CHAPTER VI.

INCANDESCENT BURNERS.

A review of gas-burners would scarcely be complete without some

reference to the incandescent burners of M. Clamond and Mr. Lewis.

Although their dependence upon an artificially produced blast or

current of air removes them from the list of appliances applicable to

ordinary conditions, the remarkable results which they afford, not

less than their originality, demand for them at least a passing

notice. The production of light by the agency of these burners is

brought about in a manner altogether different, and is due to quite

other causes than those which are concerned in the production of an

ordinary illuminating gas flame. In the latter case, the illuminating

power developed is solely due to the hydrocarbons contained in the

gas, which are decomposed by the heat of the flame, the separated

carbon being raised to a white heat. In the former, the illuminating

power is not obtained directly from the gas; but advantage is taken of

the heat of the flame, enhanced by the application of a blast of air,

to raise to incandescence some refractory foreign material, which

latter is thus made to give out light. In the Clamond burner this

refractory substance is a basket composed of magnesia, spun into

threads; in the Lewis burner it is a cage of platinum wire.

To the unthinking reader it may perhaps appear somewhat surprising

that results so remarkable as are yielded by these burners should be

obtained, while disregarding, as a source of light, the hydrocarbons

contained in gas, and employing them, in common with the other

constituents, solely as a source of heat. An explanation, however, is

readily forthcoming. As was shown in a former part of this

treatise,[16] the great bulk of ordinary coal gas consists of

constituents which, in the act of combustion, produce considerable

heat, but scarcely any light; the illuminating power developed in an

ordinary gas flame being almost wholly dependent upon the very small

proportion of heavy hydrocarbons which the gas contains. Thus, the

quantity of heat-producing elements contained in the gas being quite

disproportionate to the light-yielding hydrocarbons, there is always

produced, in an ordinary gas flame, more heat than is necessary for

effectively consuming the free carbon, which is liberated in the flame

by the decomposition of the heavy hydrocarbons. This is shown by the

fact that coal gas can usually be naphthalized--that is, impregnated

with the vapour of naphtha--to a considerable extent before the limit

of effective combustion is reached. The object aimed at in the

incandescent burners about to be described is to utilize, in the

development of illuminating power, the combined heat produced by the

combustion of all the constituents of the gas. To this end the heat

of combustion is brought to bear upon, and caused to raise to

incandescence, some refractory material, extraneous to, but brought

within the operation of the flame.

[16] See Chap. II., p. 21.

[Sidenote: Effect of injecting a blast of air into a gas flame.]

A further explanation of the superior results yielded by these burners

may be found in the employment of an artificial blast or current of

air. Indeed, without some such arrangement the desired end could not

be attained. The heat developed by the unaided flame is diffused over

too wide an area to raise the temperature of the heated substance to

the necessary degree of incandescence to enable it to give out

sufficient light. By injecting a current of air into its midst, the

flame is condensed into a smaller compass; and is brought to bear more

directly upon the precise locality where its heat may be most

effectively employed. Thus, although the total quantity of heat

developed remains exactly the same as before, it is concentrated upon

a smaller surface of the refractory substance; and the latter is

consequently more intensely heated, or, in other words, raised to a

more exalted temperature. The very superior illuminating power which

is thereby obtained is due to the circumstance that the quantity of

light yielded by an incandescent body increases in a higher ratio than

the temperature to which it is raised.

[Sidenote: Lewis's incandescent gas-burner.]

Proceeding now to describe the burners. The one invented by Mr. Lewis

(various forms of which are illustrated on the next page) consists of

an upright tube, connected at its base to the gas supply, and

surmounted by a cap or cage of platinum wire gauze; which latter

constitutes a combustion chamber, as it is there that the mixture of

gas and air is consumed. Into the lower part of the upright tube the

nozzle of an air-pipe is inserted, through which a supply of air can

be injected, under pressure, into the burner, after the manner of a

blowpipe. There are also small branch tubes leading into the upright

gas-tube, and open to the atmosphere. Through these an additional

quantity of air enters the burner; being drawn or sucked in by the

agency of the main current, which flows through the upright tube. The

resemblance to an ordinary Bunsen burner is, therefore, very close.

The mixture of gas and air thus produced, when ignited, burns at the

platinum cap; the heat which is developed causing the latter to become

highly incandescent, and so to give out a brilliant light. To prevent

the conduction of heat from the incandescent platinum, through the

upright tube, a non-conducting material--such, for instance, as

steatite or porcelain--is interposed between the gauze cap and the

metal tube.

[Illustration: FIG. 26.--LEWIS'S INCANDESCENT GAS-BURNER.]

The light produced by this burner is said to approximate more closely

to daylight than that yielded by an ordinary gas flame (the colours of

textile fabrics, for instance, being shown as well by its aid as by

daylight); while, on account of its resulting from the incandescence

of a fixed body, instead of being emitted from a flame, it is

unaffected by a gust of wind, and maintains perfect steadiness under

every condition of weather. The illuminating power developed is stated

to be equal to 5 standard candles per cubic foot of gas consumed.

[Sidenote: Clamond's incandescent gas-burner.]

M. Clamond's burner, which is shown in fig. 27, is a much more

complicated apparatus than the preceding one, and not so easily

described; but its main features may be briefly enumerated as

follows:--The air (which, as in Mr. Lewis's burner, is supplied under

pressure) is divided, as it enters the apparatus, into two portions.

One portion is at once mixed with the gas; the remainder being

conveyed, through a peculiarly constructed tube composed of small

pieces of refractory material, to the combustion chamber, or "wick,"

as it is termed, of the burner. This "wick" is a small conical basket,

made of a kind of lacework of spun magnesia, which, when raised to

incandescence by the heat produced by the combustion of the gas,

furnishes the desired illumination. The mixture of gas and air is

subdivided, by a "distributor," into two portions, one of which goes

direct to the magnesia "wick," there to be burnt, while the other is

distributed among a number of tubes, forming so-called "auxiliary

burners," the flames of which are utilized to heat the chief air

supply; being directed upon the sides of the before-mentioned tube of

refractory material, through which it is conveyed. By this means the

air is raised to a very high temperature (1000 deg. C., or 1800 deg. Fahr., it

is said) before it impinges upon the flame. The result is the

production of a most intense heat within the magnesia basket; the

latter being raised to brilliant incandescence, and so developing a

high illuminating power.

[Illustration: FIG. 27.--CLAMOND'S INCANDESCENT GAS-BURNER.]

The magnesia basket must be renewed after being in use a period of

from 40 to 60 hours, as it gradually deteriorates by the action of the

intense heat to which it is subjected; but as the cost is said to be

insignificant, this should not be a great drawback. The basket is

placed at the base of the burner, in order to obviate the shadow which

would otherwise be cast by the apparatus; and it is attached to the

main body of the apparatus by platinum wires. As to illuminating

power, the only particulars which have been made public refer to the

first two models constructed; one of which was said to develop a light

equal to that from 6.208 candles, and the other to 9.72 candles per

cubic foot of gas consumed.

[Illustration: FIG. 28.--CLAMOND'S IMPROVED INCANDESCENT BURNER.]

[Sidenote: Clamond's new burner.]

In a recently designed modification of the burner (which is shown in

the accompanying illustration) M. Clamond dispenses with an artificial

supply of air under pressure, and endeavours to obtain similar results

by other and simpler means. To this end the position of the magnesia

"wick" is reversed (it being placed at the top of the apparatus); the

current of gas is allowed to draw in upon itself a quantity of air by

a precisely similar arrangement to that adopted in the Bunsen burner;

while an additional supply of air is drawn upon the flame by the

accelerated draught produced by the aid of a glass chimney. As in the

more complicated and complete burner, the air supply is heated by

means of auxiliary burners in the interior of the apparatus. It has

been stated, on the authority of M. Clamond, that this modified burner

develops, from the gas consumed, a duty of about 6 candles per cubic

foot; being equal to the results yielded by the more complicated

apparatus. Should this be borne out in practice, M. Clamond will

have achieved a noteworthy success. It is, however, advisable to

reserve expressing any definite opinion of its merits until further

information is received, or until the burner has been tried in this

country.

Gas Burners Old and New A historical and descriptive treatise on the progress of invention in gas lighting, embracing an account of the theory of luminous combustion · 第 6 / 7 章