Scientific American Supplement, No. 430, March 29, 1884Various
Science
Scientific American Supplement, No. 430, March 29, 1884
Various
Science -- Periodicals
"The diameter of the mixing tube is a matter of importance, as it
rules the quantity of gas which can be satisfactorily burnt in any
arrangement. With large flames, given a certain size of gas-jet, the
diameter of the mixing-tube should be not less than ten times as great.
For instance, at 1 inch pressure, a jet having a bore of 1/8 inch will
pass about 20 cubic feet of gas per hour. To burn this quantity of gas,
a mixing tube is necessary 10/8 or 1¼ inch in diameter. By the first
rule this tube must be in length equal to four and a half times its
diameter, or 5-5/8 inches. It would appear that the mixing-tube, having
100 times the area of the gas jet, is out of all proportion to the size
necessary for obtaining a mixture of one of gas to nine or ten of air;
but it must be remembered that the gas is supplied under pressure. It is
therefore evident that no mere calculation of areas can be taken,
into account, unless the difference in pressure of the supply is also
considered. A complete reversal of this law is shown in that ruling the
construction of blowpipes, which I have already given in a previous
paper on 'The Use and Construction of the Blowpipe.' In these the air
supply, being under a heavier pressure, is much smaller in area than
the gas inlet; and, to obtain maximum power, the air-jet requires to be
enlarged in proportion to the gas pressure.
"Given a certain area of tube delivering a combustible mixture, the
outlet for this mixture must be neither more nor less than the size of
the tube. Taking an ordinary drilled tube, such as is commonly made, and
of the dimensions before given--i. e., 1¼ inch bore--if the holes are
drilled 1/8 inch in diameter the tube will supply 10 x 10 = 100 of these
holes. In practice this rule may be modified.
"The variations from the rule, however, must be a matter of experience
with each form of burner. There is also the fact that with small divided
flames it is not necessary to mix so large a proportion of air, as each
flame will take up air, on its external surface; but in this case the
flames are longer, hollow, and of lower temperature. As a matter of
actual practice, where a burner is used which gives a number of flames
or jets, the diameter of the mixing-tube does not need to exceed eight
times the diameter of the gas jet; the remainder of the air required
being taken up by the surfaces of the flames.
Public-domain text, read in full here on John Shaqi.
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