Seastead Drogue and Stabilizer Analysis

1. Introduction

This analysis addresses the questions posed regarding the seastead design, focusing on the range of orientations achievable with a trailing drodrogue, recommended drodrogue sizes for moving at 6 knots in various wind speeds, thoughts on adjustable drogues, and the feasibility of using stabilizers to lift the seastead at high speeds. Key assumptions are made based on the provided description and typical engineering approximations.

Key Assumptions:

2. Range of Orientation Off Downwind with Trailing Drogue

The proposed system uses two winches at the back corners, each connected to a drodrogue via ropes, forming a bridle. This allows adjustment of the drodrogue's position relative to the seastead's centerline. The range of angles off directly downwind depends on:

Typical sliding bridle systems on vessels can achieve orientations of 30° to 60° off downwind. For this seastead, with the back corners 35 ft apart (width of triangle back) and assuming ropes of moderate length (e.g., 50-100 ft), a reasonable estimate is:

Estimated range: Up to 45° left and right of directly downwind (total 90° sweep). This allows significant control to avoid beam-on winds and adjust course as needed.

Note: The actual range should be verified with simulation or scale model testing, considering the flexibility of the ropes and drodrogue behavior.

3. Drogue Size Recommendations for 6 Knots in Various Winds

The goal is to move at 6 knots (20.25 ft/s) even with the drodrogue deployed. The thrusters must overcome the combined drag of the seastead and drodrogue. Wind forces add to the load, but the drodrogue drag should balance the wind force to maintain stability.

Wind Force Estimation:

Wind force F_wind = 0.5 * ρ_air * v_wind² * Cd_air * A_air, with A_air ≈ 200 ft², Cd_air = 1.0.

Wind Speed (mph) Wind Force (lb)
30 ~464
40 ~826
50 ~1,290
60 ~1,860

Required Drogue Drag at 6 Knots:

Assuming the drodrogue drag must equal the wind force to counteract it, and using the drag formula D_drogue = 0.5 * ρ * v² * Cd_drogue * A_drogue, with ρ = 2.0 slug/ft³, v = 20.25 ft/s, and assuming Cd_drogue = 1.0 (typical for cone drogues), we solve for A_drogue.

Wind Speed (mph) Required Drogue Area (ft²) Required Diameter (ft) for Cone (Cd=1.0)
30 ~1.13 ~1.2
40 ~2.01 ~1.6
50 ~3.15 ~2.0
60 ~4.54 ~2.4
Note: These are minimum areas assuming the drodrogue moves at 6 knots relative to water. In practice, the drodrogue speed is lower, so actual required areas may be larger. Also, the seastead's own drag at 6 knots (estimated at 500 lb) reduces the available thrust for drodrogue drag. With an estimated thruster capacity of 3,000 lb, the maximum drodrogue drag could be ~2,500 lb, which is sufficient for 60 mph winds if properly sized.

Recommendation:

A drodrogue with an adjustable frontal area of 4–6 ft² (e.g., a cone with diameter 2.5–3 ft) would be suitable for the range of winds, with the ability to reduce drag in lower winds. Consider a system with multiple cones (e.g., Jordan Series Drogue) for adjustability.

4. Thoughts on Adjustable Drogues

Jordan Series Drogue:

This consists of multiple small cones in series, allowing incremental deployment. By pulling the collapse line, cones can be disabled, reducing drag. For our needs, a Jordan Series Drogue with about 20 cones of 6–8 inch diameter could provide the required drag area. Each cone contributes to drag, and the total can be adjusted by adding or removing cones from the water. This is a good option for fine-tuning drag.

Galerider-Style Perforated Drogues:

These use a perforated fabric that allows water flow, reducing shock loads. They are typically not as adjustable in drag area as Jordan drogues, but some models have adjustment mechanisms. They may come in sizes suitable for this application, but availability should be checked.

Adjustable Parachute/Basket Drogues with Collapse Line:

These drogues have a purse-string that reduces the open diameter, lowering drag. This is directly adjustable on the fly, which is beneficial for changing conditions. For the required drag range (1–5 ft² area), a parachute drodrogue with an initial diameter of 3–4 ft could be scaled down to 1–2 ft. This seems very suitable.

Conclusion: An adjustable parachute drodrogue with a collapse line is recommended for its simplicity and ease of adjustment. Alternatively, a Jordan Series Drogue offers incremental control. Both can be sized appropriately.

5. Stabilizer Lift Analysis for Running from Storms

The concept is to use the stabilizers (little airplanes) to lift the seastead partially out of the water at high speeds (e.g., 12 knots), reducing drag from the legs and allowing faster movement to escape storms. We analyze the required size of each stabilizer wing to take half the seastead weight (i.e., total lift from stabilizers = 0.5W).

Lift Equation:

L = 0.5 * ρ * v² * S * Cl

where:

Scenario A: Each stabilizer takes half the seastead weight (L = 0.5W)

L = 0.5 * 27,360 = 13,680 lb
S = 2L / (ρ v² Cl) = 2*13,680 / (2.0 * 20.25² * 0.7) = 47.66 ft²
Given existing stabilizer wing span = 12 ft, chord = 1.5 ft, area = 18 ft². This is insufficient for individual half-weight lift; would need ~2.6 times larger area.

Scenario B: All three stabilizers together take half the weight, each providing one-third (L = 0.5W/3 = W/6)

L = 27,360 / 6 = 4,560 lb
S = 2*4,560 / (2.0 * 20.25² * 0.7) = 15.89 ft²
This is close to the existing area of 18 ft². With Cl = 0.7, the existing stabilizers could provide this lift at 12 knots. At 12 knots, the lift would be L = 0.5*2*20.25²*18*0.7 = 0.5*2*410.06*18*0.7 = 5,176 lb per stabilizer, which is more than 4,560 lb. So the existing stabilizers may be adequate for lifting half the weight when all three are used.
Feasibility: The stabilizer concept is plausible. At 12 knots, the legs and stabilizers can generate significant lift. However, the stabilizers' control surfaces must be robust to handle the loads and provide adequate control. The existing stabilizer design (12 ft span, 1.5 ft chord) appears reasonably sized for the half-weight lift if all three work together.

6. Structural Thickness Analysis for Stabilizers

We determine the required thickness of the stabilizer wing to withstand bending loads at high speeds. The load is from lift; we use the lift from Scenario B (L = 4,560 lb per stabilizer) as a realistic design load.

Bending Stress:

Root bending moment M = L * (span/2) = 4,560 * (12/2) = 27,360 ft-lb = 328,320 in-lb.
Assuming aluminum with allowable stress σ_allow = 15,000 psi (with safety factor), required section modulus S_required = M / σ_allow = 21.888 in³.

Approximate Wing Thickness:

Assuming a rectangular cross-section with width = chord = 18 inches, height = thickness t. Section modulus S = b * t² / 6 => t = sqrt(6S/b) = sqrt(6*21.888/18) = sqrt(7.296) = 2.7 inches.
This is about 15% of chord, which is reasonable for a thin wing structure.

Result: The existing stabilizer wings, if properly designed as structural members, likely have sufficient thickness (or can be thickened to ~3 inches) to handle the loads at 12 knots. The description mentions a notch of 25% chord for the pivot, so thickness may be around 30% of chord (~5.4 inches), which is more than adequate.

7. Conclusion

Further Analysis Needed: Detailed CAD and finite element analysis should be conducted for precise structural sizing and control system design. Model testing is recommended for drodrogue behavior and stabilizer performance.