The Energy System of Matter: A Deduction from Terrestrial Energy PhenomenaWeir, James, active 1883-1912
Science
The Energy System of Matter: A Deduction from Terrestrial Energy Phenomena
Weir, James, active 1883-1912
Force and energy
energy in accordance with the decreased altitude of the particle. Since
the temperature of the column remains unchanged at the base surface and
only decreases in the ascent, it is clear that the entire heat and work
energy of the originally liberated gaseous mass is not expended in the
movement against gravity. Every gaseous particle--excepting those on the
absolute outer surface of the gaseous envelope--has still the property
of temperature. It is evident, therefore, that in the constitution of
the column, only a portion of the total original heat and work energy of
the gaseous substance is transformed into energy of position.
The space into which the gas expands has been referred to as unlimited
in extent. But although in one sense it may be correctly described thus,
yet in another, and perhaps in a truer sense, the space is very strictly
limited. It is true there is no enclosing vessel or bounding surface,
but nevertheless the expansion of the gas is restrained in two ways or
limited by two factors. The position of the bounding surface of the
spherical gaseous envelope depends, in the first place, on the original
energy of the gas as deduced from its initial temperature and its other
physical properties, and secondly on the value of the gravitative
attraction exerted on the gas by the planetary body. Looking at the
first factor, it is obvious that since the gaseous mass initially
possesses only a limited amount of energy, and since only a certain
portion of this energy is really available for the transformation, the
whole process is thereby limited in extent. The complete transformation
and disappearance of that available portion of the gaseous energy in the
process of erection of the atmospheric column will correspond to a
definite and limited increase of energy of position of gaseous material.
Since the energy of position is thus restricted in its totality, and the
mass of material for elevation is constant, the height of the column or
the boundary of expansion of the gas is likewise rigidly defined. In
this fashion, the energy properties of the gaseous material limit the
expansive process.
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