Scientific American Supplement, No. 561, October 2, 1886Various
Science
Scientific American Supplement, No. 561, October 2, 1886
Various
Science -- Periodicals
Fig. 8 shows a double flame burner on the principle of Mr. Heron's,
but with admission of hot air into the angle formed by the flames. As
exemplified by Mr. Heron, if two equal batswing burners separately
give a certain amount of light, on the two flames being brought into
contact, so as to form a single flame, the luminosity is considerably
increased, owing to the condensation of heat which results from their
meeting. The two incandescent sheets are, as it were, forced into one
another, so as to be combined.
[Illustration: FIG. 8. DOUBLE FLAT-FLAME BURNER]
The high-power burners of Douglass, Coze, Mallet, and others were
designed on this principle; but its application to uninclosed burners
was not very satisfactory, because the great cooling down of the inner
surface of the flames by the strong draught of cold air impaired their
illuminating power. To counteract this difficulty, M. Somzee adopts a
heating burner, A, which he places between the two batswing burners,
B, so that the products of combustion rise in the angle made by the
two lighting flames, as shown; thus greatly increasing their
luminosity while maintaining a low consumption of gas.
M. Somzee also raises the illuminating power of an ordinary flat-flame
burner by causing an obscure effluvium to traverse the dark portion of
the flame. The effect of this is to increase the activity of
decomposition in this portion, so that the particles of carbon are the
more readily set free, and remain longer in suspension in the luminous
zone. The obscure effluvium may be determined between two points by
the electric current, or be caused by the heating of an imperfect
conductor by the current; or, again, it may result from a metal
conductor heated by the reactions produced in the middle of the flame,
by separating the cone of matter in ignition. The effect may be
compared with that obtained by the concentration of two sheets of
flame; but in this case the sheets are formed by the constituent parts
of one and the same flame, whence results a more complete utilization
of the elements composing it. This system is, in fact, a
simplification of the arrangement adopted in the double-flame burner
seen in Fig. 8.
Fig. 9 shows a reflecting and regenerative burner with double glass.
The crown, made of metal polished on both sides, has a circular
groove, G, for receiving the end of the central chimney, C, and
presenting an annular aperture by which the products of combustion
enter. The second glass, C¹, is fastened to the collar of the
burner carrier, and does not come into contact with the metal crown;
so as to allow the air to enter from outside for supplying the burner.
The gas enters by the pipe, T, provided with a cock. This pipe is
continued to the top of the apparatus, and there spreads out into the
form of a dome; thus dividing into two compartments the trunconic
chamber, S¹ S squared, whence the hot gas returns to the body of the burner,
B.
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Elsewhere in the archive
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account