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f ≈ St · V / D| 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.
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 V². So going from 1 mph to 2 mph increases VIV forcing by roughly 4×.
| 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.
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. |
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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