Scientific American Supplement, No. 561, October 2, 1886 eBook

This eBook from the Gutenberg Project consists of approximately 141 pages of information about Scientific American Supplement, No. 561, October 2, 1886.

Scientific American Supplement, No. 561, October 2, 1886 eBook

This eBook from the Gutenberg Project consists of approximately 141 pages of information about Scientific American Supplement, No. 561, October 2, 1886.
the inner of the two concentric cylinders, which is heated to redness, and rises highly heated toward the upper annular burner, where the gas burns at a, a, a, in small separate flames, each entirely surrounded by the hot air.  This insures perfect combustion of the gas within the basket of magnesia placed above, and which is thus brought to a state of incandescence.  It will be seen from this description how simple and practical the arrangement is.  It is claimed for the light produced that it will stand comparison with the electric light.  Like that, it shows colors perfectly true, and will enable an observer to distinguish between the most delicate shades, allowing of the finest work being executed as by daylight.  It is, moreover, stated to be perfectly steady.  As the Clamond burner can be fixed to any gas bracket or lamp now in use, its adoption causes no other expense than the cost of the burner itself.  There is no expensive installation, and when used in combination with the electric light, it is claimed that a uniform lighting will be obtainable instead of the unpleasant contrast between gas and electricity.  Another important advantage obtained by the Clamond burner is the saving effected in the consumption of gas as compared with the same power of light obtained from ordinary burners.

* * * * *

A NEW THERMO-REGULATOR.

In the thermo-regulators which have been constructed heretofore, the heat has been regulated by the variation in the inflow of gas to the heating flame.  The apparatus described below, and shown in the accompanying cut, taken from the Zeitschrift fur Instrumentenkunde, operates on an entirely different principle.  The distillation and condensation process of a fluid heated to the boiling point in the vessel, A, is as follows: 

[Illustration]

The steam passes first through the pipes, a and c, into the serpentine tube, where it is condensed, and then flows through the tubes, d and b, back into the vessel, A, if the cock, r, is closed, but if the said cock is open, it flows into the receptacle, K. When the liquid begins to boil the steam passes freely through the tubes, d and b, part passing through the tube, f, out into the air, and the other part passing through the open cock, r, to the receptacle, K; but the condensed liquid soon closes these passages to the steam.  At h is an opening for a thermometer, t, and through this opening the liquid can be poured into the vessel, A. If the cock, r, is kept closed, the volume of liquid in the vessel, A, cannot be diminished, and the bath, B, must take the constant and uniform temperature of the steam in the vessel, A, as the vessel, B, is heated evenly on all sides.

This apparatus can also be used as an air bath, in which case the vessel, B, is left empty and closed by a suitable stopper.

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Scientific American Supplement, No. 561, October 2, 1886 from Project Gutenberg. Public domain.