Calculations with context
ITTC-1957 friction-line estimate
Calculate Re, Fr, Cf and friction-line force/effective-power components with explicit reference lengths. Total ship resistance and engine power are not calculated.
ITTC-1957 friction-line estimate
See how water-relative speed, length, wetted area and viscosity determine a friction-only teaching estimate. This is one resistance component; it is not total ship resistance or required engine power.
Re = V LRe / ν · Fr = V / √(g LWL) · Cf = 0.075 / (log₁₀ Re − 2)² · RF = ½ρSV²Cf · PE,F = RF V
The initial result below is the synthetic/default teaching case.
| Quantity | Value | Unit |
|---|---|---|
| V | 10 | m/s |
| ν | 0.000001 | m²/s |
| Re | 1000000000 | 1 |
| Fr | 0.31932996 | 1 |
| ITTC-1957 coefficient Cf | 0.0015306122 | 1 |
| Friction-line force RF | 156.88776 | kN |
| Friction-only effective power PE,F | 1568.8776 | kW |
Physical interpretation
Substitution using these inputs
- V = 10 m/s
- ν = 1 × 10⁻⁶ = 0.000001 m²/s
- Re = 10 × 100 / 0.000001 = 1000000000
- Fr = 10 / √(9.80665 × 100) = 0.31932996
- Cf = 0.075 / (log₁₀(1000000000) − 2)² = 0.0015306122
- RF = ½ × 1025 × 2000 × 10² × 0.0015306122 = 156887.76 N
- PE,F = 156887.76 × 10 = 1568877.6 W
- PE,F − RF V = 0 W
Speed sensitivity
Only V is multiplied by 0.5, 0.75, 1, 1.25 and 1.5. LRe, LWL, S, ρ, ν and g are held fixed. Cf is recalculated at each speed. Unsupported Reynolds/speed points remain unavailable; lines do not bridge them.
| V × | V · m/s | V · m/s | Re | Fr | Cf | RF · kN | PE,F · kW | Status |
|---|---|---|---|---|---|---|---|---|
| 0.5 | 5 | 5 | 500000000 | 0.15966498 | 0.0016712645 | 42.826154 | 214.13077 | Calculated from the current inputs. |
| 0.75 | 7.5 | 7.5 | 750000000 | 0.23949747 | 0.0015867486 | 91.485973 | 686.1448 | Calculated from the current inputs. |
| 1 | 10 | 10 | 1000000000 | 0.31932996 | 0.0015306122 | 156.88776 | 1568.8776 | Calculated from the current inputs. |
| 1.25 | 12.5 | 12.5 | 1250000000 | 0.39916245 | 0.0014890959 | 238.48801 | 2981.1002 | Calculated from the current inputs. |
| 1.5 | 15 | 15 | 1500000000 | 0.47899494 | 0.0014564157 | 335.88587 | 5038.2881 | Calculated from the current inputs. |
The CSV is generated locally and includes inputs, units, assumptions, model version, sources, interpolation details, every supplied curve row and sensitivity rows where applicable. Extra digits describe arithmetic, not experimental accuracy.
Model and equations
Start by declaring what each input represents. V is speed relative to the water, not speed over ground. S is an entered wetted reference area; this page does not reconstruct a hull or change the area with trim, sinkage or speed. The Reynolds and waterline lengths are separate so that their physical meanings are visible.
Convert units before using the equations: 1 kn = 1 nautical mile per hour = 1852/3600 m/s exactly; 1 cSt = 10⁻⁶ m²/s exactly. Re compares inertial and viscous scales; Fr compares speed with √(gLWL). Both are dimensionless. They describe different aspects of similarity and are not interchangeable.
For a positive speed in the declared numerical window, evaluate the base-10 logarithm in the ITTC-1957 model–ship correlation line. Multiply Cf by dynamic pressure ½ρV² and wetted area to obtain RF. Multiplying that component by V gives the effective power associated with that component only.
Dimensional check: (kg/m³)(m²/s²)(m²) = kg·m/s² = N; N·m/s = W. At fixed geometry, density and viscosity, force is not exactly proportional to V² because Cf also changes with Re. Friction power is correspondingly not exactly proportional to V³.
The 1957 correlation line is not a universal flat-plate truth. Its historical formulation includes a correction relative to the Hughes line. No additional form factor k is fitted or applied here. A separately justified viscous form-factor model would require an explicit (1+k) term and still would not supply the missing wave, appendage or air contributions.
Symbols and units
| Symbol | Quantity | Unit |
|---|---|---|
| V | Water-relative speed | m/s |
| LRe / LWL | Reynolds reference length / waterline length | m |
| S | Entered wetted area | m² |
| ρ / ν | Density / kinematic viscosity | kg/m³ / m²/s |
| g | Gravitational acceleration | m/s² |
| Re / Fr / Cf | Reynolds number / length Froude number / correlation coefficient | 1 |
| RF | Friction-line resistance component | N |
| PE,F | Effective power for RF only | W |
Worked example
Load the 10 m/s example to reproduce every number: V = 10 m/s, LRe = LWL = 100 m, S = 2000 m², ρ = 1025 kg/m³, ν = 1 cSt = 10⁻⁶ m²/s and g = 9.80665 m/s². These are illustrative inputs, not measurements of a named vessel.
Re = 10 × 100 / 10⁻⁶ = 10⁹. Fr = 10 / √(9.80665 × 100) ≈ 0.319330. Because log₁₀(10⁹) = 9, Cf = 0.075/(9−2)² = 0.001530612245.
RF = ½ × 1025 × 2000 × 10² × 0.001530612245 ≈ 156887.755 N = 156.887755 kN. PE,F = 156887.755 × 10 ≈ 1568877.551 W = 1568.877551 kW. The engine rating cannot be inferred from this friction component.
Try doubling only S: RF and PE,F double, while Re, Fr and Cf do not change. Then double only LRe: Re doubles and Cf decreases, while Fr does not change. Changing only LWL affects Fr and leaves the friction calculation unchanged. These checks expose accidental mixing of the two length definitions.
Assumptions and limits
- Positive-speed calculations require 10⁶ ≤ Re ≤ 10¹⁰. This is a deliberately bounded teaching window, not an ITTC-certified validity interval. A scale-aware allowance of four machine epsilons handles floating-point rounding at these guard edges; the calculated Re is not clipped. Turbulent boundary-layer applicability must be justified independently; a large Reynolds number alone does not establish it.
- At V = 0, Re = Fr = 0 and RF = PE,F = 0 by the explicit stationary case. Cf is undefined and is not evaluated. Positive-speed cases below the window, including the singularity at Re = 100, are rejected rather than assigned a laminar or transitional formula.
- For Fr > 0.45 the output carries a scope warning. The cited resistance procedure addresses conventional displacement vessels; a friction-line number does not make this a planing or high-speed resistance method. Fr ≤ 0.45 also does not validate the missing physics.
- No wave-making, viscous-pressure/form-factor addition, appendage, air, roughness/fouling, shallow-water, acceleration, trim or sea-state resistance is included. No propulsive, hull, relative-rotative, shaft or transmission efficiency is assumed.
- The result cannot size an engine, establish available thrust, predict a sea trial or certify performance. Measured geometry, operating condition and appropriate resistance/propulsion methods are required for those tasks.
Primary sources
Public ITTC equations checked on 9 October 2026. This simplified workspace does not implement the complete test or extrapolation procedures.
- ITTC 7.5-02-02-01 Resistance Test, 2021 revision 05, §§2 and 3.6
- NIST SP 811, Chapter 5: knot and nautical mile
- NIST SP 811, Appendix B.8: centistokes and minute conversion factors
propulsion-teaching-1.0.1
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Related context
The method explanation and worked example are on this page. The articles below provide additional context.
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