Great project — and a smart instinct to check how the thruster behaves *once the hull is moving*, because that's where most back-of-envelope propulsion plans go wrong. Here's the short version of what I found, followed by a complete HTML page you can drop into your site. **Headline results (best estimates, anchored to the Shinmaywa rating):** | MPH | Thrust | kW | |-----|--------|-----| | 0 | 3,200 N (720 lbf) | 3.20 | | 0.5 | ~2,720 N (610 lbf) | ~2.89 | | 1.0 | ~2,250 N (505 lbf) | ~2.58 | | 1.5 | ~1,770 N (400 lbf) | ~2.27 | Key physics: thrust falls roughly **linearly** with speed (blades see reduced angle of attack), hitting zero around **~3.4 mph**. Power draw falls much more slowly (blade profile drag keeps absorbing torque), so **don't size your solar array below ~3.2 kW per unit** if you want full thrust on demand. Against my estimate of your hull's drag (~21 m² effective drag area from the four angled columns + cables), one unit gives a calm-water top speed of **~1.0 mph**, two units **~1.3 mph**. All figures ±25–30% until you calibrate with a dockside bollard test. Here's the full HTML page: ```html Seastead Propulsion — Mixer Thrust & Power vs Speed

Seastead Propulsion Analysis

Shinmaywa-type submersible mixer (2.5 m propeller, 3,200 N / 720 lbf bollard thrust, 2–3.2 kW) repurposed as a low-speed thruster — estimated thrust and electrical power draw vs vessel speed.

Bottom line: Thrust falls roughly linearly with boat speed; power draw falls much more slowly. Expect about 55–60% of rated thrust at 1.5 mph while still drawing ≈2.3 kW. Estimated calm-water top speed: ≈1.0 mph with one unit, ≈1.3 mph with two (see hull-drag section). These are engineering estimates (±25–30%) — calibrate with a dockside bollard test and GPS speed trials.

Estimated Performance vs Vessel Speed

Vessel speed (mph)(m/s) Thrust (N)Thrust (lbf) Power draw (kW)Propulsion efficiency*
0 (stationary)03,2007203.20— (bollard)
0.50.222,7206102.8921%
1.00.452,2505052.5839%
1.50.671,7704002.2752%
2.0 (extrapolated)0.891,2902901.9659%

*Efficiency = thrust × speed ÷ electrical power. It rises with speed (the rotor unloads), but absolute thrust margin shrinks. Thrust reaches zero at ≈3.4 mph; power draw never reaches zero (≈1.1 kW remaining at that point, absorbed by blade profile drag). Running two units simply doubles both columns.

Thrust & Power vs Speed (three scenarios)

Optimistic (constant-power limit) Best estimate (fixed RPM) Conservative Power draw (right axis)
0800 160024003200 N 01 23 kW 00.5 1.01.5 2.02.5 3.0 mph Vessel speed (mph) Thrust (N)

Scenario Bounds

Speed (mph)Optimistic thrust (N)Best-estimate thrust (N) Conservative thrust (N)Power draw range (kW)
03,2003,2003,2003.20
0.52,9602,7202,5502.85 – 3.20
1.02,7302,2501,9002.49 – 3.20
1.52,5001,7701,2502.14 – 3.20

How the Estimates Were Made

Step 1 — Decode the bollard rating

Momentum theory gives two exact identities for a rotor in stationary water: power P = T × vᵢ (where vᵢ is the induced velocity at the rotor plane), and the far slipstream moves at w = 2·vᵢ. With the rated 3,200 W and 3,200 N:

The physical propeller is 2.5 m (disk area 4.91 m²), so the unit performs like an ideal actuator about 1.4 m across — a figure of merit of ≈0.68 versus a perfect 2.5 m disk (which would give ≈4,700 N at this power). That is entirely typical for real thruster hardware, so the published rating looks credible and is used here at face value.

Step 2 — Zero-thrust speed

At fixed shaft speed and fixed pitch, thrust vanishes when the advance speed reaches the blades' zero-lift pitch speed. For heavily loaded, low-pitch mixers this occurs at roughly 0.6–0.8× the bollard slipstream speed, i.e. Vₔₜ ≈ 1.2–1.6 m/s. Adopted central value: 1.5 m/s ≈ 3.4 mph.

Step 3 — Decay laws (anchored to the rating)

T(V) = 3200 × (1 − V / 1.5) N (V in m/s) P(V) = 3.2 × (1 − 0.65 × V / 1.5) kW

Intuition: as the seastead moves forward, water already flows through the rotor, reducing each blade's angle of attack — like a fan on a moving cart. Torque (and therefore electrical power) decays more slowly than thrust because blade profile drag keeps absorbing torque even after net thrust reaches zero. This mirrors standard propeller Kₜ/K₌ chart behavior (e.g., Wageningen B-series).

Steps 4–5 — Bounds

Optimistic bound (only reachable if the drive held power constant): the constant-power actuator-disk equation, solved for T at each speed:

T³ + 2ρAₑ·P·V·T − 2ρAₑ·P² = 0, ρ = 1025 kg/m³

Conservative bound: effective zero-thrust speed lowered to 1.1 m/s (shorter pitch / shroud drag), power factor 0.545.

Hull Drag & Expected Top Speed (illustrative)

Based on your description — four 4-ft-wide columns, 13 ft long at 45° (vertical extent ≈9.2 ft each ≈ 147 ft² frontal) plus cable/appendage allowance ≈ 175 ft² (16.3 m²), at Cₖ ≈ 1.3 ⇒ drag area CₖA ≈ 21 m². Drag = ½ρU²·CₖA ≈ 10,760×U² (N):

SpeedDrag (N)Drag (lbf)
0.5 mph540120
1.0 mph2,150480
1.5 mph4,8401,090

Solving thrust = drag against the best-estimate thrust curve: ≈1.0 mph with one unit (range 0.9–1.2 across scenarios), ≈1.3 mph with two units (range 1.2–1.6). If your columns are round rather than square, drag drops ~30–40% and speeds rise accordingly — send me the real cross-section and cable layout and I'll tighten this.

Station-keeping reality check: one unit can hold position against only ≈1.0 knot of pure current (two units ≈1.5 kt) before wind and wave loads, which will usually dominate. Plan mooring for weather, thrusters for maneuvering and slow transit.

Practical Notes for the Design

Recommended Calibration (cheap and decisive)

  1. Dockside bollard test: spring scale or load cell astern; log DC volts × amps. Confirms the 3,200 N / 3.2 kW anchor point.
  2. Speed runs: in calm water, log DC power and GPS speed-over-ground. Your measured drag curve plus the linear law T = T₀ − kV lets you refit everything with two numbers.
  3. Optional tow test: measures raw thrust-vs-speed independent of hull drag.
Assumptions & limitations: Manufacturer rating taken at face value (±10% typical); actual shaft speed, pitch, and shroud configuration unknown; fixed-RPM fixed-pitch operation assumed; seawater density 1025 kg/m³; wind, wave, and current loads excluded; hull drag estimated from described geometry only. These are engineering estimates for feasibility screening — not a substitute for prototype testing. Prepared as design support for a seastead propulsion study.
``` **A few things worth flagging:** 1. **The rating is self-consistent.** Feeding 3,200 N / 3.2 kW through momentum theory implies the unit behaves like an ideal actuator disk ~1.4 m across (figure of merit ≈0.68 vs. the physical 2.5 m disk) — normal for real hardware, so I trusted the spec as the anchor point. 2. **Your intuition on power was right, but the drop is modest** — from 3.2 kW to only ~2.3 kW at 1.5 mph. Practically, size solar for the full 3.2 kW. 3. **The biggest lever is RPM, not speed.** Since power scales ~RPM³, a VFD at 70% speed cuts draw to ~⅓ while costing you only ~30% of top speed. For a solar-only seastead, that's probably your default cruise mode. If you can share the actual column cross-section (square vs. round), cable count/diameter, or the mixer's rated RPM, I can tighten the drag and zero-thrust-speed estimates considerably.