Scientific American Supplement, No. 1082, September 26, 1896 — John Shaqi
Scientific American Supplement, No. 1082, September 26, 1896Various
Science
Scientific American Supplement, No. 1082, September 26, 1896
Various
Science -- Periodicals
A description of the Auer burner will not be expected from us. It is
now so widely employed as to render a new description useless. As an
offset we think that our readers will be more interested in a
description of the Denayrouse burner, the industrial application of
which has but just begun. This burner has been constructed in view of
the best possible utilization of the gas, in approaching a complete
theoretical combustion. In order that it may give its entire
illuminating power, gas, as we know, must be burned in five and a half
times its volume of air. In the Denayrouse burner the gas burns in
four and four-tenths its volume of air. The result reached is,
consequently, very appreciable.
[Illustration: SECTION OF THE LAMP.
A, entrance for the air; G, entrance for the gas; V, mixer; M,
electric motor.]
The apparatus consists essentially of a bronze or brass box in which
revolves a fan keyed upon an axle that passes through the box. The
axle is revolved by means of a small electro-magnetic machine mounted
upon one of the external sides of the box. The motor may also be a
hydraulic or compressed air one. Upon the axle is arranged a speed
regulator. The air enters at the bottom of the box and the gas at the
center. The exit of the mixture takes place through a chimney arranged
at the top and to which is fixed a luminous mantle. The apparatus
operates as follows: The motor causes the fan to make about 1,200
revolutions a minute. There is thus formed a strong draught of air,
which mixes with the gas that enters at the side. The ignition occurs
at the upper aperture of the chimney.
Although in this competition of gas and electricity the intensity of
the light and, its quality are important factors, it is certain that
what will decide the victory will be the price. This is why we are
going to establish the net cost of the different lights; for, although
up to the present the contest has seemed to be limited to gas and
electricity (oil and kerosene not being capable of having any other
pretension than to preserve their position), a new
competitor--acetylene--will perhaps soon put gas manufacturers and
electricians in accord, to the great benefit of the public, by
furnishing a brilliant light at a price that defies competition.
[Illustration: THE DENAYROUSE LAMP.]
In all systems of lighting, save electricity, the unit of light is the
carcel. This represents the light produced for one hour by 10 wax
candles, or, better still, it is the illuminating power given by the
combustion of 42 grammes of pure colza oil for one hour in what is
called a carcel lamp.
In electricity we count by watts. The watt, like the kilogrammeter, of
which it represents nearly a tenth, is not a unit of light, but a unit
of energy. What is called a kilogrammeter is the force capable of
lifting 1 kilogramme to 1 meter in height during 1 second. Further
along we shall estimate the watts in carcels.
Public-domain text, read in full here on John Shaqi.
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