Summary

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

We thus see that changes in the shape of a body of a fluid, such as take place in the course of its passage through a "tube of flow" in the vicinity of a streamline body, are resisted by viscosity in proportion to the velocity with which the change of form takes place, and the work done on the fluid in this manner must be supplied by a propulsive force; that is to say, the body will be resisted in its motion through the fluid from the cause stated. We have here one of the causes of viscous resistance.
Source: Wikisource

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

If, when the velocity V increases, we suppose that the layer of fluid affected to any given degree becomes thinner, and vice versa, it is clear that the viscous forces will rise in a greater ratio than directly as V, for the velocity gradient will be steeper, also the inertia forces will be less, for the mass of fluid to be set in motion will be less. It is, therefore, evident that we may suppose the thickness of the affected strata varies with the velocity in the degree necessary to preserve a balance between the viscous and inertia forces.
Source: Wikisource

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