Summary

Frederick William Lanchester Aerodynamics, constituting the first volume of a complete work on aerial flight… (1906)

If we cast aside the mythology introduced into the subject by the light radiation specialists, and treat the question as it should be treated, as a matter of ordinary dynamics, it is evident that it is the displacement of matter (if any) that gives rise to the momentum of a wave, and it is the momentum of the wave that gives rise to the pressure at reflection, and by equating the two, as has been done in the foregoing demonstration, we have the simplest known method of obtaining the expression for the velocity of sound.
Source: Wikisource

Frederick William Lanchester Aerodynamics, constituting the first volume of a complete work on aerial flight… (1906)

Without discussion of the means whereby the bird operates to play off one portion of the wind against another, we may, from the above considerations, form an outside estimate of the available energy. Thus if we prescribe some conventional form as representing the motion of turbulence, such as a simple harmonic motion in the line of flight, or a compound harmonic or circular motion of known velocity, we can calculate the turbulence energy per unit volume, and we may convert this into a thrust force per unit area of the stratum of air handled
Source: Wikisource

Frederick William Lanchester Aerodynamics, constituting the first volume of a complete work on aerial flight… (1906)

The extra energy can only be accounted for by supposing that there is a pressure against the reflector, that work has to be done in pushing it forward. . . . A similar train of reasoning gives us a pressure on the source, increasing when the source is moving forward, decreasing when it is receding.
Now it is evident that the whole of this reasoning rests on the assumption that the reflector, while impervious to the waves, is freely pervious to the medium; [18] an assumption that may be true in the case of light, but is certainly not true in the case of sound.
Source: Wikisource

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