Naval Architecture Primer for Evaluating a Foil-Legged Triangular Seastead

This page introduces the key naval-architecture ideas needed to understand and evaluate a shippable seastead concept with a 44-foot equilateral living triangle, three buoyant foil-like legs, low-mounted batteries, rim-drive thrusters, heave plates, and optional tension-leg mooring. It is written for technically interested readers, not as a substitute for a qualified marine engineer.

Disclaimer: Floating structures involve life-safety issues: stability, flooding, structural loads, electrical safety, fire, towing, mooring, and survivability in storms. This material is educational. A final design should be reviewed by a naval architect or marine engineer and tested before full-scale construction.

The design being evaluated

The concept is a triangular floating living platform intended to be packed into a single 45-foot High Cube container, shipped to a yard, and assembled. The main features are:

  • Triangular living structure: equilateral triangle, 44.0 ft side, 7 ft interior height, enclosed living area.
  • Walkway: about 3 ft wide around most of the outside, bolted on, with railings and open aluminum grating.
  • Three buoyant legs: foil-shaped, NACA-like sections, mounted near the triangle corners, intended to provide buoyancy and a softer ride.
  • Container compatibility: parts sized to fit a 45 ft High Cube container: roughly 7.7 ft wide, 8.9 ft high, 44.6 ft long.
  • Displacement target: desired rated buoyancy at waterline about 27,500 lb.
  • Batteries: about 25% of displacement, placed low in the legs for stability and power.
  • Propulsion: six fixed-orientation rim-drive thrusters, two per leg, using differential thrust for steering.
  • Station-keeping: optional helical mooring screws and tension legs for parked operation.
  • Community mode: two units may connect with a walkway and cooperate through thruster control.

The central naval-architecture question is whether this arrangement can provide enough buoyancy, stability, strength, motion comfort, propulsion, and safety while staying under its weight target and remaining shippable.

First principles: buoyancy, weight, and stability

Buoyancy and displacement

A floating object displaces a weight of water equal to its total weight. In naval architecture, the total floating weight is called displacement. If the design waterline is rated at 27,500 lb, then the entire assembled seastead plus everything on it must weigh less than that if it is to float at or above the desired waterline.

Displacement weight W = weight of displaced water Displaced volume V = W / gamma where gamma is the specific weight of water: seawater: about 64 lb/ft^3 freshwater: about 62.4 lb/ft^3

For 27,500 lb in seawater, the submerged volume is approximately:

V = 27,500 lb / 64 lb/ft^3 = 430 ft^3

This 430 cubic feet is the total underwater volume required at that waterline. If the three legs are the only buoyant bodies, then each leg must provide roughly one-third of that displaced volume, plus additional reserve buoyancy for safety, waves, loading errors, and payload.

Weight budget is the first gate

A container can carry up to about 62,000 lb, but that does not mean the seastead can weigh that much. The container rating is a shipping limit. The floating structure must obey its buoyancy limit. If all shipped parts become part of the floating seastead, then the total shipped weight is essentially the lightship weight plus any shipped outfit. That total must be far below 27,500 lb if people, batteries, systems, furniture, water, stores, dinghy, and safety equipment are also included.

Example weight-budget view, not a final calculation
Item Approximate budget Comment
Rated buoyancy at desired waterline 27,500 lb Maximum available before the design sits too low.
Batteries at 25% of displacement 6,875 lb Large battery bank; improves stability if placed low.
Remaining for structure, systems, payload, margin 20,625 lb Must include hull, walls, deck, walkway, thrusters, controllers, solar, wiring, doors, railings, dinghy, people, gear, and margin.
Important: A 27,500 lb displacement target is quite tight for a 44-foot enclosed living structure with three large buoyant legs, six electric thrusters, batteries, solar, railings, and outfit. A detailed weight estimate is one of the first things that should be produced.

Stability: center of gravity and metacenter

Stability is not just “does it float?” It is “does it resist heeling and return upright after wind, waves, people moving, or equipment shifting?” The key points are:

  • Center of gravity, G: the average height and position of all weights. Lower is usually better.
  • Center of buoyancy, B: the centroid of the underwater volume. It moves as the platform heels.
  • Metacenter, M: a stability reference point created by the shift in buoyancy when heeled.
  • Metacentric height, GM: distance from G to M. Positive GM means initial static stability.
GM = KB + BM - KG where: KB = height of center of buoyancy above keel BM = metacentric radius = I_waterplane / V KG = height of center of gravity above keel V = displaced volume

Batteries low in the legs help reduce KG. Wide separation between the three legs can help stability by increasing the waterplane moment of inertia, but the exact result depends on how much waterplane area each leg has and how far apart the leg buoyancy acts.

1. Resonant roll period

A floating platform does not just sit still; it rolls, pitches, heaves, sways, surges, and yaws. Roll is side-to-side tilting. Like a pendulum or spring-mass system, a floating body has a natural roll period. If wave energy arrives at a similar period, the motion can amplify. This is called resonance.

Approximate natural roll period: T_roll = 2 * pi * sqrt(I_xx / (W * GM)) or, using radius of gyration k: T_roll = 2 * pi * k / sqrt(g * GM) where: T_roll = natural roll period, seconds I_xx = mass moment of inertia about the roll axis W = displacement weight GM = transverse metacentric height k = radius of gyration in roll, length units g = 32.2 ft/s^2

Why it matters for this seastead

The triangular planform and widely spaced legs may give strong form stability. If GM is large, the platform will be “stiff”: it will snap back quickly, producing a short roll period and possibly uncomfortable accelerations. If GM is small, it will be “tender”: slower roll, larger angles, and potentially alarming motion if not properly damped.

Illustrative roll periods for a 20 ft roll radius of gyration
GM Approximate roll period Qualitative feel
2 ft about 15.7 s Slow, tender, potentially large roll angles.
5 ft about 9.9 s Moderate; could overlap swell periods.
8 ft about 7.8 s Stiffer; may feel quicker.
12 ft about 6.4 s Very stiff; potentially uncomfortable.

In many coastal and Caribbean sea states, dominant wave periods can be roughly 3 to 8 seconds for wind waves and sometimes 7 to 12 seconds for swell. A design should try to avoid having its roll period sit directly in the middle of the expected wave energy spectrum, or it should provide enough damping to limit the response.

Design question: What is the expected roll period with full battery load, half battery load, people on one side, and dinghy stowed? What damping is provided by the legs, heave plates, and thruster control?

The heave plates on the lower legs can help because they increase hydrodynamic damping. They do not create restoring force by themselves, but they can dissipate motion energy. Active thruster control may also help if it has enough authority, fast sensors, and stable control logic.

2. Small waterline area

The waterline area, or waterplane area, is the planform area of the floating body cut at the water surface. A conventional barge or pontoon has a large waterplane area. A semi-submersible or SWATH-like craft tries to make the waterplane area small while putting most buoyancy below the wave-affected surface layer.

Why small waterplane area can give a softer ride

  • Waves apply less direct vertical and horizontal excitation where the structure pierces the surface.
  • Heave stiffness is reduced, which can lengthen the heave period and reduce abrupt motion.
  • Pitch and roll excitation can be reduced if the buoyancy is concentrated below the surface.
  • Deck can stay higher above wave action if freeboard and reserve buoyancy are properly designed.
Heave restoring stiffness is approximately: k_heave = rho * g * A_waterplane or, using specific weight: k_heave = gamma * A_waterplane where: gamma = water specific weight, about 64 lb/ft^3 A_waterplane = total waterplane area

If the waterplane area is small, adding weight or pulling the platform downward produces less additional buoyancy per inch of sinkage. This is useful for reducing wave response, but it also means the design is more sensitive to weight and trim errors.

Application to the three-leg foil concept

This design wants the legs to behave somewhat like small-waterline-area columns or hydrofoils. Whether it truly acts that way depends on the leg geometry at the water surface:

  • If each leg pierces the water with a narrow section, waterplane area can be small.
  • If each leg has a broad chord at the waterline, the waterplane area may be larger than intended.
  • If the legs are widely separated, the waterplane moment of inertia can still be large even if total area is modest.
  • If the legs are deeply submerged with only narrow struts at the surface, the behavior becomes more SWATH-like.
Design question: What is the total waterplane area, and what is its second moment of area? These numbers strongly affect heave stiffness, initial stability, and reserve buoyancy.
Small waterline area can improve comfort, but it can also reduce reserve buoyancy. The design must still have enough volume above the design waterline to handle waves, passenger movement, battery weight variations, mooring pretension, and flooding contingencies.

3. Drag for something moving through the water

Any object moving through water must overcome hydrodynamic resistance. For this seastead, drag matters for cruising speed, energy use, thruster sizing, maneuvering, and station keeping. Water is dense: seawater has a mass density of about 1,025 kg/m³, or a specific weight of about 64 lb/ft³, so hydrodynamic forces become large quickly.

Hydrodynamic drag is often written as: D = 0.5 * rho * V^2 * S * C_D where: D = drag force rho = water density V = speed relative to water S = reference area C_D = drag coefficient, depending on shape and flow condition

Main components of water resistance

  • Frictional drag: caused by water shearing along wetted surfaces. Depends on wetted area, speed, roughness, and Reynolds number.
  • Form drag: caused by pressure differences around bluff shapes. Thick bodies, edges, brackets, and appendages increase form drag.
  • Wave-making resistance: energy lost into making waves. Important near the surface and at higher displacement speeds.
  • Appendage drag: heave plates, thrusters, conduit, ladder, mooring parts, and the dinghy all add drag.
  • Interference drag: flow disturbances where legs, braces, and hull sections meet.

The foil-shaped legs are a good idea compared with plain cylindrical legs if the flow is aligned with the foil. A streamlined section can reduce pressure drag. However, a NACA 0035 section is very thick: 35% thickness-to-chord. With an 8.5 ft chord, the maximum thickness would be about 2.98 ft before any trailing-edge truncation. That is streamlined compared with a flat plate, but still a large bluff body compared with a slender aircraft foil.

Power grows rapidly with speed

For displacement-type craft, required power often rises faster than linearly with speed. As a rough rule, if drag is approximately proportional to speed squared, then power is approximately proportional to speed cubed:

Power = Force * Velocity If D ~ V^2, then Power ~ V^3

This means doubling speed can require about eight times the power in the simple quadratic-drag case. For a seastead intended to be efficient and solar-supported, modest speed targets are usually far more realistic than high speed.

Propulsion considerations

  • Six rim-drive thrusters of about 1.5 ft diameter give redundancy and maneuverability.
  • Small propulsors can be less efficient than larger, slower-turning propellers, especially for a heavy displacement craft.
  • Rim drives need careful attention to blade tip clearance, cavitation, ventilation, debris protection, and motor cooling.
  • Fixed forward-facing thrusters can create yaw through differential thrust, but they may not provide much pure sideways force. Station keeping in beam wind or current may require mooring, angled thrusters, or additional lateral control.
Design question: What is the predicted total resistance at intended cruising speed, including legs, heave plates, brackets, and thruster installations? What thrust margin exists for wind, current, and fouling?

4. Wind drag

Wind drag is often underestimated on floating living platforms. This design has a large enclosed triangular volume, 7 ft high walls, railings, a walkway, solar panels, and possibly people and equipment on deck. Even at modest wind speeds, the forces can be large because air loads scale with projected area and the square of wind speed.

Wind force is often estimated as: F_wind = 0.5 * rho_air * V_wind^2 * A_projected * C_D A convenient approximation in Imperial units: dynamic pressure q ~= 0.0034 * V_knots^2 lb/ft^2 where: rho_air = air density, about 0.00238 slug/ft^3 at sea level V_knots = wind speed in knots A_projected = projected area facing the wind C_D = shape coefficient
Approximate wind dynamic pressure
Wind speed Dynamic pressure
10 knots about 0.34 lb/ft²
20 knots about 1.36 lb/ft²
30 knots about 3.05 lb/ft²
40 knots about 5.42 lb/ft²

The triangular living volume has three wall sides, each about 44 ft long and 7 ft high. Not all walls face the wind at once, but a broad side can have a projected area on the order of several hundred square feet. Add roof edge, railings, solar array, walkway furniture, and dinghy, and the windage becomes significant.

Example

Suppose the effective projected side area is 300 ft² and the drag coefficient is about 1.0. At 30 knots:

F_wind ~= 3.05 lb/ft^2 * 300 ft^2 * 1.0 ~= 915 lb

That is a steady side force. Gusts, turbulence, and moments around the center of gravity can make the effective loading more challenging. If the seastead must hold position with thrusters, that wind force must be overcome with a safety margin. If it is moored, the mooring system must carry those loads.

Wind effects beyond simple drag

  • Yaw moment: wind not applied at the center of drag will turn the seastead.
  • Heel moment: wind high on the walls can heel the platform.
  • Solar uplift: roof panels can experience lift and suction, especially at edges.
  • Dinghy shielding: the living area may shield the dinghy in forward motion, but not in all directions.
  • Connected units: two connected seasteads may create complex wind shadows and relative motion.
Design question: What are the projected wind areas from ahead, astern, and beam? Can the thrusters hold position and heading in the intended operating wind? What are the mooring loads in gusts?

5. Active stabilizers

Active stabilizers are systems that sense motion and apply forces to reduce it. They can be very effective, but they require power, sensors, control algorithms, maintenance, and fail-safe behavior. They should not replace basic passive stability and buoyancy.

Types relevant to this concept

  • Differential thrust stabilization: using the six rim drives to oppose roll, pitch, or yaw motions.
  • Active mooring pretension: adjusting tension legs or mooring lines to reduce heave and pitch while parked.
  • Active ballast or movable mass: shifting weight or water to trim the platform.
  • Active foils or fins: possible future enhancement, but adds mechanical complexity.

The proposed design already has some passive motion control: foil-shaped legs, heave plates, and low batteries. The heave plates are especially relevant because they increase damping in heave and pitch. Damping is what reduces the sharpness of resonant motion.

Using thrusters as stabilizers

If the control system knows the platform is starting to roll or pitch, it could command one pair of thrusters to produce a moment that opposes the motion. Because the thrusters are located near the legs and low in the water, they may generate useful moments. However:

  • The thrusters are primarily forward-facing, so their authority may be limited for pure heave or sway.
  • Continuous stabilization consumes battery energy.
  • Control delay or incorrect tuning can make motion worse.
  • The system must degrade safely if a sensor, controller, or thruster fails.
Active stabilization should be treated as a comfort and station-keeping aid, not as the primary safety system. The platform should remain safe and stable with stabilization off.

Connected seasteads

If two units connect with a walkway and coordinate their thrusters, they can potentially reduce relative motion. This is attractive but demanding. The two control systems must agree on a common reference, handle communication delays, respect each unit’s battery state, and avoid fighting each other. The walkway itself must tolerate relative surge, sway, heave, roll, pitch, and yaw without becoming a hazard.

Design question: What motion reduction is required for the walkway to be safe? What relative motion limits are acceptable? What happens if communication between units is lost while someone is on the walkway?

6. Semi-submersible platforms

A semi-submersible platform is a floating structure that gets most of its buoyancy from submerged pontoons or columns, with a deck held above the water by relatively smaller waterplane areas. Offshore oil platforms, heavy-lift vessels, and some advanced floating homes use versions of this idea.

Why semi-submersibles ride more softly

  • Wave energy is strongest near the surface. Putting buoyancy deeper reduces wave excitation.
  • Small waterplane area reduces the instantaneous change in buoyancy as waves pass.
  • Wide column spacing provides stability while keeping waterplane area modest.
  • Long natural periods can move the platform away from dominant wave frequencies.

Comparison with the proposed seastead

The proposed concept has features of both a trimaran and a semi-submersible/SWATH craft. The three legs provide buoyancy near the corners of the triangle, while the deck structure sits above them. If the legs have relatively small waterplane area and most buoyancy is below the active wave zone, the ride can be softer than a simple pontoon.

Semi-submersible behavior versus simple pontoon behavior
Feature Simple pontoon/barge Semi-sub/SWATH-like concept
Waterplane area Large Smaller
Wave excitation High Lower if designed well
Initial stability Often high from wide deck Must be engineered from geometry and low CG
Weight sensitivity Moderate Higher; small waterplane means less reserve per inch
Draft Usually shallow Often deeper
Ride quality Can be abrupt Can be softer if tuned
Design question: Are the legs truly acting like semi-sub columns, or are they more like shallow trimaran floats? The answer changes the expected motion, drag, and stability behavior.

The tension-leg parking idea is also related to offshore practice. A tension-leg platform uses taut vertical or near-vertical tendons to restrain heave. For a small Caribbean seastead, helical screws and pretensioned lines could reduce motion, but the system must be designed for fatigue, corrosion, installation load, seabed type, storm loads, and accidental slack-line/snap-load conditions.

7. Coefficient of drag due to shape

The drag coefficient, CD, is a dimensionless number that captures how much drag a shape creates for a given reference area and flow speed. It is extremely useful, but it must always be interpreted with the correct reference area and flow condition.

C_D = Drag / (0.5 * rho * V^2 * S_reference) A given C_D only means something if you know: - the reference area S - whether flow is laminar or turbulent - Reynolds number - surface roughness - angle of attack or current direction

Typical shape behavior

Very approximate shape comparison
Shape Typical behavior Relevance to seastead
Flat plate facing flow High drag, often CD near 1.1 to 1.3 based on frontal area Avoid broad blunt faces normal to flow.
Cylinder Moderate to high drag, often around 0.8 to 1.2 depending on Reynolds number Plain cylindrical legs would have more drag than streamlined foils.
Streamlined foil at low angle of attack Low drag relative to blunt bodies Foil legs can reduce forward drag if aligned well.
Thick foil at nonzero angle Drag rises with angle, separation, and roughness Legs may see current, waves, and sideslip, not just perfect forward flow.
Open grating or railing Lower solid area but can create turbulence and local drag Useful for waves and wind, but needs structural load checks.

Application to the foil legs

A NACA 0035 foil with the leading edge forward should generally have lower drag than a flat plate or cylinder of comparable frontal size, especially at low speed and small flow angle. However, the section is thick, truncated, surface-piercing, and fitted with heave plates and thrusters. The installed drag may be much higher than a clean isolated foil section.

  • The leading edge facing forward is favorable for forward motion.
  • The truncated trailing edge helps container packing but may slightly increase drag compared with a fully closed tail.
  • Heave plates increase damping but also increase drag and vortex shedding.
  • Marine growth, welds, and rough paint can increase frictional drag over time.
  • Currents and waves can hit the legs from angles other than straight ahead.
Design question: What reference area is being used for each CD estimate? Is it frontal area, wetted area, planform area, or projected side area? Comparisons are only valid if the reference area is consistent.

How these ideas interact in this design

The interesting part of evaluating this seastead is that the naval-architecture features are coupled. A change in one area affects several others.

Soft ride versus stability

A soft ride often suggests lower stiffness and lower wave excitation. But too little stiffness can mean large heel angles and poor recovery. The batteries low in the legs help because they lower the center of gravity without taking up deck space. The triangle width helps because it spreads buoyancy. The final comfort and safety depend on the computed GM, roll inertia, damping, and wave response.

Small waterline area versus payload margin

The small-waterline goal can improve comfort, but it makes the platform more sensitive to weight. If the structure comes out heavier than planned, the waterline rises, freeboard decreases, and the intended motion behavior may change. This makes weight control and a careful weight margin essential.

Foil drag versus heave damping

The foil legs reduce forward drag relative to bluff shapes, but the heave plates increase drag. This is a deliberate trade: more drag and complexity in exchange for reduced wave response. The right amount depends on whether the platform will spend most of its time parked, moving slowly, or transiting.

Windage versus thruster sizing

The enclosed living volume and solar roof create windage. If the seastead is expected to hold position electrically, the thrusters must overcome wind and current with margin. If it will mostly be moored or tension-legged while parked, the mooring system becomes a primary load path.

Container shipping versus structural continuity

Packing the structure into a container is a powerful idea, but bolted joints, alignment tolerances, watertightness, fatigue, corrosion, and assembly loads become critical. The structure must not only fit in the container; it must also carry wave, wind, occupant, mooring, and lifting loads after assembly.

Simple sanity-check calculations

1. Required submerged volume

At 27,500 lb displacement in seawater:

27,500 / 64 = 430 ft^3 total submerged volume

This is the volume below the waterline. The legs must provide this volume plus reserve. If the legs are the only buoyant bodies, the design should be checked to see whether the actual submerged foil volume exceeds 430 ft³ with enough margin for payload and waves.

2. Battery fraction

At 25% of displacement:

0.25 * 27,500 = 6,875 lb 6,875 lb ~= 3,120 kg

For LiFePO4, pack-level energy density varies widely by manufacturer and packaging, but a rough order-of-magnitude range might be about 100 to 160 Wh/kg. That gives roughly 300 to 500 kWh at the pack level. The exact number depends on cells, enclosures, BMS, cooling, and safety margins.

3. Roof area for solar

The roof is approximately an equilateral triangle with 44 ft sides:

Area = sqrt(3)/4 * side^2 Area = 0.433 * 44^2 Area ~= 838 ft^2 ~= 78 m^2

This is a useful solar area, but the panels add weight, wind uplift, wiring complexity, and maintenance access issues. They must be secured for marine vibration and spray.

4. Wind pressure

q ~= 0.0034 * V_knots^2 lb/ft^2 At 20 knots: q ~= 1.36 lb/ft^2 At 30 knots: q ~= 3.05 lb/ft^2

Multiply by projected area and drag coefficient to estimate wind force. This quickly shows whether thruster or mooring capacity is realistic.

5. Roll period example

T_roll ~= 2 * pi * k / sqrt(g * GM) Assume k = 20 ft and GM = 5 ft: T_roll ~= 2 * pi * 20 / sqrt(32.2 * 5) ~= 9.9 seconds

This is only an example, but it shows why GM and mass distribution matter. The actual radius of gyration depends on how the batteries, structure, people, and equipment are distributed.

Evaluation checklist

Area Question to answer Good sign Red flag
Weight What is the detailed lightship weight and payload budget? Itemized weight sheet with margin. No detailed weight estimate; structure assumed “light enough.”
Buoyancy What is the submerged volume at design waterline and at maximum load? Reserve buoyancy and clear freeboard margin. Waterline near deck edge; no reserve volume.
Stability What are KG, GM, heel angles, and righting moments? Positive stability with adequate margin under passenger and wind loads. Only “batteries are low” with no calculated stability curve.
Roll period What is the natural roll period in loading conditions? Roll period and damping tuned away from dominant wave periods. Very short stiff roll or uncontrolled resonant roll.
Waterplane What is the waterplane area and moment of inertia? Clear calculation showing intended small-waterline behavior. Unclear whether legs produce small or large waterplane area.
Drag What is total resistance at intended speed? Resistance broken into friction, form, wave, and appendage components. Only clean-foil section drag considered; no installed drag.
Wind What are wind forces and moments? Projected areas and thruster/mooring margins calculated. Assuming wind is negligible because the platform is slow.
Thrusters Can six rim drives maneuver and hold the craft in design conditions? Thrust maps, redundancy, and failure modes analyzed. No calculation of required thrust for wind/current.
Mooring Are helical anchors and tension legs adequate? Geotechnical data, fatigue analysis, and pretension plan. Assuming calm protected water without storm planning.
Structure Can bolted joints and deck beams carry wave and lifting loads? Structural analysis of frames, beams, walkway, and leg attachments. Only container packing considered, not ocean loads.
Safety What happens if one leg compartment floods? Damage stability and multiple sealed compartments verified. Unsealed penetrations, no damage stability analysis.
Regulations What rules apply? Early consultation with marine surveyor, class society, or coast guard. Assuming no rules because it is small or slow.

Recommended next steps

  1. Create a detailed weight estimate. Model every structural panel, leg, battery pack, thruster, controller, rail, door, solar panel, wire, bolt, gasket, and piece of furniture. Add a realistic margin.
  2. Build a hydrostatic model. Use marine design software or naval-architecture calculations to find displacement, draft, trim, center of buoyancy, waterplane area, GM, and righting arms.
  3. Check stability in load cases. Include full batteries, empty batteries, people on one side, wind heel, dinghy loaded, and one-compartment flooding if applicable.
  4. Estimate roll and pitch periods. Compare them with expected local wave periods. Add damping from heave plates in the analysis.
  5. Estimate installed drag. Include legs, heave plates, thrusters, conduit, ladder, walkway supports, and surface roughness.
  6. Calculate wind loads. Use projected areas from multiple directions. Check thruster authority and mooring loads.
  7. Analyze structures. Check global bending, leg-to-deck connections, bolted joints, walkway supports, rail loads, solar wind uplift, and lifting/shipping loads.
  8. Review electrical and battery safety. LiFePO4 is chemically safer than some lithium chemistries, but marine electrical systems still need proper insulation, fusing, BMS, ventilation, corrosion control, and fault protection.
  9. Prototype or model test. A scale model in waves can reveal motion, resonance, green water, and steering behavior much faster than theory alone.
Summary: The concept has interesting and defensible features: triangular wide stability, low batteries, foil-like legs, small-waterline potential, redundant electric propulsion, and container-based transport. The key to evaluating it is not just the geometry, but the numbers: weight, submerged volume, GM, roll period, waterplane area, drag, wind force, thruster authority, structural loads, and safety margins.