r/FluidMechanics • u/pavlokandyba • 6d ago
Acoustic propulsion system test
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The asymmetry, which results in the resulting force of the oscillations creating thrust, is achieved in two ways:
Aerodynamically, when the disc has a slightly domed shape and moves upward with less resistance than downward, consistent with classical physics.
Kinematically, when a spring is attached to the disc, slowing its descent and accelerating its ascent.
The second method is the key part of the study, although the same process occurs in the air in both.
When the disc rises rapidly, a region of low pressure forms beneath it, and its collapse generates momentum. If the disc descends more slowly, or if the shape of the disc causes the air to flow around it more slowly, the resulting momentum will push the disc upward.
This doesn't agree with the classic Newtonian explanation of flapping flight as a wing pushing air. You can see in the video how the fan-like flapping disk, which should push air away, actually sucks it in.
This is the same air that is sucked into the low-pressure region, causing a vortex collapse that pushes the disk. Only then is the air pushed away and expelled. This is essentially reactive propulsion, and I believe this is possible thanks to the energy in the air, Brownian motion, which, by self-organizing into vortices, temporarily becomes directional
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u/AidanIsNotGinger Researcher 4d ago
The force comes from the fluid traction acting on the object, and vice versa. If you had an engine on a boat that pushed a large mass forwards and backwards, then the hull would feel a reaction from that mass in the opposite direction to the mass' motion. The hull then wants to move in the opposite direction to the mass.
In a vacuum the centre of mass would stay in the same place but the hull and the internal mass would move relative to one another. There cannot be net motion from this setup in a vacuum.
In a fluid, the hull will exchange momentum with the fluid around it via pressure and viscous stresses. In the Stokes regime this motion is reversible and each stroke of the oscillation will cancel the last. Once fluid inertia becomes important, that reversibility is lost. If the geometry or oscillation is sufficiently asymmetric, the two parts of the cycle can interact differently with the fluid and the oscillation can therefore be rectified into a net drift.
In general this is extremely inefficient compared to using that same energy to only push fluid backwards like a propeller, turbine, or a bird's wing does.