KNOWLEDGE HUB / OFFSHORE LIFTING

Dynamic Amplification Factor (DAF)

A peak load needs a reference.

DAF is the peak of a named load response divided by its matching static or quasi-static reference. State where it is measured, what it is compared with, and which lift phase it describes.

01 / READ THE RESPONSE

One trace. Three things to report.

The peak gives the DAF. The reference gives it meaning. Minimum tension needs its own check.

SCHEMATIC · NO CASE VALUESPeak, reference and minimum of a load responseA schematic load trace with three numbered markers. One marks the peak used for DAF. Two marks the matching quasi-static reference at a response ratio of one. Three marks the minimum tension, a separate check. The zero line is shown. This is explanatory artwork, not a modelled lift result.Load response / reference1.00123Start of stated intervalEnd of stated interval
The same response point and reference apply throughout. The trace explains the reporting method; its shape is not an engineering result.
1

Peak response

Divide the maximum response by the matching reference to obtain the DAF.

2

Reference load

Name the load channel and reference. Hook load and sling-group tension describe different locations.

3

Minimum tension

Report it separately. A peak ratio alone does not establish whether the line stayed taut.

State with every DAFResponse pointReference loadLift phaseAnalysis intervalEvidence basis
02 / CHOOSE THE ANALYSIS

Which analysis does your lift need?

Choose the lift phase you are assessing. You will get either a study route or, for one narrow taut-line case, an illustrative harmonic screen. No output here is lift engineering.

Lift-off or transfer between moving bodiesStudy route

No number from this screen.

Lift-off is governed by the relative motion of two bodies, the velocity at the moment of engagement, and contact — none of which a single-body harmonic model represents.

The analysis has to represent

  • relative motion of the two bodies, including phase
  • relative velocity at engagement
  • clearance, contact and load transfer off the supporting body
  • hoist speed and preload
What to prepare for a study
  • both vessels or the vessel and the fixed structure, with their motion basis
  • the lift-off sequence and hoist speed
  • object mass, centre of gravity and lift points
  • rigging arrangement and hoist-wire properties
Ask ND to scope this lift case →
Clear of deck and water — line continuously tautIllustrative screen

An illustrative harmonic screen is available for this phase.

It applies only while the load is clear of deck and water and the line stays taut throughout. It is not a design-basis DAF, a crane-capacity check, an allowable sea state, or equipment selection.

What you need to hand

  • Crane-tip vertical amplitude Atip (m) or acceleration atip (m/s²), and where it came from
  • The excitation period T — the imposed response period, not wave Tp
  • For the amplified result: a known Tn, or meff and Keff to derive it
  • A damping ratio ξ. There is no default — near resonance it largely sets the answer
  • Optional: static hook tension W0 (kN), to get forces rather than factors

Only have Hs and Tp? Sea state alone does not define crane-tip motion — vessel response, heading, loading condition and crane position are all needed. This screen will not guess it for you.

Open the illustrative taut-line harmonic screen

Illustrative only. Not lift engineering, and not a substitute for analysis.

Crane-tip vertical motion
Add hoist and load dynamics optional

Without this the screen reports only the rigid crane-tip term. With it, it adds the amplification the suspended system contributes near resonance.

I need a project-specific study scope instead →

Splash-zone entry or exitStudy route

No number from this screen.

Water entry is governed by buoyancy through the surface, added mass, drag and slamming, plus the wave kinematics at the object. Those forces are simply absent from this model.

The analysis has to represent

  • displaced volume against immersion depth
  • the buoyancy transition through the free surface
  • added mass and drag
  • slamming, and the wave kinematics at the object
  • lowering speed through the zone
What to prepare for a study
  • object geometry and the hydrodynamic basis for it
  • dry mass, centre of gravity and submerged weight
  • lowering speed and the intended crossing window
  • sea state and the vessel motion basis at the lifting point
Ask ND to scope this lift case →
Submerged lowering or landingStudy route

No number from this screen.

Submerged lowering and landing are governed by buoyancy, added mass, drag, wire dynamics and touchdown contact. Both the static reference and the effective inertia change as the object goes down.

The analysis has to represent

  • submerged weight and buoyancy
  • added mass and drag at depth
  • wire and rigging dynamics over the full payout
  • touchdown and contact at the seabed or structure
What to prepare for a study
  • water depth and the lowering profile
  • object geometry, mass and hydrodynamic data
  • wire payout, stiffness and rigging arrangement
  • landing target and its acceptance criteria
Ask ND to scope this lift case →
Pile run, shock or possible slackStudy route

No number from this screen.

A pile run or snap is a transient, tension-only event: the line goes slack and re-tensions. A steady-state linear model cannot represent it — it is precisely the case this model is invalid for.

The analysis has to represent

  • the run-out or lowering velocity
  • the engagement and re-tension condition
  • tension-only line behaviour through slack
  • the force–stroke behaviour of any shock absorber, including end stops
What to prepare for a study
  • pile or object mass and the run-out velocity
  • the hoist arrangement and its stiffness
  • the allowable peak load at the crane tip
  • the operation sequence around the event
Ask ND to scope this lift case →
Model boundaries — what this screen cannot calculate
  • Crane-tip motion from a sea state — that needs vessel response at the lifting point
  • Irregular-wave statistics, operation duration, or an Hs × Tp operating window
  • Water entry: buoyancy, added mass, drag and slamming
  • Lift-off, set-down, contact, and two independently moving bodies
  • Slack, re-tension and snap — these are transient and non-linear
  • Winch and control-system behaviour, compensator stroke and end stops
  • Distributed wire and crane modes — this is a single vertical mode
THE FULL TECHNICAL GUIDE

Mechanisms, calculations and project evidence.

Continue through the original explanation, or jump to the matched case studies.

What is Dynamic Amplification Factor?

The Dynamic Amplification Factor (DAF) is the peak value of a named load response divided by its matching static or quasi-static reference — for the same load channel, location, configuration and lift phase. A DAF of 1.30 means the peak total load is 30% above that stated reference; a DAF of 2.0 means it is twice the reference. A DAF of 1.0 means only that the reported peak equals the reference; it does not prove the lift saw no motion, no low minimum tension and no slack.

A DAF is incomplete unless it states the response point (crane tip, hook, sling group or payload), the reference load and the lift phase. Peak hook load over static hook load is not interchangeable with peak sling tension over a submerged reference — and DAF is a peak ratio, not a safety factor, a crane utilisation or an allowable sea state.

In offshore lifting, waves cause the crane tip to move up and down while the payload hangs below. This relative motion creates dynamic forces in the lifting system — tension spikes when the crane tip accelerates upward, and slack when it drops. The DAF captures how much worse these dynamic forces are compared to a calm-water lift.

What causes DAF in real crane lifts?

In real crane lifts, DAF is driven by relative motion through the whole load path. The crane tip, hook, wire, slings and payload do not move as one rigid body: relative acceleration changes tension, compliance stores and releases energy, hydrodynamic forces alter the effective load, and loss and recovery of tension creates a nonlinear snap event. A descending boom tip does not itself prove slack — slack occurs only when computed tension reaches zero.

Supply-vessel deck lift. A cargo container on a supply vessel follows the vessel heave and roll, while the crane tip follows the crane vessel or platform. If the hook is moving up as the deck or container is moving down, the sling can go from slack or low tension to fully loaded in a fraction of a second. This snap load can be much higher than the static container weight.

Splash-zone crossing. During a splash-zone crossing, buoyancy, drag, added mass and wave particle velocity change quickly as the payload passes through the free surface. The hook load can rise and fall rapidly, especially when the crane, wire and payload dynamics line up with the wave period.

Other common triggers include sudden lift-off from deck, landing impact, snagging, fast crane motion, emergency stops and resonance in the crane-wire-payload system.

Snap loads — slack and re-tensioning

The most violent DAF events are snap loads: the sling goes slack, then re-tensions suddenly. While the wire is slack the hook and payload move independently, and when it comes taut the velocity difference has to be absorbed by wire stretch almost instantly. For an idealised, undamped single-mode screen, payload of mass m (plus added mass mA if submerged) on a load path of combined tangent stiffness k, the velocity-driven tension increment above the quasi-static load is approximately

F snap equals v rel multiplied by the square root of k multiplied by the quantity m plus m sub A.

where vrel is the relative velocity at the moment the wire re-tensions. This is not the total peak snap tension: k is the combined tangent stiffness of the whole load path, the mass term is an equivalent participating mass, not automatically payload plus added mass, and once a line can lose tension, peak and minimum tensions belong to nonlinear, tension-only transient analysis. Within the screen the increment scales with the square root of stiffness, doubling k raises it by about 41% for the same velocity mismatch, but added compliance also increases travel and shifts the natural period, so it is not automatically safer: available stroke and end-stop loads must be checked. DNV-RP-N103 sets out when snap loads must be assessed and how the peak is calculated. Keeping the line under tension through the wave cycle prevents the slack-to-taut transition in the first place — a passive heave compensator can do this within its analysed motion and force–stroke envelope, but that envelope has to be demonstrated, not assumed.

Simulated hook load at deck lift-off: bare rigging snaps to 3.2 times static load with repeated slack windows; a preloaded shock absorber holds the load near 1.3 times static
Figure 1 — Snap load at deck lift-off, illustrative 1-DOF simulation: 20 t payload, 4 MN/m bare-system stiffness, a prescribed 1.5 m/s relative velocity at sling engagement, crane-tip motion 1.0 m at 7 s. Bare rigging (navy) sees a 3.2× spike with repeated slack–snap cycles; a preloaded gas-spring shock absorber with damping (red) takes the same lift-off at 1.28× static. The peaks belong to this model only — they are not typical values, product guarantees or a certified calculation.

How to reduce DAF

  • Shock absorbers for snap loads. A POLARIS crane shock absorber adds stroke and damping between the crane and payload. It absorbs the kinetic energy of a single shock event (deck lift-off, a snap load, an overload) before it becomes peak crane load, provided its force–stroke behaviour, available travel and end-stop loads suit the event. It needs time to reset afterwards, so for repeated slack–snap cycles in the wave zone, use heave compensation instead.
  • Passive heave compensation for splash-zone crossings. A passive heave compensator reduces relative motion between the crane hook and subsea payload. This keeps rigging tension smoother through the splash zone and reduces the dynamic amplification the crane sees — within the unit’s analysed load, frequency and stroke envelope.
  • Control the lift as well as the equipment. Lower crane speed, avoid resonant sea states, plan weather windows and use soft lift-off procedures. The equipment reduces DAF, but the operation still sets the starting conditions.

Product routing follows the governing mechanism — the scenario section below shows which. For crane-side demand, compare the crane load chart.

How to Calculate DAF

A first screening estimate for a dry lift, clear of deck and water on a continuously taut line, with the payload following a prescribed sinusoidal crane-tip motion, is

DAF=1+aheaveg

where aheave is the maximum vertical acceleration at the crane tip and g is gravitational acceleration (9.81 m/s²). For sinusoidal crane-tip motion with single amplitude ζ (the vertical motion at the lifting point, not Hs) and response period T, which is not automatically the wave-spectrum peak period Tp:

aheave=ζ×(2πT)2

For example, with a 1.5 m heave amplitude and an 8 s period:

aheave=1.5×(2π8)2=0.93m/s²DAF=1+0.939.81=1.09

This is the rigid crane-tip screen only. The coupled hook response can be higher near a system natural period or lower in the isolation region — it depends on the frequency ratio, damping, stiffness, line length, payload mass and hydrodynamics. Legacy DNV-OS-H205 lifting provisions were consolidated into DNV-ST-N001; the project-nominated edition and its factors govern.

Schematic response-ratio trace over a normalised analysis interval: quasi-static reference at 1.0, an oscillating response, the peak marked with an open diamond as DAF equals maximum response over the reference, and the minimum marked with a note that near-zero minima mean slack risk
Figure 2 — How a DAF is extracted from a response: the peak of the stated load channel divided by its quasi-static reference over the stated analysis interval. The trace is schematic, not a design result. In-air design values must also respect DNV-ST-N001’s weight-banded Table 16-1 minimums (offshore: 1.25 stepping down to 1.10 as hook load grows); subsea lifts have no flat minimum — their DAF is calculated per Section 16.17 with RP-N103 methods, where a compensator directly lowers the result.

More accurate DAF calculations model the vessel, crane, hoist wire, rigging and payload hydrodynamics as one coupled system. Commercial time-domain tools such as OrcaFlex — and ND’s own CONSTELLATION) are used for this; for the water-entry physics, see the splash-zone crossing guide.

Why there is no transferable DAF range

A standard minimum factor, a project-calculated response and a result from one simulation are different kinds of number. Every value needs its load channel, reference load, lift phase and evidence basis.

Dynamic amplification factor by lift scenario — uncompensated, with stated mitigation, and the evidence basis.
Lift scenarioUncompensatedWith stated mitigationBasis
General offshore liftNo universal rangeNo universal reductionPhase-specific analysis and the approved project basis
Subsea liftCalculatedMatched calculationContract-nominated DNV-ST-N001 basis using applicable RP-N103 methods; no flat value stated here
Snap / lift-off — illustrative case3.2× (Figure 1 case)1.28× (Figure 1 case, shock absorber)Single 1-DOF illustrative simulation — not an upper bound

Minimum tension is a separate acceptance check, not part of the DAF definition. Any preliminary no-slack or percentage threshold shown in an ND screen is an ND screening default unless the project basis identifies an applicable requirement and clause.

Which DNV document does what
  • DNV-ST-N001 — the marine-operation load cases, planning and the marine-warranty basis.
  • DNV-RP-N103 — modelling guidance and simplified formulations for marine-operation design loads.
  • DNV-RP-N202 — heave-compensator design parameters, performance and validation.
  • DNV-ST-0378 — lifting-appliance design and certification; it does not set the project DAF or approve a lift operation.

The contract- and MWS-nominated editions, project assumptions and acceptance criteria govern. Equipment certification and operation-specific lift approval are separate matters.

What a defensible before/after comparison contains
Use the same vessel response, environmental forcing, response point, static reference, lift phase, model options, seeds, duration and extreme statistic. Report DAF alongside minimum tension, stroke and end-stop response. The paired GRP and pile-run cases below show this reporting pattern; neither supplies a range for another lift.

What a commissioned study returns instead

Two separate commissioned CONSTELLATION cases, shown because they cover physics the screen above deliberately excludes. Each is a matched pair (the same lift run with and without ND equipment in the load path, from one set of inputs) and each carries its full engineering basis. They are not generated from your inputs, are not a validation of the screen, and are not transferable to another lift.

Sling-group tension against time for a 35 t GRP cover crossing the splash zone, with and without a RIGEL passive heave compensator on the same wave realisation. Without the compensator the tension repeatedly falls to zero and snaps to 1846 kN; with RIGEL it stays between 183 and 655 kN and never goes slack.
Splash zone · RIGEL. The same sea state and the same wave seed, with and without the compensator. Bare, the sling group goes slack ten times and snaps to 1,846 kN (payload DAF 5.38); with RIGEL it never goes slack and peaks at 655 kN (DAF 1.91). Read the full case study →
Engineering basis for this figure
Case
CONSTELLATION legacy-named preset rigel_grp_splash_55t, scenario package DS10-PKG-SZ, loaded with the declared 35 t payload and gas/oil ratio 1.4. The legacy filename does not describe the current payload mass. Both columns were produced back to back by docs/audits/rigel-splash-2026-07-26/paired_traces.py.
Version and date
CONSTELLATION v1.2.96, commit 45998bc. Run 3 August 2026.
Operation phase
Splash-zone crossing — lowering through the water surface. No lift-off phase and no landing phase are modelled.
DAF definition
Payload DAF = the maximum sling-group tension over the run divided by the payload's static weight in air, 35 t × 9.80665 m/s² = 343.2 kN. That denominator is the definition declared for this ND case. The peak is the maximum of the time series on the solver's own grid, not of the plotted samples.
Assessed load point
The four-leg sling group immediately above the payload. Not the hook and not the crane tip — those also carry the rigging and compensator weight, and give a different number.
Vessel motion and sea state
North Sea Giant: 25,397 t displacement, 161 × 30 m, draft 7.5 m, GMT 1.5 m, GML 80 m, radii of gyration 10.5 m and 38.2 m, heading 180° (stern seas; 0° is head seas in this model), six-degree-of-freedom response with the crane-tip RAO included. Irregular waves Hs 1.8 m, Tp 7.5 s, JONSWAP with the simulator's auto-derived peak-enhancement factor, 200 spectral components, water depth 30 m.
Duration, realisations, extreme statistic
120 s per run, eight wave realisations (seeds 1–8) per column. The chart plots realisation 6, which carries the governing peak line load and the governing DAF in both columns. The envelope below is the worst value of each metric across the eight — no single realisation produces all four worst numbers at once.
Payload, rigging and equipment
35 t GRP protective cover, 15.0 × 12.0 × 3.0 m, slam area 180 m², displaced volume 10.73 m³, released 5 m above the surface toward a 15 m target depth. Rigging: four-leg wire-rope sling group at 60°, 3.0 m legs, group stiffness 84,823 kN/m; upper sling 5.0 m at 22,619 kN/m. Crane: wire luffing, 75 t at 30 m radius, hoist stiffness 13,622 kN/m, hook 7.5 t, 20 mm wire on four falls, lowering 0.16 m/s. Compensator: RIGEL 75 t / 4.5 m stroke, passive with no EQ control, gas/oil ratio 1.4, gas datum 2,400 mm from retracted, orifice 35 % extend and 70 % retract, pre-tension 35 t.
Hydrodynamic basis
Water entry on the relative motion between payload and wave kinematics: buoyancy from the instantaneous submerged volume, slamming on the 180 m² water-plane area, drag at Cd 1.3, hydrodynamic added mass at Ca 2.2, and the Froude–Krylov term. These coefficients are declared case inputs and require project validation.
Is the pair like for like?
Yes. Both columns are the same preset on the same build, run over the same eight seeds in one session; only the compensator's presence in the load path differs. The plotted pair is realisation 6 on both sides, so the two traces see identical wave forcing.
Governing limit
For this ND pre-engineering screen, payload DAF ≤ 2.0 and snap-load ratio ≤ 0.90 are company acceptance defaults; DNV-RP-N103 informs the analysis method but is not cited here as the source of those limits. With RIGEL: DAF 1.15–1.91 (8 of 8 inside the ND default), snap ratio at or below 0.359 (8 of 8), zero slack-sling events, peak sling 655 kN = 89.0 % of the unit's own 735.75 kN SWL, stroke utilisation 59–77 %. Without: DAF 3.41–5.38, snap ratio 1.000, up to 11 slack-sling events. Approved project criteria supersede these defaults.
What this is not
Not a design-basis DAF for any other lift, not a crane-capacity check, and not an operating window. It is one commissioned case at one sea state, and it says nothing about the screen above it.
Provenance note
This replaces a figure published in July 2026 that stated a payload DAF of 1.10. That run used an earlier 55 t payload configuration at Hs 2.0 m with overrides not stated in its caption, was a single realisation on a build that ignored the wave seed, and does not reproduce on the current code. It was withdrawn rather than restated.
Hook load against time for a 1500 t pile run arrested at 5 metres per second, with and without a POLARIS shock absorber, from one set of inputs. Without the absorber the hook peaks at 37,664 kN and goes fully slack twice; with POLARIS it peaks at 23,627 kN and stays loaded.
Pile run · POLARIS. One set of inputs, run with and without the absorber. Without it the hook peaks at 37,664 kN (DAF 2.28) and the line goes fully slack and re-tensions twice; with POLARIS the peak is 23,627 kN (DAF 1.43) and the line stays loaded throughout. Read the full case study →
Engineering basis for this figure
Case
CONSTELLATION preset factory:polaris_pile_run, scenario package DS10-PKG-POL-PIR, single velocity point at 5.0 m/s, valve force set to 18,000 kN (preset default 17,658 kN).
Version and date
CONSTELLATION v1.2.96, commit 29267cc. Run 3 August 2026. The compensated column is the case locked on 7 July 2026 and reproduces on this build to within 0.05 % on DAF.
Operation phase
Pile run — the drop-and-arrest event during driving (ND-DS-10 §10). Dry, in air, clear of the splash zone.
DAF definition
DAF = the maximum hook tension over the 5 s window divided by the static suspended weight at the hook: hook 160 t + POLARIS body 17.10 t + rod 10.85 t + payload 1,500 t = 1,687.95 t, i.e. 16,553 kN. The peak is tracked on the 0.05 ms integration grid, not the 1 ms output grid — reading it off the output samples under-reports a sharp arrest. Below the absorber a second DAF is reported against the payload's own 14,710 kN: 1.31 with POLARIS, 2.41 without.
Assessed load point
The hook and crane connector, above the absorber. The rod force below the absorber is a separate channel and a different number.
Vessel motion and sea state
None, deliberately. A pile run is a sub-second shock event, so the host vessel is muted and no wave loading is applied — the case isolates the arrest. There is no Hs, Tp, spectrum or heading to quote, and this figure says nothing about behaviour in a seaway.
Duration, realisations, extreme statistic
5.0 s window, output every 1 ms, integrated at 0.05 ms. One deterministic run per column — no seeds and no ensemble, because there is no random forcing to average over. The quoted peak is the maximum of the time series, not a statistical extreme, and it is not comparable with an eight-seed envelope like the splash case beside it.
Payload, rigging and equipment
1,200 t pile plus a 300 t hammer, clamped, 1,500 t combined impact mass, run-out 5.0 m/s. Load path: crane 17,454.3 kN/m with 66.85 kN·s/m damping, hook 160 t, upper sling 49,762.8 kN/m, POLARIS body 17.10 t, rod 10.85 t, lower sling 46,652.7 kN/m, payload 1,500 t.
Initial velocity and absorber settings
5.0 m/s downward at t = 0 from full static engagement — the assembly has hung on the unit before the run, so the gas is already at operating pressure and both slings are taut at their static tensions. POLARIS 2,000 t / 6.0 m stroke, valve force 18,000 kN, gas precharge force 15,696 kN, gas fraction 0.40. The run uses 4.98 m of the 6.0 m stroke (83 %) and the annular oil chamber never empties (floor 6.2 %).
Is the pair like for like?
Yes, and it is checked rather than asserted. Both columns are generated from one parameter set; the script compares the two field by field and refuses to run unless the absorber flag is the only difference. Same masses, stiffnesses, damping, gravity, initial state and integration step. The counterfactual replaces the compensator with a rigid link and changes nothing else.
Governing limit
Crane SWL 24,517 kN (2,500 t). With POLARIS the hook peaks at 23,627 kN, 96.4 % of it. Without, it peaks at 37,664 kN — 154 % of crane SWL — and the line goes fully slack and re-tensions twice inside five seconds, which no peak-load figure on its own captures.
Independent verification
The compensated case was cross-checked against OrcaFlex 11.3e on 17 July 2026, with the compensator reduced to a measured force law: crane peak +0.23 %, crane DAF 1.4299 against 1.4266, peak stroke −0.4 %, chain-force RMS under 1 % across the arrest.
What this is not
Not transferable to another pile, hammer, crane or valve setting, and not a load chart. There is no winch or operator response in the model, so the uncompensated trace after the first arrest is a free ring-down of the same chain.
Provenance note
Until 3 August 2026 the "without" case could not be simulated: driving the gas volume to zero to emulate a locked cylinder sends the pressure term singular, so ND published an analytic DNV-RP-N103 snap instead, whose value depended on which stiffness path was argued to govern — 34,190 kN treating the crane as compliant, 44,759 kN treating it as rigid. A rigid-link arrest mode was added to the simulator so the counterfactual is now computed rather than estimated. It lands at 35,387 kN on the payload side, between the two estimates and 21 % below the crane-rigid figure ND published in July.
Need an operating window, not an illustrative factor? CONSTELLATION is commissioned engineering, not an unlocked version of this screen. ND agrees the vessel and crane response, the lifted object, rigging, operation sequence and acceptance limits, then models the operation across sea states to return the operating window, the governing limit, and what the compensator buys. Ask ND to scope this lift case →

DAF by lift scenario

Two examples illustrate different governing mechanisms — they do not divide every offshore lift into only two regimes. The controls differ because the load patterns differ.

Configuration illustration — a passive heave compensator crossing the splash zone
Splash-zone crossing

Crossing the water surface

At water entry, crane-tip response combines with changing buoyancy, drag, added mass and possible slam. Slack and re-tension are possible outcomes, not automatic load components. A correctly sized passive heave compensator helps maintain positive tension within its analysed force–stroke envelope; the water-entry slam itself stays a hydrodynamic (DNV-RP-N103) check.

Drivers: slam · varying buoyancy · crane-tip heave

Keep it low with — passive heave compensation
Configuration illustration — a pile run arrested by a crane shock absorber
Pile run & lowering

Running a pile or heavy structure

A pile run is a loss-of-support or run-out transient — steady lowering is not itself a snap load. The released mass, run velocity, line and tackle dynamics and the arrest system determine the peak: a sharp, short-duration spike rather than a wave-cycle heave.

Drivers: snap / shock load · lowering speed · rigging stiffness

Cap the peak with — a crane shock absorber

DAF — frequently asked

What is a typical DAF for an offshore lift?
There is no universal range. Define the response point, quasi-static reference, lift phase, forcing and extreme basis, then apply the contract-nominated standards edition and project criteria. A value from another lift is context, not a transferable design factor.
How do you calculate DAF?
Define the response and its matching quasi-static reference, then divide the peak total response by that reference for the stated lift phase and analysis interval. The crane-tip screen DAF=1+aheaveg applies only to a dry, continuously taut lift following prescribed crane-tip motion — it excludes rigging dynamics, added mass, drag, slamming and slack.
What is a snap load?
The short-duration re-tensioning load after a line has gone slack. It is a nonlinear transient — an ordinary harmonic DAF cannot represent it — and it can reach several times the static load in a pile-run or lift-off event.
How much does passive heave compensation reduce DAF?
There is no fixed percentage or transferable range. Quantify it with paired analyses of the same lift — same forcing, response point, reference, seeds, duration and extreme basis — with and without the unit, checking minimum tension, stroke and end stops alongside the peak.
Is DAF a safety factor?
No. DAF describes the amplification of a stated response. Safety, consequence and partial factors — and any dynamic allowance already embedded in the approved crane chart — are separate checks; do not double-count them.

DAF and Heave Compensator Selection

DAF is an output, not a sufficient product-sizing input. Equipment is selected from the governing lift phase and the quantities behind the factor: static, peak and minimum tensions, relative motion and velocity, required stroke, force–stroke behaviour, damping, cycle duty, recovery time and end-stop loads. A lower DAF does not by itself establish crane capacity, a weather window or an allowable Hs.

What a compensator buys on a specific lift, and which unit fits, comes out of a modelled case, not a rule of thumb. The scenario section above routes by mechanism; a commissioned CONSTELLATION study sizes the equipment against the stated operating limit and reports peak and minimum tensions alongside the factor.

Need a design-basis DAF?

Send the lift phase, load definition, vessel and crane motion basis, rigging and the operating limit. We'll come back with the required input list and a proposed analysis scope — no project factor is issued from a form. Prefer to inspect worked cases first? The benchmark figures below are the same models we quote from.

Free download · 8 pages

Offshore Lift Load Cases — ND benchmark figures

What a lift actually measures, with and without passive compensation, from Norwegian Dynamics' own time-domain simulations. It reproduces no standard — the value is the figures, which no standard publishes.

  • Peak sling load and amplification, with and without a compensator, on the same sea
  • The full configuration of every case, so you can set it up yourself
  • Where each result stops being valid, printed next to the result
  • An input checklist for scoping your own lift

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Related products

  • RIGEL — Passive heave compensator
  • CYGNUS — Passive heave compensator
  • ANTARES — Adaptive passive heave compensator

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