“ARWIMS — amphibious paddle-track propulsion system — hydrodynamic planing on retractable tracks”

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Technical Information Note
ARWIMS Hydrodynamic Simulator v2.1 — June 11, 2026

Audience: Naval engineers and architects
Subject: Complete description of the calculation model, assumptions, and formulas

1. Problem statement

ARWIMS (AllRoad Water Ice Mud and Snow) replaces conventional propellers with 2 to 4 retractable paddle tracks mounted under the hull. The core questions are:

The simulator answers by computing required power P_req(V) for each operating regime and comparing it to available engine power.

2. Subject of the study

The subject is a vehicle equipped with one or more retractable paddle tracks. It can travel on land using its tracks, and on water by flotation (displacement), or by hydrodynamic planing using the track bottom runs and hull bottom as lifting surfaces.

A. Track geometry

Regardless of the number of tracks:

2-track configuration: one track to starboard, one to port; track system length = 80% of hull length.

3-track configuration: one central track forward, two lateral tracks aft; each track system length = 25% of hull length.

4-track configuration: two tracks to port, two to starboard; each track system length = 37.5% of hull length.

B. Paddle geometry

Each track carries paddles inclined 30° forward from the vertical (i.e., 60° from horizontal). This inclination simultaneously generates a horizontal propulsion component and a vertical lift component. Winglets on both sides of each paddle prevent lateral water leakage. Paddles are deployed on the lower run only when fully submerged — there is therefore no ventilation or cavitation.

The relative speed of the paddles with respect to the water equals the track slip: 5% of the vehicle's speed through water (micro models), or 6% → 4% (full-scale, interpolated between 5 and 30 knots).

C. Central hull

The hull is a shallow-V planing form. For 2- and 4-track configurations, the central hull width equals the overall beam minus the lateral track widths (catamaran-type appearance). For 3-track configurations, the hull spans the full beam with recesses for the embedded tracks.

3. Simulator architecture

Pure client-side JavaScript. For each calculation, five steps are executed:

  1. Read user inputs
  2. Compute track and paddle geometry
  3. Compute hydrostatics (draft, wetted surface)
  4. Compute dynamic lift-off speed from paddle geometry
  5. For each regime: sweep V from V_min to V_max in 0.5-knot increments (refined to 0.05 knots near the limit); keep the highest V where P_req(V) ≤ P_available

4. Inputs

ParameterSymbolUnit
Length overallLm
Beam overallBm
Total loaded weightWkg
Engine powerPkW
Track width (% of beam)k%
Track length (% of hull length)%
Number of tracksNt
Total submerged paddlesNs
Mechanical efficiencyetaMeca— (default 0.92)

5. Geometric model

n_s = Ns / Nt    (submerged paddles per track)
n_p = 2·n_s + 6    (total paddles per track: both runs + roller semi-circles)
Ls = L × trackLenPct / 100    (track system length, capped at config maximum)
w_t = B × k / 100    (track width in metres)
r = Ls / (n_p × 0.9)    (roller radius)
paddle_length = r × 0.9
A_paddle = w_t × paddle_length × cos(30°)    (projected horizontal paddle area)
A_paddle_total = A_paddle × n_p × Nt    (all paddles, all tracks)

For micro-scale models (<2 m, <100 kg), A_paddle is scaled by 0.16 for experimental calibration.

6. Hydrostatics

∇ = W / ρ,    ρ = 1025 kg/m³
Wc = B (Nt = 3)   else   max(0.1, B − 2 × w_t)    (central hull width)
T = ∇ / (L × Wc × 0.8),    floor 0.15 m for full-scale vessels
Sw = L × (Wc × 0.85 + 2 × T × 0.90)    (geometric wetted surface: flat bottom + two sides)

This formula separates the flat hull bottom (factor 0.85, accounting for hull shape) from the two lateral sides (factor 0.90), and uses only the central hull width — not the full beam — since the track volumes replace the outer hull bottom.

7. Displacement resistance model

For both displacement regimes (ARWIMS and propeller reference), total resistance is the sum of viscous and wave-making components.

Viscous resistance (ITTC 1957 with form factor)

Re = V·L / ν,    ν = 1.19×10⁻⁶ m²/s
Cf = 0.075 / (log₁₀(Re) − 2)²
Rf = (1 + k) × ½·ρ·V²·Sw·Cf,    (1 + k) = 1.20 for this hull form

Wave-making resistance (Guldhammer-Harvald)

A tabulated wave resistance coefficient CR(Fn) is used, calibrated for a wide flat hull with block coefficient Cb ≈ 0.80 and L/B ≈ 3–5:

Fn0.100.150.200.250.300.350.400.42
CR0.0010.0020.0040.0070.0120.0200.0350.045
Rw = CR(Fn) × ½·ρ·V²·Sw
R_total = Rf + Rw

A hard upper speed limit is applied: for displacement regimes, V_max cannot exceed the hull speed V_hull = 0.4·√(g·L) in m/s (converted to knots). Beyond this limit, P_req returns 999 999 kW, making the speed unattainable.

8. Dynamic lift-off speed

The minimum speed at which the paddle tracks can fully support the vessel's weight hydrodynamically is computed from the momentum equation. Each paddle acts as a deflector: the lift force equals ½·ρ·V²·A_total·CL, where CL is the thin-airfoil lift coefficient for the paddle inclination:

CL_paddle = 2π·sin(30°) ≈ 3.14
V_liftoff = √( 2·W·g / (ρ · A_paddle_total · CL_paddle) )

This speed is used as the lower bound (V_min) of the planing regimes. Planing is always physically achievable at sufficient speed — there is no static pressure limit, only a dynamic speed threshold.

9. KEY POINT: No track drag

Classic mistake: modeling paddles as a brake R = ½ρV²ACd applied at full boat speed.

ARWIMS reality: paddles operate at 4–6% slip. The relative water/paddle speed is V_slip ≈ 0.05·V_boat, not V_boat. The tangential force on each paddle points aft relative to water — therefore forward relative to the vessel: it is thrust, not drag.

Consequence in the simulator:

Why this matters for planing: in planing regimes, the paddles' velocity relative to the water is only slip × V. Their contribution to drag is therefore negligible. The dominant resistances are the induced drag of the planing surfaces and the viscous friction on their wetted area — both of which favour ARWIMS tracks over a conventional hull, as detailed below.

10. Planing resistance model

All three planing regimes (hull+track, track-only, propeller planing) use a two-component model:

P_req = (R_induced + R_friction) × V / η / 1000    [kW]

The planing fraction f ∈ [0, 1] blends from displacement to full planing as speed increases. At f = 0 the vessel is in full displacement; at f = 1 it is fully planing.

A. Hull + track planing (hulltrack)

The lower track runs act as flat planing surfaces at trim angle τ ≈ 5°. The paddles on these runs add lift at nearly zero additional drag cost (their relative velocity to water = slip × V ≈ 5% of boat speed), boosting total lift without a proportional increase in resistance. The effective lift-to-drag ratio of the ARWIMS planing system is therefore:

L/D_track = 1 / tan(5°) ≈ 11.4
R_induced = W·g / L/D_track × f

The planing fraction f starts at Fn_liftoff (the Froude number corresponding to V_liftoff) and reaches 1.0 at Fn_liftoff + 0.3:

f = clamp( (Fn − Fn_liftoff) / 0.3, 0, 1 )

The effective wetted surface blends from the full hull Sw (at f = 0) to the track bottom run area plus a 15% hull residual (the stern that still grazes the water at full planing):

Sw_planing = Ls × w_t × Nt    (track bottom runs only)
Sw_blend = Sw×(1−f) + Sw_planing×f + 0.15×Sw×f
R_friction = 1.20 × ½·ρ·V²·Sw_blend·Cf

Wave-making resistance applies only in the transition zone and fades as f → 1:

Rw = CR(Fn) × ½·ρ·V²·Sw_blend × (1 − f)

B. Track-only planing (trackonly)

The hull is fully clear of the water. Same L/D model as hulltrack, but no hull residual — the only wetted surface is the four track bottom runs:

f_to = clamp( (Fn − Fn_liftoff×1.3) / 0.6, 0, 1 )
R_induced = W·g / L/D_track × f_to
Sw_eff = Sw_planing × f_to + Sw×0.10×(1−f_to)
R_friction = 1.20 × ½·ρ·V²·Sw_eff·Cf

Because the hull stern no longer grazes the water and there is no wave-making resistance at full planing, track-only achieves higher top speed than hull+track for the same power.

C. Propeller planing reference (propplane)

For the conventional planing hull benchmark, a Savitsky-derived L/D approach is used:

L/D_prop = 5.0    (representative of a good planing hull)
f_pp = clamp( (Fn − 0.8) / 0.4, 0, 1 )
R_planing = W·g / 5.0 × f_pp
Sw_eff = Sw × (1 − 0.55 × f_pp)
η_prop = 0.50 + 0.10 × f_pp    (0.50 at displacement, 0.60 at full planing)

Wave-making resistance applies in the transition zone (fades as f_pp → 1), identical method to hulltrack.

Comparative summary

Regime L/D (planing) Wetted area at full planing η
ARWIMS displacement n/a (hull speed limit) Sw (full hull) 0.55
Hull + track planing ~11.4 (τ = 5°) Sw_planing + 15% hull residual etaMeca × (1 − slip) ≈ 0.87
Track-only planing ~11.4 (τ = 5°) Sw_planing only etaMeca × (1 − slip) ≈ 0.87
Propeller displacement (ref) n/a (hull speed limit) Sw (full hull) 0.50
Propeller planing (ref) 5.0 (Savitsky) Sw × 0.45 at full planing 0.50 → 0.60

The ARWIMS L/D of ~11.4 versus 5.0 for a conventional hull means the induced resistance is 2.3× lower at the same weight and speed. This, combined with the lower wetted area (track runs only vs. full hull bottom), explains the speed and fuel advantage.

11. Power calculation and speed search

P_req(V) = (R_induced + R_friction + Rw) × V / η / 1000    [kW]

The algorithm sweeps V in 0.5-knot increments from V_min to V_max, keeping the last V where P_req ≤ P_available. A fine refinement step (0.05 knots) is then applied around that point to improve accuracy. The search range for each regime:

RegimeV_minV_max
Displacement (ARWIMS & propeller)0 knV_hull × 1.5 (hard-capped at V_hull)
Hull + track planingmax(V_liftoff, 4 kn)100 kn
Track-only planingmax(V_liftoff × 1.3, 8 kn)120 kn
Propeller planing (ref)10 kn100 kn

The minimum speed for all displacement regimes is 0 knots. The minimum speed for planing regimes is the dynamic lift-off speed (or a practical lower bound), ensuring the regime only reports achievable conditions.

12. Limitations

Conclusion

The simulator demonstrates that the ARWIMS speed and fuel advantage arises from two compounding effects: (1) the effective lift-to-drag ratio of the paddle-track planing system (~11.4) is more than twice that of a conventional planing hull (~5.0), because the paddles add lift at near-zero drag cost while the flat track bottom run provides the primary planing surface; and (2) the wetted area at full planing is reduced to the sole track bottom runs, eliminating the hull bottom friction entirely in track-only mode. The propulsive efficiency of the track system (η ≈ 0.87) is also higher than a propeller at displacement speeds (η = 0.50).


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Model version: v2.1 — June 11, 2026