Summary

Samuel Tolver Preston Application of the Kinetic Theory of Gases to Gravitation (1877)

Taking, therefore, the visible universe as a whole, we have no streams of particles, but simply a gas at rest. The streams only exist within the range of free path of the particles, or within the range of gravity. We may compare the medium filling the visible universe to the air of a room, in which there are no streams, but the air is as a whole at rest. Contract the room (in imagination) up to the range of free path of the molecules of air, and we have streams of molecules sweeping in all directions through the room.
Source: Wikisource

Samuel Tolver Preston Application of the Kinetic Theory of Gases to Gravitation (1877)

By making, therefore, the normal velocity of the particles of the medium sufficiently great, all perceptible resistance to the passage of bodies through it will disappear. It is as if the medium did not exist;it becomes quite impalpable, or its presence impossible to detect. This is consistent with observation. The amount of energy, or motion, abstracted from a body passing through the medium, and given up to the medium, is exactly measured by the resistance encountered by the body. It is this transference of energy to the medium that constitutes the "resistance."
Source: Wikisource

Samuel Tolver Preston Application of the Kinetic Theory of Gases to Gravitation (1877)

The old postulate of perfectly rigid molecules put a difficulty in the way of assuming that the molecules of a solid are in contact, because the "elasticity" (or compressibility within certain limits) of a solid could scarcely be reconciled with this postulate of perfectly rigid molecules, the dynamical theory of molecules put forward by Sir William Thomson, which explains the elasticity of a molecule by a simple motion of the matter forming it, enables us to explain the elasticity of a solid (with molecules in actual contact) by the elasticity of the molecules themselves.
Source: Wikisource

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