```html 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

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

Option 2 — Wing-shaped fairing (fixed orientation, snap-on)

Option 3 — Other solutions (often used in moorings/risers)

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.

7) What I would need to tighten this estimate


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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