Wind Turbine Aerodynamics - 5b - Unsteady Momentum Model
18 August 2026, Galih Bangga
Unsteady BEM
- unsteady inflow, unsteady excitation: $u, v, w = f(x, y, z, t)$
- apply corrections to standard BEM theory
- get correted output: $a, a' = f(x, y, z, t)$
Dynamic Wake
- unsteady flow phenomena in the inflow affecting the rotor loads:
- gusts
- yaw misalignment
- control actions, e.g. pitching, yawing
- wake reacts delayed to inflow changes
- BEM ist steady, but unsteadyness can be added
- dynamic inflow model can predict the delay for the wake
Approach to calculate the induced velocity on slide 11
Yaw Misalignment
- incoming flow is not aligned with rotor axis
- wake is not aligned with free wind direction
- azimuthal variation of induced velocities:
- induced velicity is larger when wind turbine blade points downstream because it is deeper in the turbine wake
- induced velocity is smaller when wind turbine blade points upstream
- upstream blade sees higher wind velocities leading to higher loads