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Estimated Cable Noise/Vibration vs Speed (3/4" Duplex SS in Seawater)
Estimate: Noise / Vibration From 3/4" Cables Moving Through Water at 0.5–1.5 mph
What this is: a first-order estimate of vortex-induced vibration (VIV) and likely noise characteristics for a taut,
circular cable in seawater.
What this is not: a substitute for a proper VIV analysis (needs actual cable lengths, tension, end constraints,
damping, current shear, wave orbital velocities, wake interference from your legs/columns, and structural transmission paths).
1) Key assumptions used for the estimates
- Cable diameter: 3/4 in =
D = 0.01905 m.
- Seawater kinematic viscosity:
ν ≈ 1.0×10^-6 m²/s (order-of-magnitude; temperature/salinity matter).
- Vortex shedding Strouhal number for a circular cylinder in this Reynolds-number range:
St ≈ 0.2.
- Vortex shedding frequency:
f_s ≈ St · U / D.
- Interpretation:
- Hydrodynamic forcing is primarily at
f_s (and harmonics / broadband components).
- Perceived “noise” onboard is usually structure-borne (vibration transmitted into legs/platform), not “audible sound in air” directly from the cable.
- At the speeds you listed,
f_s is in the infrasonic / very low frequency range (a few Hz). Humans won’t “hear” 2–7 Hz as a tone in air, but you may feel it as vibration, and it can excite higher structural modes that become audible.
2) Calculated Reynolds number and vortex shedding frequency
| Speed |
Speed U (m/s) |
Re = U·D/ν |
Shedding freq. fs ≈ 0.2·U/D (Hz) |
What it tends to feel/sound like |
| 0.5 mph |
0.2235 |
~4,300 |
~2.35 Hz |
Mostly low-frequency pulsing. Not an audible “whine,” but can be a slow rumble/rocking feel if it couples into the structure.
|
| 1.0 mph |
0.4470 |
~8,500 |
~4.69 Hz |
Stronger VIV risk than 0.5 mph. Still low-frequency, but more likely to drive a cable mode and transmit noticeable vibration.
|
| 1.5 mph |
0.6705 |
~12,800 |
~7.04 Hz |
Higher forcing frequency and load. Can be felt as a faster “thrumming”. If the cable locks-in to a mode, vibration can become clearly noticeable onboard.
|
3) Will it actually vibrate a lot? (Lock-in risk)
VIV becomes a problem when the shedding frequency f_s is near one of the cable’s natural frequencies
(f_n) and the system damping is low. For a taut cable/string, a rough fundamental estimate is:
f1 ≈ (1 / (2·L)) · sqrt(T / μ)
where L = span length, T = tension, and μ = effective mass per length (cable mass + added mass in water).
With spans on the order of 50–74 ft (15–23 m) and typical marine tensions (many kN), it is plausible for the
fundamental (or low-order) modes to land in the ~2–8 Hz range, which overlaps the f_s values above.
That overlap is where “lock-in” can occur and vibration amplitudes can grow.
Practical takeaway: at 0.5–1.5 mph, the vortex shedding frequencies line up with the “easy-to-excite” low modes
of long, taut cables. So the risk is not that you’ll hear a high-pitched singing noise; it’s that you may get
structure-borne low-frequency vibration (and potentially audible secondary effects if it excites other parts of the structure).
4) Relative magnitude of hydrodynamic forcing vs speed (why it ramps up quickly)
VIV forcing scales roughly with dynamic pressure ~ (1/2)ρU², so going from 0.5 mph to 1.5 mph increases
available excitation energy by about (1.5/0.5)² = 9× (very roughly), even before considering lock-in details.
So if vibration is “barely noticeable” at 0.5 mph, it can become “obvious” by 1.5 mph.
5) Mitigation options: strakes vs fairings vs other
Option 1 — Helical strakes
- Effectiveness: Often reduces VIV amplitude substantially (commonly cited ~50–90% reduction, highly case-dependent).
- Pros: Works regardless of flow direction (good if currents/waves reverse or yaw occurs).
- Cons: Significant added drag (can be 2× or more for some geometries), more marine growth surface area, can snag debris, harder to build/maintain on cables.
- When it’s a good fit: If your heading and/or local currents are variable and you need a “works in any direction” solution.
Option 2 — Wing-shaped fairing (fixed orientation, snap-on)
- Effectiveness: Can be excellent at suppressing VIV and reducing drag when properly aligned to the flow.
- Pros: Typically lower drag than strakes and strong VIV suppression.
- Cons / risk for your case:
- If the actual flow direction at the cable changes (yaw, maneuvering, cross-currents, eddies, wave orbital velocities), a non-rotating fixed fairing can stall, reducing effectiveness and possibly creating unsteady loads.
- Cables are not perfectly straight; local angle-of-attack can vary along the span.
- When it’s a good fit: If you can be confident the flow direction relative to the cable is consistent (or you design the fairing to tolerate some misalignment).
Option 3 — Other solutions (often used in moorings/risers)
- Increase damping / add dampers: External tuned dampers or inline “bending stiffeners” / clump weights can reduce response by adding damping and changing mode shapes.
- Change the “cable” type: Chain or jacketed/sheathed lines can disrupt coherent shedding (sometimes at the expense of drag/weight). Synthetic lines (e.g., HMPE) have different damping and stiffness, which can help or hurt depending on tensioning and layout.
- Break up the span: Intermediate supports/bridles that shorten effective free span length can shift natural frequencies away from the shedding band and reduce amplitude.
- Surface roughness / spiral wraps: A simple spiral rope wrap can sometimes reduce coherence of shedding (less effective than engineered strakes/fairings, but simpler and cheaper to test).
6) Recommendation for your specific speed range
Given your stated operating speeds (0.5–1.5 mph) and the likelihood that long taut cables will have natural
frequencies in the same few-Hz band as vortex shedding, I would treat VIV as a real design consideration.
-
If you truly move in a consistent direction relative to the cables (and local currents are usually aligned),
then Option 2: wing-shaped fairings are usually the best mix of VIV suppression and low drag.
-
If direction can change materially (cross-currents, drifting, yawing at anchor, waves), then a fixed fairing can underperform.
In that case, Option 1: helical strakes (or a fairing that can weathervane) is more robust, with the tradeoff of higher drag.
-
Best “engineering path”: plan a small-scale test section (or one full-length cable) with a removable mitigation
(spiral wrap → strake → fairing) and instrument it (accelerometer on the structure + tension measurement).
This quickly tells you if the issue is negligible or needs investment.
7) What I would need to tighten this estimate
- Cable lengths (each segment), approximate pretension, and whether cables are submerged, partially submerged, or near the surface.
- Whether the 3/4" cable is bare wire rope, solid rod, jacketed, etc. (surface strongly affects VIV).
- Expected current profile, wave climate (wave orbital velocities can dominate), and whether you’ll ever travel sideways relative to the cable plane.
- Connection details (hard pin, soft shackle, elastomer, etc.) and what structure the cable loads transmit into.
Summary in one line: At 0.5–1.5 mph a 3/4" cable sheds vortices around ~2–7 Hz, which is squarely in the range that can excite long taut cable modes; you’re more likely to get low-frequency structural vibration than audible “singing,” and fairings are typically best if flow direction is consistent, while strakes are more direction-agnostic but higher drag.
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