the
required torque hydraulic fluid is injected to spread
apart and lubricate the moving parts. With the large
area involved, relatively small pressures are required.
Slip Joints
A 'slip joint' comprises two concentric cylinders or
barrels that telescope. The outer barrel is attached to
the marine riser, and the riser is held in tension by
wire ropes from the outer barrel to the tensioner.
Buoyancy Modules
Buoyancy or flotation modules can be attached to the
riser to decrease the tension required at the surface. These modules may be thin-walled air cans or fabricated
2.4 DESIGN CONSIDERATIONS
Riser Tensioning
The preferred riser tension can be defined for. any given
situation as the tension that will minimize.:. the
probability of damaging the riser yet cause minimal wear
to the tensioners. Adeqúate tension must be held on thé
riser to insure riser integrity and to keep the riser
system (including the ball joint) straight enough to
drill (in
the case of a
drj)ling riser) without the.drilipipe's rubbing and damaging the riser.
The marine risér is analogous to a horizontal steel beam
that is supported at both ends and loaded between the
supports. Ït will sag, but the sag will be less if we
pull on both ends of the beam A riser is similar, but it is nearly vertical and the loading consists of forces
resulting from waves, current, riser weight and the
weight of mud (or transported fluid) in the riser. As
the vessel offset increases, the weight of the internal
fluid and riser weight becomes more important in
influencing bending momements. The riser will sag in a
manner similar to the horizontal beam, and tensioning
likewise will decrease the amount of sagging.
It is convenient to define three modes of operation for
the riser as
follows:-Operational - where the bail joint angle is
les than 4°.
Ñon-operationaì. - when the ball joint angle is greater than 40 The ball joint must be kept 'of.f step' as long as the riser is connected, usually until the vesSel or rig has reached an
of fset of 10% of the water depth.
Disconnected - when the riser is disconnected
from the wélihead, and concern for riser
tension is replaced by concern for tenSiöning
and paying out of the guidelines if the vessel
is movéd.
Non-Operational but Connectéd Mode.
Figure 2.3 is a typical example of maximum/minimum stress
behaviour in a riser when the ball joint is on or near
the stop. When 'on stop', maximum and minimum Stresses
will occur at or near the connection between the riser
and the ball joint. When the ball jòint is 'off stop',
maximum stresses my occur at another position in the
riser In Figure 2 3, the ball joint is just 'off stop'
when the maximum and minimum stresses at the ball joint
become coincidental. For this case,. the ball joint
disengages at about 100 kips (100,000lbs = 45359kg )
Increasing the tension to 150 or 190 kips has little
effect on the riser stress, but decreasing the tension to 50 kips could lead to riser failure. The-minimum tension to be allowed for the conditions stated in Figure 2.3 is
loo kips.
Riser tension cannot be held constant in floating
drilling (or production) operations,
and the applied
tension will fluctuate about a mean setting. This
f luctuation is considered by many in the industry to be
about 15% of the mean tension.
As 100 kips
is theminimum allowable tension, then the tension should be set above 100/0.85, or 118 kips. At a setting of 118 kips, the tension is expected to fluctuate between 100 and 136
kips. This is the 'calculated' tension settings to
minimize the riser stresses for 10% offset and the
conditions listed in the figure. Lower offsets will
require lower tension settings using the same criterion;
however, tensioners are not designed to change tension
rapidly if something should happen. Thus tension
settings for field operations should be based on the
possibility of a failure of systems that will affect
riser stresses.
Operational Mode
Four degrees is the maximum ball joint angle that can be
tolerated without damaging the riser and the BOPs during drilling and other operations. The four-degree angle is
based on experience combined with experimental data of
researchers. In practice, this operating angle will
coincide with vessel or rig offsets of three to four
percent of water depth.2.5 INSPECTION AND MAINTENANCE
Each riser component, especially riser joints, should
receive periodic inspection and maintenance. Visual
inspections shoúld be made each time the riser is run. Resilient seals should be inspected and replaced when
necessary. Each entire joint should be inspected,
particularly at the sealing areas. Damaged joints should
be sent ashore for additional inspection and repair.
Welds should, as is usual, receive particular attention
2.6 STATIC AND DYNMIIC ANALYSIS OF VERTICAL TENSIONED
MARINE RISERS
The approach here follows that adopted by Pateland Lyons
(1990). The reader is also referred to many of the
publications on this subject, including Gardner and Kotch
(1976), Sparks (1979), Patel et al (1984), Mclver and
Lunn (1983), McNaxnara et al (1986) and Wang (1983).
If the riser is simply considered as a beam column then
the governing differential equation used for internal
deflection is:
I
EI
d2x
J I- dy2 T(x) d2x dy2wdx
dy=
f
(1)where EI is the riser stiffness, T is the axial tension in the riser pipe wall, w is the weight per unit length of riser and contents and f is the lateral (viz normal)
force per unit length. The co-ordinate system used is
shown in Figure 2.4 with x measured from the bottom of
the riser and positive upwards while y denotes the
horizontal riser deflection from the vertical through the
riser bore.
In order to take account of the effects of internal and
external pressure in the governing equation for static
deflection, reference will be made to the static forces
acting on a pipe element in Figure 2.5 (from Patel and
Lyons (1990)). For simplicity the analysis is restricted
to two dimensions.
The static forces acting on the element (Figure 2.5) are
as follows)
An axial tension and shear force within the pipe
wall material.
A horizontal force due to the resultant of external
and internal hydrostatic pressures,
called (F +
F.)
xoA vertical force due to the resultant of external
and internal hydrostatic pressure (Fr0 + F,, )
A drag force due to sjeady current. The velocity
vector is resolved into components normal and
d2 uy
tangential tò the elenent.,
wIth only the normal
component assumed to exert a distributed force of N
per unit length.
5. The zeiqht of the. element ( acting vertically.
downwards.
Summing up the components Of forçe in the y direction
for the elemêht in Figure 2.5 yields the
equation:-(T + (IT) sin (O ±dO)
- T sin O - (V + dV) CQS (O + dO) + V cos
O+(F +F:)-W
NcosOrdO =0
yo y' R
similarly for the x direction we get
(T + dT) cos (O + dO) - T cos
O + (V ± dV) sin (O + dO)
-V sin O
+ (F+ F.)
+ N sin O r dO
= O
ese equations can be simplified (for small dO) and cömbined to
give:-TdO - dV + (F .± F
W) cos O
yi yo R
= (Ç +
F.) sin O
N r do. = 0
(4)The analysis now continues With
establishing expressions for the terms
(F ,
F ,
F , F )The derivation
for this is given in Patel andxo xl yo - yl - -- -- -
-Lyons (1990). When expressions
these terms are substituted into
Equation4,weget
-T ± p A
p. A] dû - dV + {
(cos. O - sin O dO): (Y A - y
A.)- y
A COS O - N: } rdû 0 (5)with WR= y A r dO where
is the weight per unit volume
of the pipe
Using the small deflection equation
dV d2
lEI
dy
dy2 I. dy2and assuming that the angles between pipe elements and the
vertical arealways small as well as
assuming that
all deflections are small (for avertical riser), the following expression can be obtained.
EI d2x dy2 dy 2 N
{l+1
J2}_L12 dx- (T+p A
-pA.).d2x
dy2-(y A
s s-y A +yA) dx
o o ii - =N
(7) dyFor a flexible
riser
the approximations leading to Equation 7 are not valid (small deflections, small angles with vertical etc) andthe
governing equation is consequently more complex.
This turns out to
be:-(T + p A
p. A.)
d2y { 1+
rsi
J2}'
o o dx dx2 +(y A
- y.
A.- y
A )
dVdx
= 0
(8)The term (T+ pA;
p. A.) is sometimes called the effective tension (T).
J
The complexity of the governing equation (even for static analysis of a vertically tensioned riser) means that in
practice solution techniques involve either a finite
element or finite difference approach Such approaches are commonplace and a number of purpose-designed computer
programs are available for the static and dynamic
analysis of both tensioned and flexible risers Examples
of such Software will be given during the SchOoL
he reader is referred to the literature for more
detailed information on dynamic analysis and the
influence of other effects on riser dynamic behaviour,
such as vortex shedding The latter effect is
particularly important in influencing the response of
2.7 MODEL TESTS OF TENSIONED RISERS
Model tests of tensioned marine risers have been
carried
out by a number of researchers. The purpose of these
model tests has been to confirm the results of numerIcal simulations and to identify features of dynamic behaviour
that would not appear to be adequately modelled in
numerical simulations A brief account will be given here of model tests carried out by members of the
Heriot-Watt University Marine Riser Group under G C Hartnup.
The majority of these tests were conducted as part of the
SERC/MTD Compliant Systems Programme over the period
1983-1985, although this group had been involved in model
testing riser systems prior to 1983.
One of the riser systems tested during this programme of research was the Buchan riser. This riser had been in
service for some time prior to the time that the model
tests were conducted. Furthermore, a certain amount of full size data was available Tests were carried out at
the BMT
Ltd No 3 Tank at Feithain, Middlesex, whichfacility has since been decomissioned.
Tests were carried out with the top of the rIser fixed in position, and with simulated vessel motion. The water
depth simulated was 116m. Tests were car:ied out in
conditions representing both regular and random waves,
both with and without current, current being represented
by carriage motion in the towing tank.
Tests were carried out at a scale of 1/14.5.
Figure 2.6 Shows details of the model Buchan riser. The
central riser was strain-gauged along its length, as was one of the satellite risers. The motions of the riser
were measured by a purpose-designed TV monitoring system, developed by G C Hartnup. One important aspect was the feature of attempting to model as accurately as possible
during the tests the tensioner system. It was found
during, the tests that comparison with predicted bending movements along the central portion of the riser were not
satisfaCtory. It was concluded that this was probably
due to the fact that the tensioner system js not normally
'modelled' in computer simulations.
Typical results obtaixed f rotn the model tests are given
in Figure 2 7 which shows the amplitudes of in-line
bending movements, in-line displacements and transverse displacements for a wave only situation corresponding to
a regular wave of height 442m (full scale) an4 period
i! I
Figure 2.1
24" Riser System with Diverter for Drilling Hole for 20" Casing
-DERR)C( FLOOR BELL NIPPLE FLOW LINE
BAG TYPE PREVENTER
HYDROLIC VALVE OPERATOR
BLEED-OFF LINE
VALVE
HEAVE COMPENSATOR LINZ
INNER BARREL OF TELCOPING JOINT
-SEA LEVEL
OUTER BARREL OF TELESCOPING JOINT
-RISER COUPLING
FLEXI8LE JOINT
-.
GUIOE FRAME-HYDRAULIC LATCHPERMANENT GUIDE BASE TEMPORARY GUIDE BASE
50 70
From Sheffield (1990)
TENSIOÑ REOUI RED TO
DISENGAGE
BALI. JOINT MEAÑ MAXIMUM TENSION TENSION
F
--J--I
O
-
---::- r
110' 130 - 150 170 APPLIED TENSION - KIFS -
-;Figure2.3
Typical ciirve ofstress vs applied tension of risers -nonoperationa.l mode
O MAXIMUM RISERSTRESS 3-=-- MINIMUM RISERSTRESS
BALL IN1STREES
RISER DIA. -16 IN. WATER DEPTH 500 FT WAVE HEIGHT. 20 PT- -
-AVERAGE CURRENT, 0.33 KNOTS MUD WEIGHT. 10 PPG VESSEL OFFSET-10% o 190 .4
'r
y
Figtre
.4The conventional vertical riser coordinate system notation, with x measured from the bottom of the riser.
From Patel and Lyons (1990)
y
o
XFigure 2.5
Riser element describing the static behavidur of a marine riser of arbitary geometry
¡ , TENSION WIRES EXPORT RISER SATELLITE RISER
289m
S1R41H 6AUGE PUSIT1OIIS ON52mm
1R0T SMUUTERISER. (BU CHAN RISE'
only) 5 10 11 13. TS0 :u
Figure 2.6 Test Point Positions on Risers
¿ 2SaJJ 9t 'd
EXPORT RISER TEST PO!ITS..SPIDER HEIGI{FS LED POSITIONS STRAIII 6AtJG.
(from base of riser) POSITIONS
BOSlrnm 7701mm 7701mm
- - 7670mm
7202mm 6675mm 6576mm69 mm
6151mm 5525mm 5100mm 5100mm SOC9riim 1457(4mm 14O14Bmm35mm
3523mm 3L92n'm 2966mm 2199mm 2129mm 216rnrn 1673mm 1023mm 1023mm 873mrr;(114th spider on HHL RISER o[y
Omm.
\\\\\\\\\\\ \\\\\SEABEO
lOSimm x 10mm 0/0
LR6ER O[t1ETER STUB (on LUCHAN RISER only)
.ot ¿N nzf (lacvj sa. 'a. su lea I.I4T IN PT (MC% W.1 sia 'e. aie tú
-Figure 2.7 Envelopes for 14.5 waves of 7.62 secs
-I5 -Ii -S i Ì ¿N-t.fl f9OJC rOI4T1 (XI? flZT) IS -13 -t. IS 1»4Ddt iCU 14t3 (XX? P!!?)
i.
3 -4 a ¿ I ts iaa4vV5L DI$JiJ2fI4TS -IS -i -4 i ¿ a 12 -17 ai -21 -IS i 12 21 -IS i Í2 24 LLJ4NTS IN-4.114 D;Lvr3(I1
WC31-
Nl. JIZZfl /.IY(.D44l1D4TIII FiAT IAJ5 5SA5Z) sa.
3.. FLEXIBLE RISERS
3.1 Description of Sytems and ComponentS
A nnnber of factors will Influence the design of a
flexible riser system These factors affect the
requirements relating to the integrity of the riser and would consequently influence the detailed design of the 'structure' of the riser and the selection of the various materials involved in the
construction
of the riser.Predominant amongst the design önsjderations are:
- the ability of the riser tO withstand the range
of loads that it will be subjected to during
its working life (both
internally
and: externaly applied).
. that the riser cönfiquration i
appropriate to
its service conditions, . which will be
influenced by the location of the floating
surface facility (or 'rig') in relation to the
position of the subsea welihead or 'Christmas
Tree' as well as the water depth and the
environmental wave/current climaté prevailing
at the locätion of the facility.
the ability of the
internal
and externalcoatings to resist attack by corrosion and
deterioration This aspect is complex since in
addition to the natural fluids experienced in
oil production, many chemical additives may be
present in practice.
- the long-term integrity of the flexible riser.
In relation to this, aspects that need to be
considered are:
wear (particularly jn relation to unbonded
flexible pipe)
steel corrosion
deterioration and physical parameters (eg.
pressure and temperaturé) of fluids
fatigue characteristics öf steel and 'plastic
materials'
- effective reliable and cost-effective
manufacturing
= certification requirements
- specifiç client specifiçatipn requirements
Types of. Construction
There are generally two types of flexible pipes: the
bonded and the unbonded. The bonded type comprises
layers of fabriç, elastomers and steel "bonded" together using adhesives and chemical agents Elastomeric
materials are used mainly to embed steel components,
reducing steel to. Steel contact. . Vulcanisation is
applied to cure elastomers, complete steel embedrnent, and
ensure final bonding making a "homogeneous structure".
the unbonded type consists of several individual layers which remain separated allowing internal movement between
components. An. intermediate thermoplastic sheath and
lubricating medium may be used to reduce internal
friction and contact between steel layers. The structure remains unbonded and heterogeneous following manufacture.
Flexible pipes have been made principally by föur major
manufacturers, Coflexip of France, Dunlop of the UK,
Pag-o-Flex of Germany, and Furukawa of Japan Nowadays Coflexip have a
dominant share of the market so the
description that follows of the unbonded type of
construction refers exclusively to the types manufactured
by Cóf.lexip..
Coflexip Unbonded. Pipe
There are two basic designs of unbonded flexible risers manufactured by Coflexip; these are 'rough bore' and
'smooth bore' (see Moore (1989)).
Rough Bore Structures
The rough bore construçtion is used whenever there is a danger to the polymeric liner from permeating
gas, for instance, in multiphase oil and gas
production, gas export, gas lift, gas injection and
annulüs control. A typical construction is shown in
Figure. 3.1 and each layer has the following
functions:.
- the inner interlocked steèl carcass (or the
interlock tube), prevents the collapse of the
thermoplastic layer.
- the intermediate thermoplastic sheath, ensures
that the pipe remains leak proof during
service.
a spiralled steel layer of "zeta." wires,
sustains the radial loads generated by the
internal pressure.
- an additional intermediate thermoplastic layer,
serves as. anti-friction layer.
- double crosswound tensilé armours, provides
- an external thermoplastic sheath, protects the
metallic layers of the pipe against external
corrosion or abrasion and binds the underlying
armours.
Smooth Bore Structures
These are used in applications
which do not
involve gas diffusion through the
pressure-containing plastic layer. A typical structure
is shown in Figure 3.2. In essence it is
similar to that of the rough bore
structureexcept that the interlocked steel carcass is
omitted.
Dunlop Bonded Pipe
In contrast to the Coflexip pipe already described,
Dunlop pipe is a construction with all layers "bonded"
together by elastomeric material. Figure 3.3
illustrates structural components of the pipe. As can be
seen, the pipe construction comprises the following
elements:
- Stainless steel strip wound interlock tube
- Duralon elastomeriC liner
- Textile reinforced primary carcass - Duratite hydraulic transfer layer - 2 or 4 brass coated reinforced cables
- Textile reinforced secondary carcass - Nylon fabric reinforced cover
The functions of the layers are described in detail
below:
a: Stainless Steel Interlock tube
This liner, often referred to by the manufacture as the
steel carcass, the flex, or the interlock, provides the necessary hoop strength to resist point and distributed
loads, external pressure and radial forces caused by
tension in the reinforcement cables. The interlock tube
also helps prevent rupture of the elastoineric liner in
the event of rapid internal depressurisation.
Furthermore, the interlock acts as a building mandrel
during pipe fabrication.
b. Duralon elastomeric liner
This layer is resistant to sour crude, gas and chemicals
and provides a barrier preventing gases from permeating
STEEP S RISER (Fiqure 3.6)
This has been developed as a safe solution to the problem of over-crowding on the sea-floor for production systems
where the subsea equipment is located directly beneath
the floating facility.
T1e steep S system differs from the lazy S system in that
the flexible riser itself is used to anchor the
subsurface buoy, and the riser terminates at the riser
bore.
This type of riser has been operating in. the Far East and
in Brazil, and is now being adopted for systems in the
North Sea It was the design selected by Sun Oil for its
Balmoral development.
LAZY WAVE RISER (Figure 3.7)
The lazy wave riser is the result of applying the
distributed buoyancy concept to the lazy S configuration
The inidwater arch, dead weight and connecting tie are al].
eliminated. By determining the most appropriate
distribution of buoyancy modules for each individual
case, it is possible to gain precise control over the
loads exerted on the floating facility, and installation procedures are thereby simplified.
This geometry is best applied to production schemes
involving satellite wellS and/pr floating export systems.
STEEP WAVE RISIR (Figure 3.8)
The steep wave is a straightfòrward extension of the
classic 'steep s' configuration There is no midwater
arch, and the associated buoyancy tanks are replaced by smaller buoyancy modules strategically distributed along the flexible riser itself Installation techniques can be simplified because there is no large single element
These features make the steep wave system particularly
Manufacturing Inspection
As with all supplied products, the reliability of the manufactured article is critically dependant on the
quality of inspection that would occur during and
immediately following manufacture considerable efforts have been devoted to inspection during the manufacturing process to ensure that the as-delivered product meets the
c. Intermedi ate, textile reinforced layers
These layers are spirally applied after extrusion of the Duralon liner Their principal functions are to act as hydraulic transfer layers and to bond the pipe wall into
a homogeneous Strudture during vulcanisation.
d1 Reinforcement cable laye
These are the man internal pressure ôontaining elements
within the pipe construction They are spirally applied
to the pipe in paired, balanced layers to ensure
efficient load sharing.
é. Duratite hydraulic transfer layers
The hlburatite'! iS a specially developed rubber compound
applied between the cable layers This compound
encapsulates and protects the cable wires and also acts
as a hydraulic transfer layer assisting in the load
sharing between dable layers.
f. Cover
The elastomeric cover provides prótection to the internal
layers of the pipe It should withstand long term
exposure to sea water and should also resist abrasion and
marine growth.
After the whole pipe has been formed of the above
structural layers, it is heat-and-chemical treated, ie
vulcanised, to consolidate and to bond the constituent
materials It should be noted here, that there is an
important structural element which is not bonded to the
elastomeric layers - the 'interlock tube' Fluid is
deliberately allowed to pass to the Duralon liner in
order to tränsf er pressure to the load bearing
3.2
RISER CONFIGURATIONSThêre are a variety of possible configurations for
flexible risers, the selection of which
depends on a
number of factors pertinent to the field location añd the specific application These factors will be discussed in this section Among a wide range of possibilities, themost frequently encountered configurations can be
classified-under five main types (see Qin (1987)).
FREE-HANGING RISER (Figure 3o4)
This is most suitable for temporary production or for
permanent field development in average weather
conditions As the simplest configuration, it requires a
minimum investment in equipment The flexible riser runs
in a catenary òonfiguration from the upper connection
point on the floater straight down to the sea-bed where it Öan be connected to any type of subsea equipment.
Möst early flexible risers were of the free hanging riser
type This kind of riser has seen service in various
parts of the World, notably in Indonesia, the
Mediterranean and Brazil, in water depths of 300m and
even deeper.
LAZY S RISER (Figure 3.5)
The lazy S riser is well adapted for all types öf field development and is particularly recommended for the most
severe environments. This system s used to best
advantage in production schemes involving satellite
wells, or whenever the subsea equipment is located at
son distance fröm the floater.
The syctem comprises a flexible pipe
running
down fromthe upper connection on the floater via a subsurface buoy
and inldwater arch, in a double catenary. The first
catenary, suspended between the floater and the buoy,
absorbs most of the motion induced by current and waves, and the second catenary runs directly from the inidwater
arch to the sea bottoni for connection to the subsea
equipment. The subsurface buoy is tensioned by means of
achain and dead weight.
The lazy S system is usually installed in diverless
operations from the laying vessel. This type of riser is currently operating with success in the Mediterranean and
STEEP S RISER (Figure 3.6)
-This has been developed asa safe solution to the problem of over-crowding on the sea-floor for production systems
where the subsea equipment is located directly beneath
the floating facility.
The steep S System differS fröm the lazy S system in that
the flexible riser itself is used to anchor the
subsurface buoy, and the riser terminates at the riser
bore.
ThiS type of riser has been operating in the Far East and
in Brazil, and is now being adopte4 for Systems in the
North Sea It was thé design selected by Sun Oil for its
Baimöral development.
LAZY WAVE RISER (Figure 3.7)
The lazy wave riser is the result of applying the
distributed buoyancy concept to the lazy S configuration. The midwater arch, dead weight and connecting tie are all
eliminated By determining the most appropriate
distribution of buoyancy modules for each individual
case, it is possible to gain precise control over the
loads exerted on the floating facility, and installation
procedures are thereby simplified.
This geometry is best applied to production schemes
invoiving satellite wells and/or floating export systems.
STEEP WAVE RISER (Figure 3.8)
The steep wave iS
a straightforward extension of theclassic 'steep s' configuration There is no midwater
arch, and the associated buoyancy tanks are replaced by smaller buoyancy modules strategically distributed along the flexible riser itself Installation techniques can
be simplified because there is no large single element
These features make the steep wave system particularly
3.3 DESIGN CONSIDERATIONS FOR FLEXIBLE MARINE RISERS
The design of a. flexible marine riser system will reqiire cònsideration of a number of factors in relation to its
-- functional suitability, and its
long term integrity
In addition, aspects related to its ease of manufacture and the cost of the product will need to be assessed.
The "functional suitability" of the flexible riser system
relates to the need to ensure that the. system in its
entirety (from its interface at the sea-béd connection
an4 its interface near the surface vessel) will retain
structural integrity from internal and external loadings
that it will be subjected tb during operation In
practice,
the motions of the upper end point
(at thevessel) and the as-laid configuration of the system will
greatly influence the magnitudes of local loads in
tension (or compression), bending and torsion. The
resulting stresses in the plastic and metallic materials
will be influenced by the precise structure of the
f lexible riser as a component, and whether or not the
component is of the 'unbonded' or 'bonded' variety. In
view of the complexities of the component design, the
prediction of the mechanic1 èrformance of a particular
riser component is extremely difficult, and great
reliance will need to be placed on the results of
component tests in which segments of the riser are
súbject tO loadings characteristics of those that would be encountered in actual service conditions.
The nature of the transported fluid will also have a
bearing on the design of the riser system. Although the temperatures of the fluids would not be sufficiently highas to cause concern with respect to the metallic
materials, the temperature restrictions of the plastic
materials provide a basic design criterion which must be closely adhered to, especially regarding the long-term
plastic age.ing effect at high temperatures.
Dynamic effects will need to be taken into consideration,
both in relation to dynamic local loads resulting from
the qlobal dynamic response of the system, as well, as
locally occurring effects such as the influence of
impulse loads caused by the occurrence. of slugs in the
fluid flow.
The assessment of the 'long-term' integrity of the riser
will need to take account of the fatigue performance of
the metallic reinforcement. In this context, the.
estimation of the magnitude and number of stress dycles
in the steel at critical locations will be a crucial
element of the design process. Other areas of concernthat would need to be addressed are the wear of the steel
(particularly in the case of unbonded types of
construction), and the corrosion of steel. Whereas f or
steels, the assessment of 'long-term' integrity is
relatively straight forward and well understood, this is
not the situation for the plastic materials. This
assessment would involve a comprehensive understanding of the behaviour of the plastic materials. This would
include an assessment of the long term deterioration of the plastic components under the service conditions, and this will be influenced by the loading (both internally
and externally applied), the nature of the transported
fluid and its temperature and pressure, its resistance to
gas permeation, blistering, ageing etc.
OTHER COMPONENTS
Apart from the basic pipe structures there is, of course, a considerable amount of ancillary equipment used in a
flexible riser system. The short term integrity and ong
term integrity assessment of the systems must evidently include attention tö these items as, in many instances, these could turn out to be critical arêas from the design
point of view.
The 'end fittings' provide the important function of
ensuring that the riser loads (in bending, torsion and
tension) are satisfactorily resisted whilst ensuring that a comprehensive sealing system is achieved both radially
and axially. A detailed discussion of the design
requirements for terminations is given by MacFarlane
(1989). Each manufacturer has tackled the problems
associated with fittings in Specific ways. The adequacy
of terminátions must be determined through careful
detailed design, prototype as well as through in-service experience.
In addition tO 'end-fittings', another important
ancillary component in flexible riser systems is the
'bending stiffener'. This is located normally at the
bottom and top connections. The purpose of the
'stiffener' is to provide additional resistance to
overbending of the riser at critical points (such as the
ends of the riser).
As has already been described, buoyancy is normally
required in a riser system either in the form of Subsea arches (subsea buoyancy unit) or discrète buoyancy units to provide distributed buoyancy over certain sections of the system. These buoyancy sub-systems require careful design and the material for their construction needs to be selected appropriately so as to ensure that they have a long-term resistance to water ingress. Most commonly,
syntactic foam is used which is coated with polyurethane
3.4 INSTALLATiON AND INSPECTION
Section 3.2 has described, the rangé Of riser
configurations that can be adapted in practice
Eventually each donfiguratiön requires its Own
installation procedure, although therè are many featùres common to each procedure. By way of illustratiòn we will concentrate on the installation procedure for the riser system in a lazy-S configuration (see Figure 3 9) The
account here follows that given by Johnston (1989).
Johnston describes the procedure as involving the following sequence of operations
Pre-installation survey
Install RSD (Riser Stability Device)
Attach RRC (Riser Release Connector) to riser Establish pull-in wire
Deploy riser
uli-in RRC to FPF (Floating Production Facility) Connect RR
Lay öut upper catenary Deploy gravity base Attach arch
Figure 3.9 (stage 1) shows the operation of pulling in
the RRC (viz connecting the two halves of the RRC)-. This
task is a common requirement for all riser systems
installation. The lower half of the RRC is first
attached to the riser upper flange on the installation
vessel. The pull-in wire is etablished between the
FPF-based pull-in winch and the lower half of the RRC. The
riser upper flange with the RRC attached is overboarded
from the installation vessel using the vessel crane By
paying out on the riser installation reel and taking up
on the FPF-based pull-in winch, the lower RRC is transferred until the riser is hanging vertically from
the FPF
The RRC lower half and the riser are then
pulled up and mated with the RRC upper half, which is
fixed to the FPF. Once the RRC halves are mated, the
hydraulic clamp within the RRC is operated to lock them
together.
Service. Inspection
As with all offshore equipment and systems, the role of
in-service inspection is particularly important in relation to identifying those areas that have failed or
are likely to fail in the near future. Gross failure (as noted by MacFarlane (1989)) should be signalled weil in
advance by defOrmation of the metal components and
inspection should concentrate on this. As a consequence
of this routine inspection should aim to identify major displacement and deformations in the riser rather than
hope to achieve an indication
that a small break or
3.5 DYNAMIC ANALYSIS OF FLEXIBLE NARINE RISERS
In determining the dynamic behaviour, òne usually starts
with the initial configuration of the systems derived
from a static analysis. The dynamic analysis takes into account the time-varying effects of waves, vessel motion,
the inertia of the system and relative velocities, and
yields the time histories of the responses, for example,
histories of tension and bend radii or curvatures
However, due to the compliant nature of the system, the complexity of the nonlinear hydrodynamiC load conditions and motion phenomena, and the nonlinear properties of the
pipe itself, the problem of determining the static and
dynamic behaviour of a flexible riser turns out to be a very difficu,t and còmplicated 9ne..
The reader is here referred to publications by a number
of authors
on the
subject of dynamic analysis. Inparticular, reference should be made to Qin (1987) and
Owen and Qin (1986) Patel and Seyed (1989) consider the
problem of identifying the dynamic excitation forces and
resonant motiOns arising from Slug f lOw through the
riser A wide range of computer software exists for
analysis the dynamic behaviour of flexible marine risers
and these can be used by designers of such systems A
fairly comprehensive review of the current status of the development of dynamic analysis programs is given by
3.6 MECHANICAL BEHAVIOUR OF FLEXIBLE MARINE RISERS
This refers to the examination of the response
of the
riser as a whole and its individual structural
components
to various applied loads
The published literature in
this area is much more limited than
that available in the
area
of
global
dynamic
responSe.
Individual
manufacturers
have
presented
siiiplified
methods
for
analyzing component response for their specifiC
products,
The
complexity
of
the
composite
construction
of
a
flexible riser component means that it
is not readily
amenable to analytical treatment.
Computer models of
component mechanical behaviour would need to be supported
by
experimental
results
from
prototype
tests.
Unfortunately,
the amount of
published infOrmation in
this context is sadly very limited.
The reader is here
referred
to
Chen(1990),
whose
thesis
concerns
the
mechanical behaviour of a bonded flexible
pipe, typical
of that used for offshore applications.
Two general approaches can be identified
for the study of
the mechanical behaviour of flexible pipes of
composite
construction, these are:
Simplified or analytical approach employing existing
cable theory and the theory of the
mechanics of
composite materials, and
Finite element modelling
With regard to the second approach
(b),
there are
a
number of difficulties to be addressed
For example, the
effect of
large deformations,
incompressibility of the
elastomer layers, and the material heterogenity as
well
as non-linerarity,
all present problems
for utilizing
general purpose finite element packages.
It would be difficult, if not
mpossib1e, to establish a
general model capable of dealing with all types of pipes
Special
treatment
is. required
to simulate
particular
features of different
pipes, such as the 'smooth bore' of"Coflexip" pipe, the interlock tube of the "Dunlop" pipe
and the corrugated steel liner of "Pag-o-Flex" pipe.
The
key to success
is toobtain a comprehensive understanding
of the mechanisms involved in progressive deformation and
ultimate failure, the ways in which the several metallic
and non-metallic layers interact and a sound knowledge of
the material behaviour for each component involved in the
3.7 EXPERIMENTAL. STUDIES
Experimental work provides valuable information f Or
validating computer simulatjons and assists the design of
prototype systems. Suôh validation of computer
Simulations is required both for global dynamic response
as well as in simulations developed to determine the
mechanical response characteristics of the riser. In
bth these situations there are a number of difficulties
in developing a reliable analytical model and numerOus
assumptions have invariably to be made.
Ïn the case of validating the computer simulations for
global dynamic response of flexible riser systems, one
can use both full-scale offshore field tests and model
tests. Full scale tests f flexible risers are of great
interest in the determination of their loadings and
motions under realistic Sea environments. Such an
investigation was conducted by O'Brien et al (1984). The
purpose of this particular project was to verify the
behaviour, of a flexible pipe from seabed to a Surface
buoy in a water depth of 106m under severe weather
conditions typical of the North Sea area. The system
consisted of a 135m long 10 inch inner diameter 4500 psi
flexible pipe, filled with water under pressure and
suspended between a surfaçe buoy and a subsea floater
submerged in a catenary form. The data obtained from
this investigation enabled the effective lifetime of a
flexible pipe to be estimated. Data was also available to correlate with results frOm computer programmes that
predicted the overall system response. However, full
scale tests are very limited, largely because of the
costs involved in carrying them out. Also, full scale
tests have no control over the environmental conditions
and the other test conditions.
Model tests, on the other hand, can be an effective way
of investigating the dynamic responses of flexible
risers, thereby validating various mathematical models.
One of the major difficulties in model testing: flexible
riser Systems
is the problem of scaling. Ideally,hydroelastic modelling, with proper scaling of elastic,
dynamic and hydrodynainic factors, is required. Such
scaling is, of course, never achievable in practice and
one has to concentrate on providing correct. dimensional
similitude for those non-dimensionless groups that have
the greatest bearing' in influencing system dynamic
response.
Qin (1987) provides extensive details of model tests that
were carried out at Heriot'-Watt University, Edinburgh,
United Kingdom, and the techniques involved in these
tests and some of the more important test results will be
As already mentioned, there are considerable difficulties
involved in predicting the mechanical behaviour of a
flexible pipe. This problem is particularly acute in relation to the determination of the bending stiffness of
a pipe. Furthermore, in view of the need to establish
service lives for flexible pipes
and the problem of
estimating these theoretically for such a complex
component as a flexible pipe,
one has to make use of
prototype tests of specimens that are subjected to
realistic loading conditions over a large number of load
cycles.
A good
review of the methods involved incomponent prototype testing is given by Cocks (1989), for the Dunlop bonded type of construction of flexible pipe. Each manufacturer, of course, needs to develop their own
specific types of tests to suit the needs of their
particular product. In general such prototype tests
would include the
following:-- hydrostatic burst tests - tensile tests
- hydrostatic collapse tests - bending stiffness tests
- in-plane and rotational fatigue tests
- multi-load dynamic tests
3.8 FUTURE PROSPECTS
The preceeding sectIons have aIady illustrated the many challenges that still remain in relation to the future application and utilization of flexible riser systems by the offshore oil and gas industry The concept of the flexible pipe has now 'come of age', despite theear1y
reluctance of some operators to adopt such a product
The advantages of. using flexible risers very definitely. outweigh its disadvantages The generally high cost of producing flexible pipe will clearly reduce as improved methods of manufacture are introduced There is still a need to obtain more information from prototype testing of
specimen lengths Unfortunately, much of this
information is not available to the purchaser and the
designer needs to lean heavily on the assurances given by
the product manufacturer on matters such as long term
reliability Operators are now requiring much longer
'life times' for the products supplied to them, and the attention on product safety js intensifying. There are
still considerable discrepancies between the predictions
of mechanical performance and those observed during
prötotype testiñg. In reality, there are probably
problems with both approaches. Further work is needed to
brïdge the gap.
Ïn relation to the area of materials, there is a
continuing need to research the suitability of individual materials for particular applications As has been seen,
each application has to be addressed on its own
particular merits and materials have to be selected
appropriately. One of the challenges today is to provide
hïgh temperature plastics at reasonable cost. Future
development of materials will probably be driven by
deepwater developments. With depths up to 100m being considered for future offshore developments, riser weight will be one of the crucial factors in future designs.
, TYPICAL" ROUGH BORE" DYNAMIC
AIsÈks-riifcrcí-EXTERNAL ThERMOPLASTiC
DOUBLE CROSSWOUNDTENSILE ARMORS -. '-.
t
ZETA SPIRAL4 INMEDIAT ., LThERMCPLAST1C j . CARPRODUCTION: CRUQEJGAS INJECTION: GAS EXPORTGAS... TEST,KJU. ...
HTT.
Figure 3.1
Rough bore Coflexip pipe construction
Figure' .2
A Stainless steel strip wound interlock tube
B Duralon elastomeric liner
C Textile anti-extrusion layer
D puratite hydrailic transfer layer
High tensile steel strand retnforcement
F Textile anti chaffing layer
G Nylon fabric ±eihfdrced cover
Figure 33
Dunlop bond. pipe const-ruö:iOfl
Figure 3.4
Figure 3.
Free-hanging flexible riser
Lazy-S flexible riser
configuration
configuration
Figure 3.6
Figure 3.7
Lazy wave flexible riser
conf:igurat ion
Figure 3.8
Steep wave flexible riser
MSL
F.PF
..\\,/i\\V
3. Overboard riser lower end flange
Installation
vessel
MSL
Seabed
2. Deploy mid - water arch
FPF Winch wire Mooring line Gravity base ,RSD MSL 4. System as installed RRC Mid-woter arch F1eibTe Riser lower riser end flange - RSD Seabed \SV AV /'\ Figure 3.9
Installation sequence for lazy-S flexible riser system
(from Johnston (1989))
FPF
Installation
vessel
Pull -in
winch. PiilI -in Installation
wire vessel MSL FPF
/
SV/L
RRC/ upper RRC half lower half RSO Seabed I. Pull-in RRCREFERENCES
:-'
Z: ''Chen (1990) Chen z : "The Mechanical Behaviour and
Fatigue Analysis of Flexible Pipes", Doctoral Thesis,
Heriot-Watt University, June 1990.
Cocks (1989) Cocks P J : "Testing and structural
integrity of flexible pipes", Engineering Structures, Vol
11, No 4, October 1989.
Gardner and Kotch (1976) Gardner T W and Kotch M A :
"Dynamic Analysis of riser and caissons by the finite
element method", OTC 1976, Paper No OTC 2651 (1976).
Johnston (1989)
Johnston D R A
: "Installationaspects of flexible riser systems," Engineering
Structures, vol 11, No 4, October 1989.
Kodaissi et al (1990) Kodaissi E, Le Marchiand E and
Narzul p : "State of the art on the dynamical programs
for the flexible risers systems", 9th International
Offshore Mechanics and Arctic Engineering Symposium,
OMAE, 1990.
MacFarlane (1989) MacFarlane C : "Flexible riser
pipes: problems and unknowns", Engineering Structures,
Vol 11, No 4 October 1989.
Mclver and Lunn (1983) Mclver D B and Lunn T S
"Improvements to frequency domain riser programs", OTC
1983, Paper No OTC 4550, Houston, May 1983.
McNamarra et al (1986) McNamarra J F, O'Brien P J and
Giiroy S G : "Non-linear analysis of flexible risers
using hybrid finite elements", Proceedings of OMAE 1986,
Tokyo, Japan 1986.
Moore (1989) Moore F : "Materials for flexible riser
systems: problems and solutions", Engineering Structures,
vol 11, No 4, October 1989.
O'Brien et al (1984) O'Brien E G, Joubert P,
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large high pressure flexible pipe", Offshore Technology Conference, OTC 4379, Houston, Texas, May 1984.
Owen and Qin (1986) Owen D G and Qin K : "Model
tests arid analysis of flexible riser systems",
Prdceedins of the 1986 Offshore
Mechanics and Arctic Engineering Symposium, OMAE, Tokyo, Japan 1986.Palmer (1985) Palmer A C : "Flexible Risers", The
Way Forward for Floating Production Systems, IBC
.P::a11d Ly.ç.n. (1990) Patel .14 H aith Lyons. G J. :
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Technology Reference Book", Edited by Nina Morgan,
Butterworths, 1990. .
Patel et al (1984) Patel M H, Sarohia S and Ny K F
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Engineering Structures, 6, p00, 1984.
Patel and Seyed (1989) Patel M H and Seyed F B
"Internal flow-induced behaviour of flexible risers",
Engineering Structures, Vol 11, No 4, Öctober 1989.
Sheffield (1980) Sheffield R : "Floating Drilling :
Equipment and Its Use", Gulf Publishing Company, Houston
1980.
Sparks (1979) Sparks C P : "Mechanical behaviour of
marine risers mode of influence of principal parameters", Proceedings of the Winter Annual Meeting of ASME, 7, New
York, 2 - 7 December 1979,
Qin (1987) Qin J : "Dynamic Behaviour of Flexible
Marine Risers", Doctoral Thesis, Heriot-Watt University,
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