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Offshore structures: fixed platforms, floaters, moorings and risers

Naval Architecture and Ocean Engineering (B.Tech) · Ocean engineering · free study notes for exams, placements and interviews

In short

Offshore structures are the platforms, hulls, anchors and pipes that let an industry drill, produce and export hydrocarbons (and now wind power) in water from a few metres to over 2,000 m deep. They divide broadly into fixed structures, which transmit all loads to the seabed and stand rigid against waves, and floaters, which are buoyant hulls held in place by mooring systems and connected to the wells by risers. The engineering question is always the same - make the natural periods of the system fall outside the energetic wave band (roughly 4-20 s), then check strength, fatigue and stability. It is a core part of the Ocean Engineering / Offshore Structures papers in IIT Madras, IIT Kharagpur, IIT Bombay, AMET and IMU curricula and appears in GATE Naval Architecture and Marine Engineering (NM) under offshore structures and station-keeping. Employers include ONGC, Oil India, L&T Energy Hydrocarbon (Hazira, Kattupalli), Larsen & Toubro's offshore yards, Shapoorji Pallonji Offshore, Dolphin Offshore, Aker Solutions, SBM, Technip Energies India, DNV, ABS and IRS, plus NIOT and the offshore wind programme off Tamil Nadu and Gujarat.

Explained

Classification of offshore structures

Fixed structures

Floating production systems

Loads, analysis and design philosophy

Mooring systems and station keeping

Risers and subsea connections

Codes, standards and Indian regulation

Key points

Formulas and examples

Morison's equation (force per unit length on a vertical slender cylinder):
f = ½ ρ Cd D u|u| + ρ Cm (πD²/4) u̇
ρ = sea water density (about 1,025 kg/m³), Cd = drag coefficient (about 0.65-1.05 for a clean to rough cylinder), Cm = inertia coefficient (about 1.6-2.0), D = diameter including marine growth (m), u = water particle velocity (m/s), u̇ = acceleration (m/s²); f in N/m.
Keulegan-Carpenter number KC = um T / D ; diffraction parameter D/L
KC small → inertia dominates; KC large → drag dominates; D/L > 0.2 → use diffraction theory, not Morison.
Heave natural period of a floater: Tn = 2π √( (M + A33) / (ρ g Aw) )
M = mass (kg), A33 = heave added mass (kg), Aw = waterplane area (m²), g = 9.81 m/s².
TLP heave (tendon-dominated): Tn = 2π √( (M + A33) / (n EA / L) )
n = number of tendons, E = Young's modulus (Pa), A = tendon cross-section (m²), L = tendon length (m).
Mooring catenary (uniform line, horizontal seabed): h = (H/w)[cosh(w x/H) − 1] ; s = (H/w) sinh(w x/H)
Tension at a point: T = H + w h ; minimum suspended length for no uplift at anchor: s = √(h(h + 2H/w))
H = horizontal tension (N), w = submerged weight per unit length (N/m), h = vertical height from touchdown to fairlead (m), s = suspended line length (m).
Riser effective tension: Te = Tw − p_i A_i + p_o A_o ; apparent (submerged) weight wa = w_pipe + w_content − w_displaced
Te in N; p = internal/external pressure (Pa), A = internal/external area (m²).
VIV lock-in: f_s = St·U/D , reduced velocity Vr = U/(f_n D)
St (Strouhal number) about 0.2 for a circular cylinder; lock-in when Vr is roughly 5-7.
Fatigue: N = A·S−m (S-N curve) ; Miner's rule: Σ (n_i / N_i) ≤ 1/SF
S = stress range (MPa) after SCF, m = slope (3 or 5 in air/seawater DNV curves), SF = design fatigue factor (2-10).
Stability of a floater: GM = KB + BM − KG, BM = I_T / ∇ ; righting moment = Δ·GM·sin θ
Spar: CB above CG so BG is itself restoring; ∇ = displaced volume (m³), I_T = transverse waterplane inertia (m⁴).

Example 1 - Wave force on a jacket leg by Morison's equation. A vertical leg of outside diameter 1.2 m carries 50 mm of marine growth all round, so D = 1.2 + 2(0.05) = 1.3 m. At the still-water level the design wave gives u = 3.0 m/s and u̇ = 1.5 m/s². Take Cd = 1.05, Cm = 1.8, ρ = 1,025 kg/m³.

Example 2 - Heave natural period of a semi-submersible. Displacement 52,000 t (M = 5.2 × 10⁷ kg), heave added mass 60% of displacement (A33 = 3.12 × 10⁷ kg), four circular columns of 16 m diameter at the operating draught.

Example 3 - TLP tendon stiffness and heave period. A TLP in 900 m of water has 8 tendons, each of cross-sectional area 0.055 m², E = 2.07 × 10¹¹ Pa, length 900 m. Mass + heave added mass = 4.0 × 10⁷ kg.

Example 4 - Catenary mooring line check. A chain of submerged weight 2.0 kN/m runs from the seabed to a fairlead 1,200 m above the touchdown point (deep-water case), with horizontal tension H = 1,800 kN.

Example 5 - VIV lock-in speed for a riser. A production riser of 0.3 m outside diameter has a first-mode natural frequency of 0.20 Hz. Take St = 0.2.

FeatureJacket (fixed)Jack-upSemi-submersibleTLPSparFPSO
SupportPiles to seabedLegs on spudcansBuoyancy + catenary/taut mooringBuoyancy + vertical tendonsBuoyancy + taut mooringBuoyancy + turret/spread mooring
Typical depthUp to about 300-400 mUp to about 120-150 m300-3,000 m300-1,500 m300-3,000 m300-3,000 m
Heave motionNilNil (elevated)Small (long period)Nearly nilSmallSignificant
TreesDryDryWet (subsea)DryDry or wetWet (subsea)
Riser typeRigid verticalRigid verticalSCR / flexibleTTR, rigidTTR, SCRFlexible / SCR
StorageNoNoNoNoLimitedYes (large)
MobilityNoneSelf-elevating, movableMovablePermanentPermanentDisconnectable or permanent

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Related topics

Ocean waves and wave loads on structures · Coastal engineering basics · Ship hydrostatics and stability · Marine geotechnics and pile foundations · Subsea pipelines and flow assurance · Offshore wind energy structures

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