Guide
Hull Wake and Propulsor Integration
A yacht propeller does not operate in uniform open water. The hull boundary layer, stern geometry and appendages create a three-dimensional wake at the propeller disk, making inflow quality central to propulsive efficiency, cavitation and vibration.
Published: Aug. 10, 2026
Last verified: Aug. 10, 2026
Open-water propeller data describes a propeller operating in a comparatively uniform inflow, but a propeller installed behind a yacht sees water already altered by the hull. Viscous boundary-layer development, pressure recovery around the stern and the presence of shafts, brackets, skegs and other appendages change both the magnitude and direction of velocity reaching the propeller disk. Propulsion integration therefore begins with the flow created by the yacht itself.
A nominal wake survey measures the velocity distribution at the intended propeller plane with the hull and relevant appendages represented but without the working propeller altering the flow. The resulting field shows where axial velocity is slower or faster than the vessel speed and where cross-flow or swirl exists. It gives the naval architect a detailed picture of the environment into which the propeller will eventually be installed.
Water close to the hull is slowed by viscous shear and forms a boundary layer that grows as flow moves aft. At the stern this lower-velocity water can occupy a substantial part of the propeller disk. Because propeller blade loading depends on local inflow velocity, a non-uniform boundary-layer wake causes each blade section to encounter changing conditions during every revolution.
An average wake fraction is useful in propulsive-efficiency calculations, but two sterns can have a similar average while producing very different circumferential distributions. A smooth wake creates more uniform blade loading. Sharp velocity deficits or strong cross-flow can create cyclic loads, cavitation and pressure fluctuations. Designers therefore examine the complete wake field rather than relying only on one averaged coefficient.
Afterbody fullness, buttock shape, transom immersion, tunnels, skegs and shaft exits influence how water turns and accelerates toward the propeller. Abrupt curvature can encourage separation, while well-developed stern geometry can deliver smoother flow. The best geometry is not simply the one that gives the lowest bare-hull resistance; the propeller must also receive an inflow that supports efficient and quiet operation.
Moving the propeller vertically, longitudinally or laterally changes which part of the stern wake it encounters. Clearance from the hull also affects pressure interaction and available propeller diameter. Twin-screw yachts introduce additional choices involving lateral separation, shaft angle and bracket geometry. Propeller location should therefore be established with wake information rather than inserted after the hull form has been frozen.
Shaft brackets, struts, stabiliser fins, skegs and other underwater components can create local velocity deficits, vortices and flow-angle changes. ITTC wake-testing guidance specifically recognises the need to represent appendages that influence propeller inflow. A clean bare-hull CFD result can therefore be misleading if the delivered yacht carries major appendages upstream of the propeller disk.
Once the propeller produces thrust, it accelerates water and changes pressure around the stern. The actual effective wake experienced by the working propeller is therefore not identical to the nominal wake measured without it. Hull and propeller interactions are represented through self-propulsion analysis and associated coefficients. This is why open-water propeller performance and nominal wake data need to be combined with an integrated propulsion prediction.
Wake surveys can measure velocity at the propeller disk in a physical model, while CFD can resolve detailed flow throughout the stern and identify the origin of velocity deficits or vortices. Self-propulsion calculations then include the working propeller or a suitable propulsor representation. Agreement between experimentally observed and numerically predicted flow improves confidence in the final design.
An efficient propeller cannot fully compensate for a badly distorted wake, and a low-resistance stern can still produce poor propulsion if the inflow is unsuitable. Hull shape, appendages, propeller location, diameter and loading therefore belong to one iterative design problem. Naval architecture creates the flow environment in which the propulsor must work, making wake quality a fundamental part of whole-yacht efficiency.
Sources and verification
Primary source: International Towing Tank Conference — Nominal Wake Measurement by LDV Model Scale Experiments
- ITTC Nominal Wake Measurement by LDV Model Scale Experiments — defines nominal wake measurement at the propeller disk and requires appendages capable of influencing propeller inflow to be represented in the model.
- USNA EN353 Resistance and Propulsion — covers resistance, propulsion-train efficiency, propeller operation, matching, cavitation and appendage resistance.
- ITTC Practical Guidelines for Ship Self-Propulsion CFD — provides current CFD guidance for integrated hull and propulsor calculations.
Wake fraction and propulsive coefficients depend on the hull, propeller, speed, loading condition, appendages and prediction method. Values from a different yacht or an isolated propeller should not be transferred directly to a new design.