Particle — where it appears
Named by 4 essays across 3 fields — each of them below, with the objects they name alongside it.
A force without the flow that makes it
A sphere carried along by a flow does not travel at the speed of the fluid at its centre. It travels at the average of the flow over its own surface — and getting that result needs no solution of the flow around the sphere at all, only the answer to a completely different problem that everybody already knows.
The curve that measures a gradient
Three of the four curves drawn through a flow answer the same question — where did the fluid go. The fourth answers a different one. A line of particles released together is displaced by the local velocity and by nothing else, so its shape is the velocity profile, and dividing the elapsed time back out returns that profile exactly rather than approximately.
The drag that integrates a whole history
A particle released in still air does not stop exponentially. The unsteady drag on it carries a term that is an integral over everything the particle has already done, weighted by the inverse square root of how long ago — so there is no time constant, and five particle time constants later it is still moving four times faster than the quasi-steady answer allows.
A particle is a low-pass filter
A seeding particle does not report the flow; it reports the flow through its own transfer function. At a Stokes number of one it follows 71 per cent of the motion and lags it by 45 degrees, and a fifty-micron droplet at a kilohertz is following two per cent of what it is supposed to be measuring.
Named alongside it
The objects these essays reach for when they reach for this one.
MeasurementConvolutionInstrumentMemory kernelModel validityRegimeRelaxation timeStokes flowAdded massBoundary conditionBoundary layerCreeping flow