```html Cable Noise/Vibration Estimate (VIV) – 3/4" Duplex SS Cables

Estimate of noise/vibration from 3/4" (19 mm) duplex stainless cables moving through seawater

Important: Cable “singing” / vibration is dominated by vortex-induced vibration (VIV). The actual vibration and radiated noise depend strongly on: cable tension, span length, end restraints, any contact points/chafe gear, marine growth/roughness, proximity to leg wakes, and whether thruster wash impinges on the cable. The numbers below are order-of-magnitude engineering estimates for a smooth, bare, circular cable in open flow.

Assumptions used for the estimates

1) Expected vortex shedding frequencies vs speed (the “tone” that can drive vibration)

Speed (mph) Speed V (m/s) Re = V·D/ν Shedding freq. f (Hz)
(≈ 0.2·V/D)
What it tends to feel/sound like
0.5 0.224 ≈ 4,100 ≈ 2.35 Hz Very low-frequency “push-pull” loading; may feel like a slow rumble if it couples into the platform.
1.0 0.447 ≈ 8,100 ≈ 4.7 Hz Low-frequency vibration; more likely to become perceptible in structure if a cable/span resonance exists near this band.
1.5 0.671 ≈ 12,100 ≈ 7.1 Hz Noticeable excitation band for many cable spans; can become “busy” if multiple spans lock-in.
2.0 0.894 ≈ 16,200 ≈ 9.4 Hz Still low-frequency, but forcing is stronger (~V²). Highest likelihood of objectionable vibration if untreated.

Key point: the frequency content is mostly ~2–10 Hz for your 0.5–2 mph range. That is below “audible pitch” for most people, but it can be very effective at producing structure-borne vibration (rattles, creaks, thumps) and a low “rumble” sensation if it couples into the frame.

2) How strong is the forcing on a bare cable? (order-of-magnitude)

A rough estimate of cyclic lift force per unit length on a smooth circular cylinder in this Reynolds regime is: F' ≈ 0.5·ρ·V²·D·CL,rms, with CL,rms often on the order of 0.3–0.8 depending on conditions. Using 0.8 as a conservative “could happen” value:

Speed (mph) V (m/s) Estimated cyclic force per length F' (N/m) Same (lb/ft) Implication
0.5 0.224 ≈ 0.39 N/m ≈ 0.03 lb/ft Often small unless tension/span resonance is “just right.”
1.0 0.447 ≈ 1.55 N/m ≈ 0.11 lb/ft Can become noticeable on long spans with low damping.
1.5 0.671 ≈ 3.49 N/m ≈ 0.24 lb/ft Moderate forcing; VIV lock-in becomes a real concern.
2.0 0.894 ≈ 6.20 N/m ≈ 0.42 lb/ft Highest forcing in your set; untreated VIV is most likely to be objectionable here.

These forces scale with . So going from 1 mph to 2 mph increases VIV forcing by roughly 4×.

3) Is noise/vibration from the cables likely to be an issue?

4) Mitigation options (your list) and recommendation

Option VIV reduction (typical) Drag penalty Pros Cons / gotchas Fit for “waves & cross-currents”
1) Helical strakes Often 60–90% reduction in VIV amplitude / coherence High (commonly +50–100% drag on that member) Simple, passive, works regardless of flow direction; very common offshore Drag hurts your low-power propulsion; collects growth; bulky; can complicate handling/maintenance Good
2) Fixed “wing” snap-on fairing Can be 80–95% if perfectly aligned Low when aligned Best hydrodynamics when aligned; can reduce both VIV and drag If yaw/cross-flow occurs, can stall, lose effectiveness, and sometimes create its own unsteady loading Poor to fair (only if you truly maintain direction)
3) Freely rotating wing fairings Commonly 80–95%+ reduction over a wide range of directions Low (often less than bare cylinder when working correctly) Best overall for variable flow direction; widely used for offshore risers More complex; needs robust rotation hardware; fouling/jamming risk; design details matter Best
4) Other Varies Varies Can be very effective if you change the problem (materials/layout/damping) May require redesign Depends

Recommendation for your use case (low-speed propulsion + variable cross-flow):
Prefer (3) freely rotating wing fairings on the long, continuously submerged cable runs. If you want the simplest, most robust passive approach and can accept extra drag/power, then (1) helical strakes are the next-best choice.

5) Estimated residual noise/vibration with mitigation (relative, practical expectations)

Because absolute acoustic levels are highly installation-dependent, the table below gives expected relative outcomes (how “noticeable” it is likely to be) and a rough residual vibration amplitude in terms of cable diameter D, assuming the system is otherwise well-built (no loose fittings).

Speed (mph) Bare cable (no treatment) With helical strakes With rotating wing fairings
0.5 Low likelihood of objectionable VIV.
Typical cross-flow vibration (if it occurs): ~0.05–0.3 D.
Main content: ~2.35 Hz.
Usually minimal.
Residual: ~<0.05–0.1 D.
Usually negligible.
Residual: ~<0.05 D.
1.0 Moderate VIV risk on long spans; may be felt as low-frequency rumble if coupled.
Typical: ~0.1–0.6 D during lock-in.
Main content: ~4.7 Hz.
Generally low.
Residual: ~<0.05–0.15 D.
Generally very low.
Residual: ~<0.05–0.1 D.
1.5 Moderate to high chance of lock-in depending on tension and damping.
Typical: ~0.2–1.0 D possible in “worst practical” cases.
Main content: ~7.1 Hz.
Usually reduced to low to moderate (but drag penalty increases power needed).
Residual: ~<0.1–0.25 D.
Usually low.
Residual: ~<0.05–0.15 D.
2.0 High risk of objectionable vibration on long spans if untreated.
Typical: ~0.3–1.0 D (sometimes higher locally).
Main content: ~9.4 Hz.
Typically moderate or better (but highest drag/power cost here).
Residual: ~<0.1–0.3 D.
Typically low.
Residual: ~<0.05–0.2 D.

6) “Other solutions” that often matter more than people expect

7) Practical takeaway


If you can provide (a) approximate underwater span lengths for each cable run, (b) cable tension range, (c) whether any runs are in the wake of the 4-ft legs, and (d) how close the thrusters are to the cables, I can refine the estimate toward a “likely/not likely” VIV lock-in map and a better sense of how much vibration would reach the living platform.

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