BAYLE'S LAMP CHIMNEY.

The different types of lamps used in domestic lighting present several

imperfections, and daily experience shows too often how difficult it is,

even with the most careful and best studied models, to have a perfect

combustion of the usual liquids--oil, kerosene, etc.

[Illustration: BAYLE'S NEW LAMP CHIMNEY.]

Mr. P. Bayle has endeavored to remedy this state of things by experiments

upon the chimney, inasmuch as he could not think of modifying the

arrangements of the lamps of commerce "without injury to man" interests,

and encountering material difficulties.

The chimney is not only an apparatus designed to carry off the smoke and

gases due to combustion, for its principal role is to break the

equilibrium of the atmospheric air, which is the great reservoir of

oxygen, and to suck into the flame, through the difference of densities,

this indispensable agent to combustion. The lamps which we now use are

provided with cylindrical chimneys either with or without a shoulder at

the base. The shouldered chimney would be sufficient to suck in the

quantity of air necessary for a good combustion if we could at will

increase its dimensions in the direction of the diameter or height. But,

on account of the fragile nature of the material of which it consists, as

also because of the arrangement of the lighting apparatus, we are forced

lo give the chimney limited dimensions. The result is an insufficient

draught, and consequently an imperfect combustion. It became a question,

then, of finding a chimney which, with small dimensions, should have great

suctional power. Mr. Bayle has taken advantage of the properties of

convergent-divergent ajutages, and of the discovery of Mr. Romilly that a

current of gas directed into the axis and toward the small base of a

truncated cone, at a definite distance therefrom, has the property of

drawing along with it a quantity of air nearly double that which this same

current could carry along if it were directed toward a cylinder. In

getting up his new chimney, Mr. Bayle has utilized these principles as

follows: Round-burner lamps have, as well known, two currents of air--an

internal current which traverses the small tube that carries the wick, and

an external one which passes under the chimney-holder externally to the

wick. In giving the upper part of the chimney, properly so called, the

form of a truncated cone whose smaller base is turned toward the internal

current of air, that is to say, in directing this current toward the

contracted part of the upper cone, at the point where the depression is

greatest, a strong suction is brought about, which has the effect of

carrying along the air between the wick and glass, and giving it its own

velocity. The draught of the two currents having been effected through the

conical form of the upper part of the chimney, it remained to regulate the

entrance of the external current into the flame. If this current should

enter the latter at too sharp an angle, it would carry it toward the mouth

of the chimney before the chemical combustion of the carbon and oxygen was

finished; and if, on the contrary, it should traverse it at too obtuse an

angle, it would depress and contract it. Experience has shown that in the

majority of cases the most favorable angle at which the external current

of air can be led into the flame varies between 35° and 45°. We say in the

majority of cases, for there are exceptions; this depends upon the

combustive materials and upon the conditions under which they enter the

flame. The annexed figure shows the form adopted by the inventor for oil

and kerosene lamps. As may be seen, the chimney consists of two cones, A

and B, connected end to end by their small bases. The upper one, A, or

divergent cone, is constructed according to a variable angle, but one

which, in order to produce its maximum effect, ought not to differ much

from 5°. This cone rests upon the convergent one, B, whose angle, as we

have said, varies between 35° and 45°. To the large base of this cone

there is soldered a cylindrical part, c, designed for fixing the chimney

to the holder. The height given the divergent cone is likewise variable,

but a very beautiful light is obtained, when it is equal to six times the

diameter of the contracted part. When the lamp is designed to be used in a

still atmosphere, free from abrupt currents of air, the height may be

reduced to four times the diameter of the base, without the light being

thereby rendered any the less bright. As for the height to be given the

convergent cone, B, that is determined by the opening of the angle

according to which it has been constructed. Finally, as a general thing,

the diameter of the small base should be equal to half the large base of

the convergent cone, B.

The new chimney should be placed upon the holder in such a way that the

upper part of the wick tube, D, is a few millimeters beneath the base of

the convergent cone. The height to be given the wick varies according to

the lamp used. It is regulated so as to obtain a steady and regular

combustion. In oil lamps it must project about 1½ centimeters. If two

lamps of the same size be observed, one of which is fitted with the new

chimney and the other with the old style, we shall be struck with the

difference that exists in the color of the flame as well as in its

intensity. While in the case of the cylindrical glass the flame is red and

dull, in that of the circuit it is white and very bright. This, however,

is not surprising when we reflect upon the theoretical conditions upon

which the construction of the new chimney is based--the strong influx of

air having the result of causing a more active combustion of the liquid,

and consequently of raising to white heat the particles of carbon

disseminated through the flame. As it was of interest to ascertain what

the increase of illuminating power was in a given lamp provided with the

new chimney, Mr. Felix le Blanc undertook some photometric experiments.

The trials were made with a Gagneau lamp provided with a chimney of the

ordinary shape, and then with one of Mr. Bayle's. The measurements were

made after each had been burned half an hour. The light of the standard

Carcel lamp being 1, there was obtained with the Gagneau lamp with the

ordinary chimney 1.113 carcels, and with the Bayle chimney 1.404 carcels.

Thus 1.113:1.404 represents the ratio of the same lamp with the ordinary

chimney and with that of Bayle. Whence it follows that the light of the

lamp with the old chimney being 1, that with the new one is 1.26, say an

increase of about 25 per cent. There is nothing absolute about this

figure, however. On kerosene lamps the new chimney, compared with the

contracted Prussian one, gives an increase of 40 per cent. in illuminating

power, and the oil is burned without odor or smoke.

As it was of interest to see whether this increase in intensity was not

due to a greater consumption of oil, a determination was made of the

quantity of the latter consumed per hour. The Gagneau lamp, with the old

chimney, burned 62.25 grammes per hour, and with the Bayle 63 grammes in

the same length of time.

It may be concluded, then, that the increase in light is due to the

special form given the chimney. This new burner is applicable to gas lamps

as well as to oil and petroleum ones.

The effects obtained by the new chimney may be summed up as follows:

increase in illuminating power, as a natural result of a better

combustion; suppression of smoke; and a more active combustion, which

dries the carbon of the wick and thus facilitates the ascent of the oil.

The velocity of the current of air likewise facilitates the action of

capillarity by carrying the oil to the top of the wick. Moreover, the

great influx of air under the flame continually cools the base of the

chimney as well as the wick tube, and the result is that the excess of oil

falls limpid and unaltered into the reservoir, and produces none of those

gummy deposits that soil the external movements and clog up the conduits

through which the oil ascends. Finally, the influx of air produced by this

chimney permits of burning, without smoke and without charring the wick,

those oils of poor quality that are unfortunately too often met with in

commerce.--_La Nature._

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Scientific American Supplement, No. 458, October 11, 1884 · 第 16 / 41 题