Rotor — where it appears
Named by 4 essays across 3 fields — each of them below, with the objects they name alongside it.
The cushion that is there after all
A wing near the ground makes more lift for reasons that have no cushion in them, and that account cannot reach two cases — a wing descending, and a rotor in the hover, where there is no steady flight for the image-vortex account to be about. Those cases have a term that really is about carried air, and it grows without limit as the gap closes.
The stress that picks the aerodynamics
The free term in a rotor's pressure rise wants radius and speed, and both are capped by something with no fluid in it. Integrate a blade's own weight outward and the root stress comes out as the annulus area times the square of the shaft speed — with the chord cancelled, the blade count cancelled, and every property of the gas cancelled.
A blade that flies through what it shed
A rotor blade meets the tip vortex the blade in front of it left, a fifth of a second earlier, at a few per cent of the radius. What it feels is a doublet — five and a half degrees of upwash and then five and a half of downwash within a few chords — and the peak goes as one over the miss distance.
The inflow that takes time to arrive
Momentum theory gives a rotor's induced velocity from its thrust, instantly. It does not arrive instantly: the air the disc has to accelerate has a mass, and the response is a first-order climb with a time constant of 33 milliseconds — a twentieth of the time the wake itself takes to convect a radius.
Named alongside it
The objects these essays reach for when they reach for this one.
Added massBlade-elementCorrelationInduced velocityMemory kernelModel limitModel validityRegimeActuator discAnnulusCirculationControl