Quantitative Relationships

It has been found that, if the optical readings from the Tyndall meter are plotted as ordinates against the time t (the time elapsed after detonation) as abcissas, and that portion of the curve between t = 0 and t = 30 considered, the curve generally descends sharply at first, from a high point representing the density immediately after the production of the smoke, to a point in the neighborhood of t = 8, where it flattens out and descends much more slowly with a slope that changes little. The area under the significant portion of the curve, that is, the area circumscribed by the curve from the point t₃₀ to t₀, the vertical axis from this point to the origin, the horizontal axis from the origin to t₃₀ and the line perpendicular to this axis, cutting the curve at t₃₀, is a rough measure of the relative values of different smokes. This area is calculated as the sum of two rectangles, from t₀ to t₈ and from t₈ to t₃₀.

Some results are as follows:

Area 30
Phenyldichloroarsine181
Triphenyldichloroarsine  178
Diphenylcyanoarsine137
Diphenylchloroarsine101
Cyanogen bromide 94
Methyl dichloroarsine 70
Phenylimidophosgene 69
Mustard gas 38

The curves in [Fig. 101] show the way in which the readings fall off with time. Each substance of course has its characteristic curves.

Fig. 101.—Typical Curves Showing the Decrease
in Concentration of Smoke Cloud with Time.

Toxic Materials

The selection of materials for the production of toxic smokes can only be carried out experimentally. A number of very toxic substances have been shown to be valueless as toxic smokes because of low penetration, decomposition during the process of smoke production, or for other reasons.

Arsenic compounds produce smokes distinctly better than the average. Inorganic compounds which have high melting and boiling points are very poor smoke producers. The only exception to this is magnesium arsenide, which may suffer decomposition. Compounds like mercuric chloride and arsenic tribromide, which boil or sublime at comparatively low temperatures, produce good smokes. Most materials which boil below 130° C. produce no smoke as they evaporate on dispersion. It is difficult to set any upper limit for the boiling point beyond which materials do not produce good smokes, but in all probability 500° C. is not far from the maximum. Liquids and solids are, on the whole, almost equally good as smoke producers. The physical condition of the material has no great effect upon the amount of smoke which it will produce. This seems to depend only upon the physical and chemical properties of the material.