The Mach cone — where it appears
Named by 2 essays across one field — each of them below, with the objects they name alongside it.
The note that changes on approach, and the two ways of getting it
A moving source and a moving listener produce different formulas for the same shift, because the medium is watching. The difference is small, real, and the reason light had to be treated differently.
The wave that arrives first by going the long way
A shot fired at the ground sends a wave straight along the surface layer to a distant listener, and another down to a faster rock beneath, along the boundary and back up. The second path is longer, and beyond a certain distance it arrives first, because most of it is run at the faster speed. Huygens's construction shows what the second wave is: a front drawn by wavelets that the disturbance racing along the faster floor sends up into the slower layer, the Mach cone of a source moving faster than the layer can carry sound. Reading where it overtakes the direct wave gave Andrija Mohorovičić the thickness of the Earth's crust in 1909, and gives every refraction survey since the depth to whatever lies beneath.
Named alongside it
The objects these essays reach for when they reach for this one.
Critical angleCrossover distanceDoppler effectFrequencyHead waveHuygens principleMohorovicic discontinuityRedshiftRefraction seismologyRelativistic dopplerTravel timeWave speed