CHAPTER XVI

SCREENING SMOKES

The intelligent use of screening smokes in modern infantry tactics

offers innumerable advantages through concealment and deception. It

confers upon daylight operations many of the advantages which were

gained by conducting operations at night with few of the disadvantages

of the latter.

Smoke screens have been frequently used by the Navy and by Merchantmen;

a common method of escape was to shut off the air from the fire with

consequent incomplete combustion of the fuel, thus causing a cloud of

dense black smoke. This is often mentioned in the blockade runners of

the days in the Civil War, where wood, high in pitch and rosin, was

freely introduced into the furnaces, in order that they might escape

under cover of this smoke.

Early in the present war it was found that black smoke had a low

obscuring power, showed frequent rents or holes and were difficult

to standardize. Their production also caused a considerable loss in

the speed of the vessel. They therefore fell into disuse except for

emergency purposes and today the standard smoke for screening purposes

of all kinds is, without exception, white.[33]

[Footnote 33: While it is a well known fact that black smoke is not as

efficient as white smoke for screening purposes, the reason for this

fact is not clear.]

PROPERTIES OF SMOKE CLOUD

The properties most desired in a screening smoke, apart from low cost,

are: (_a_) _Maximum screening power_, which refers to the question of

density, i.e., a relatively thin layer must completely obscure any

object behind it, and (_b_) _Stability_, which implies, among other

things, a low rate of settling or dissipation. There is little reason

to doubt that, within limits, the smaller the particles of a smoke

cloud, the more completely will the smoke possess these qualities.

The screening power of a smoke cloud depends very largely upon the

scattering of the light coming through it, and by analogy with those

peculiar solutions which we call colloidal, we should expect the

scattering to increase as the degree of subdivision increases, within

limits. The rate of settling is unquestionably an inverse function

of the size of the particles. The chief aim, therefore, in smoke

production is to attain as high a degree of subdivision as possible.

Methods may be classified as good or bad, in so far as they satisfy or

fail to satisfy this criterion.

RAW MATERIALS FOR SMOKE CLOUDS

It is obvious that only gases or substances capable of being brought

into the vapor state or into a very fine state of subdivision can be

used for producing smoke clouds. The reaction product, of which the

smoke particles consist, should preferably be:

(_a_) _Solid._ Otherwise the particles will tend to grow in size by

condensation of the liquid particles present in the cloud.

(_b_) _Non-volatile._ If volatile, the particles will disappear by

evaporation as the cloud is diluted by air currents. Larger particles

will also form at the expense of the smaller ones.

(_c_) _Non-deliquescent._ If the particles are deliquescent, they will

tend to grow by condensation of water vapor upon them.

(_d_) _Stable_ towards the usual components of the atmosphere,

especially moisture.

While it might seem that it would be difficult to fulfill these

conditions, there are several chemical compounds which have been

successfully used as smoke producers. This does not mean that they

fulfill all the conditions, but they represent a compromise between the

various requirements.

=Phosphorus.= One of the earliest materials to be used in smoke clouds

was phosphorus. This is prepared on a commercial scale by heating

phosphate rock (which contains calcium phosphate) with sand and coke

in an electric furnace. Phosphorus occurs in two forms, white and red.

_White phosphorus_, which is formed when the vapor of the substance

is quickly cooled, is, in the pure state, almost colorless, melts at

44° C., boils at 287° C., is readily soluble in various solvents, and

is luminous in the air, at the same time emitting fumes (the oxidation

product, phosphorus pentoxide). On gentle warming in the air, it takes

fire and burns with a brightly luminous flame. _Red phosphorus_ is

obtained by heating white phosphorus out of contact with the air, to a

temperature of 250° to 300° C. Red crusts then separate out from the

colorless liquid phosphorus, and almost the entire amount is gradually

converted into a red, solid mass. If this is freed by suitable solvents

from the small amounts of unchanged white phosphorus, a dark red powder

is obtained, which remains unchanged for a long time in the air, does

not appreciably dissolve in the solvents for white phosphorus, does

not become luminous, and can be heated to a fairly high temperature

without igniting. Further, red phosphorus is not poisonous, while white

phosphorus is highly so.

Either form burns to phosphorus pentoxide, which is converted by the

moisture of the air to phosphoric acid,

4P + 5O₂ = 2 P₂O₅

2P₂O₅ + 6H₂O = 4H₃PO₄

Since one pound of phosphorus takes up 1.33 pounds of oxygen and 0.9

pound of water, it is not surprising that phosphorus is one of the best

smoke producers per pound of material. Comparison of the value of the

two forms for shell purposes have invariably pointed to the superiority

of the white variety.

In addition to its use as a smoke producer, it is used in incendiary

shell and in tracer bullets. For incendiary purposes a mixture of red

and white phosphorus is superior.

=Chlorosulfonic Acid.= Chlorosulfonic acid, ClSO₂OH, was first

employed by the Germans to produce white clouds, both on land and on

sea. For this purpose, they sprayed or dropped it onto quicklime, the

reaction between it and the lime furnishing the heat necessary for

volatilization, though in this way about 30 per cent of the acid is

wasted.

Chlorosulfonic acid is obtained from sulfur trioxide and hydrogen

chloride, which combine when gently heated:

SO₃ + HCl = ClSO₂OH

[Illustration: FIG. 86.—75 mm. White Phosphorus Shell. 2 seconds after

bursting.]

On a commercial scale, hydrogen chloride is passed into 20 per cent

oleum, until saturation is reached. This is heated in a nitric acid

still, when the chlorosulfonic acid distills over between 150°-160° C.

With 30 per cent oleum, the conversion factor is about 42 per cent. The

residue in the still is about 98 per cent sulfuric acid.

It forms a colorless liquid, boiling at 152° C., and having a density

of 1.7.

Chlorosulfonic acid fumes in the air, because reaction with water forms

sulfuric acid and hydrochloric acid.

ClSO₂OH + H₂O = H₂SO₄ + HCl

This material was not used by the United States since oleum was found

superior.

=Oleum.= Oleum is a solution of 20 to 30 per cent sulfur trioxide

(SO₃) in concentrated sulfuric acid. It has been used by the Germans

to produce clouds on land and sea, by its contact with quicklime, and

by the Americans for screening tanks and aeroplanes. Sulfur trioxide

has been found to be superior as a shell filling. It is believed that

the smoke producing power of oleum is due solely to its sulfur trioxide

content, the sulfuric acid itself acting only as a solvent. The rather

high freezing point of the oleum containing high percentages of sulfur

trioxide is a disadvantage.

=Sulfur Trioxide.= Sulfur trioxide, SO₃, is a colorless mobile liquid,

which boils at 46° C. and solidifies to a transparent ice-like mass,

melting at 15° C. It is prepared by passing a mixture of sulfur dioxide

and oxygen over finely divided platinum or other catalysts at a

temperature between 400 and 450° C. Sulfur trioxide can only be used as

a filler for shell and bombs, and is probably the best substitute for

phosphorus.

=Tin Tetrachloride.= Tin tetrachloride, SnCl₄, is obtained by the

action of chlorine on metallic tin. It is a liquid, boiling at 114° C.,

and having a density of 2.2. It fumes in the air, because it hydrolyzes

to stannic hydroxide:

SnCl₄ + H₂O = Sn(OH)₄ + 4 HCl

It makes a better and more irritating smoke for shell and hand

grenades, than either silicon or titanium tetrachlorides. Since there

is practically no tin in this country, the other tetrachlorides were

developed as substitutes.

=Silicon Tetrachloride.= Silicon tetrachloride, SiCl₄, is prepared from

silicon or from impure silicon carbide by heating it with chlorine in

an electric furnace. The raw material (silicon carbide) is a by-product

in the manufacture of carborundum. It is a colorless liquid, boiling at

about 58° C., and fumes in moist air, owing to hydrolysis:

SiCl₄ + 4 H₂O = Si(OH)₄ + 4 HCl

It is not very valuable in shell, though it is more effective on moist,

cool days than on warm, dry ones. Its greatest use is found in the

smoke cylinder, combined with ammonia. By the action of the moisture of

the air, the following reaction takes place:

SiCl₄ + 4 NH₃ + 4 H₂O = Si(OH)₄ + 4NH₄Cl

The addition of a lachrymator gives a mixture which works well in hand

grenades for mopping up trenches.

=Titanium Tetrachloride.= Titanium tetrachloride, TiCl₄, is made from

rutile, TiO₂, by mixing with 30 per cent carbon and heating in an

electric furnace. A carbonitride is formed, which is said to have the

composition Ti₅C₄N₄, but the actual composition may vary from this to

the carbide TiC. This product is heated to 600-650° C., and chlorine

passed through, giving the tetrachloride. It is a colorless, highly

refractive liquid, which boils at about 136° C., is stable in dry air

and fumes in moist air. The best smoke is produced by using 5 parts of

water to one of the tetrachloride, instead of the theoretical 4 parts

[which would form Ti(OH)₄.] Since it is more expensive to manufacture

and not as effective as silicon or tin tetrachloride, it is used only

as an emergency material.

=Berger Mixture.= One of the most important smoke materials was the

zinc-containing mixture, which was used in the smoke box, the smoke

candle, certain of the smoke grenades and in various forms of colored

smokes. The basis of this was the _Berger Mixture_, which had the

composition:

Zinc 25

Carbon tetrachloride 50

Zinc oxide 20

Kieselguhr 5

This formula produced a light gray carbon smoke, with much carbon in

the residue. In this mixture the zinc and carbon tetrachloride react to

form zinc chloride and carbon; the kieselguhr keeps the mixture solid

by absorbing the tetrachloride, while the zinc oxide is practically

useless, as its absorbing power is small.

In order to accelerate the reaction and to oxidize the carbon, thereby

changing the color of the smoke from gray to white, an oxidizing

agent was added. Sodium chlorate was chosen for economic reasons. The

reaction now proved to be too violent, and the zinc oxide was replaced

by ammonium chloride. This cooled the smoke, retarded the rate of

burning and added to the density of the smoke, since the obscuring

power of the ammonium chloride is high. The kieselguhr was replaced by

precipitated magnesium carbonate, which is as good an absorbent, gives

a much smoother burning mixture, and also adds somewhat to the density

of the smoke by virtue of the magnesium mechanically expelled. The

mixture then had the composition:

Zinc 34.6

Carbon tetrachloride 40.8

Sodium chlorate 9.3

Ammonium chloride 7.0

Magnesium carbonate 8.3

SIZE OF SMOKE PARTICLES

In the problem of smoke production, the size of the particle is of

great importance. Being a physical quantity it can easily be correlated

with such physical properties as settling, diffusion, coagulation, and

evaporation. These factors are more important in connection with toxic

smokes, since there the penetration factor must be considered.

Smoke appears to consist of particles of all sizes from 10⁻³ cm.,

which may just be resolved by the unaided eye, to molecular

dimensions, 10⁻⁸ cm. The larger particles settle out most rapidly and

so do not remain long in suspension.

MEASUREMENT

Wells and Gerke have developed a form of ultra-microscope which is

well adapted to the measurement of the size of smoke particles. The

ultra-microscope is a low power microscope using intense dark ground

illumination for viewing particles which are too small to be seen

by transmitted light. They are rendered visible in this way, since

any object, no matter how small, which emits enough light to affect

the retina is visible, provided the background is sufficiently dark.

Thus stars are visible at night and dust particles are easily seen

in a sunbeam in a darkened room. The larger particles, viewed in

this way, do not appear larger but brighter. The apparent size of

the particles is determined by the diffraction pattern and is thus

dependent only on the optical system used to view them. The more

intense the incident light, the brighter the particles appear. In the

ultra-microscope described, the image of an intense source, such as a

concentrated filament lamp, or an arc, is focused upon the particles in

the microscopic field, but the axis of the illuminating beam, instead

of coinciding with the axis of the microscope, as ordinarily used,

is perpendicular to it. The beam itself, therefore, never enters the

microscope at all, but passes under the objective into a blackened

chamber where it is absorbed. The field of the microscope is made dark

by placing underneath the objective another “black hole” or blackened

chamber with an opening just a little larger than the field.[34]

[Footnote 34: This ultra-microscope is described in _J. Am. Chem. Soc._

=41=, 312 (1919).]

The method used for measuring the velocity consisted in causing the

particle to describe a definite stroke many times in succession in an

electric field. This was accomplished by reversing the direction of the

field with a rotating commutator. The convection due to the source of

light is perpendicular to this motion so that a zigzag line is obtained

(see Fig. 88). The amplitude of this oscillation is an accurate measure

of the distance traversed by the particle under the electric force for

a definite small interval of time. The speed of the rotating commutator

and the electric field are both susceptible of precise measurement, so

that the size of a single particle is precisely determined.

[Illustration: FIG. 87.—Ultramicroscope for Measuring Size of Smoke

Particles.]

[Illustration: FIG. 88.—Measurement of Smoke Particles by Use of

Ultramicroscope.]

When a sample of smoke is viewed in the ultra-microscope, it appears

like the starry heavens, except that the stars are dancing violently

about. At first little distinction is made between the particles, as

there seems to be no order in their motion, but soon it becomes evident

that the brighter particles are more sluggish than the dim ones. This

is due to the greater mass of the bright particles, for they are

larger. The particles are all moving slowly away from the source of

light and eventually diffuse to the walls of the cell.

When the electric field is turned on, about one-third of the particles

immediately migrate, about equally in both directions, to the two

electrodes. If the field is reversed, the direction of migration

is reversed and if the commutator is used the particles oscillate

regularly. Sometimes the particles may be seen to combine and become

neutral, in which case oscillation ceases.

CONCENTRATION OF SMOKE

In measuring the concentration of smokes, the following terms are

useful:

=Density.= The density of a smoke is defined as the reciprocal of the

thickness of the smoke layer in feet necessary to obscure a given

filament. Thus six inches of a smoke of density 2.0 is required to

obscure an electric light filament, whereas one requiring four feet

would have a density of 4. Another way to show the significance of this

definition is to point out that if a definite weight of a stable smoke

is diluted with air after it is formed, the product of the volume by

the density always remains constant. Any marked variation in this rule

may be taken as evidence that the particles of smoke are undergoing a

change, in most cases due to evaporation.

=Total Obscuring Power.= The volume of smoke produced per unit weight

of material used is the second factor in determining the value of a

smoke. The product of this volume per unit weight by the density of the

smoke is the real measure of effectiveness, and is called the total

obscuring power (T. O. P.) of the smoke. If the volume is expressed in

cubic feet per pound and the density in reciprocal feet, the unit of T.

O. P. is square feet per pound. That is, it expresses the square feet

of a smoke wall, thick enough to completely obscure a light filament

behind it, which could be produced from a pound of the reacting

substances. The total obscuring power of some typical smokes are as

follows:

Phosphorus 4600

NH₄Cl(NH₃ + HCl) 2500

SnCl₄ + NH₃ + H₂O 1590

Berger Mixture 1250

SnCl₄ + NH₃ 900

SO₂ + NH₃ 375

In all measurements of density, and therefore of T. O. P., the _rate

of burning_ must be considered. If a slow burning material be compared

with a rapid one, the former will not reach its true maximum density,

as a great deal of the smoke may settle out during the time of burning.

Comparisons of T. O. P. are significant only when made on smoke

mixtures of the same type and in about the same quantities.

MEASUREMENT

Two methods of measuring the effectiveness of a smoke cloud have

been devised, one, the smoke box, which measures the obscuring power

directly by observing at what distance a lamp filament is obscured by

intervening smoke, the other, the Tyndall meter, which measures the

intensity of the scattering of the light.

The earliest measurements of smoke intensity are perhaps those of

Ringelmann (_Revue Technique_, =19=, 286), who devised the well known

chart of that name, intended mainly for measuring intensities of black

smoke issuing from a chimney at a distance. The first measurements

for military purposes are probably due to Bertrand, who made numerous

comparative studies with his “salle opacimetrique.” This was a room

23 × 14 × 3.6 meters, with 7 windows. Two doors, one provided with

3 oculars 2 cm. in diameter, gave access to the room. On the other

door, opposite the first, were hung several black signs. Six pairs

of columns were spaced along the room at measured distances. When a

smoke is produced in the room, the black paper signs first become

invisible, then the door itself, and finally the columns, pair by

pair. They reappear in the reverse order, and as a measure of relative

opacity Bertrand took the time elapsing between the detonation and the

reappearance of the farther door.

[Illustration: FIG. 89.—Tyndall Meter.]

[Illustration: FIG. 90.—Cottrell Precipitation Tube.]

=Smoke Box.= The smoke box, used by the C. W. S., was constructed of

wood with tight joints, and had a moveable brass rod running through it

to which was attached a small size 25-Watt Mazda lamp. The density of

each smoke introduced in the box is determined by moving this lamp back

and forth until a point is reached when the pattern of the filament

can just be distinguished by the observer looking in at the glass

window, external light being excluded by a black cloth. The thickness

of the smoke layer between the glass window and the light is recorded

as the measure of the smoke density. For field tests, a larger box, 6

× 8 × 8 feet (288 cubic feet) was constructed. The observation light

was moveable in a line connecting the mid-points of opposite sides of

the box. To insure uniform distribution of smoke, a fan with 18-inch

blade revolved at any desired speed between 60 and 250 r.p.m. With

this, results are obtained indicating both the original density and its

stability.

=Tyndall Meter.= The Tyndall meter was first devised for studying

smokes and mists. Tolman and Vliet adapted it to Chemical Warfare

purposes, and used it in studying the properties of smokes.

The apparatus (Fig. 89) consists eventually of an electric light bulb,

a condensing lens giving a beam of parallel light which passes through

the diaphragm, and a Macbeth illuminometer for measuring the strength

of the Tyndall beam. In case the material is a liquid suspension or

solution, it is introduced into a cylindrical glass tube, while smokes

and mists are premixed directly through the apparatus. The long closed

tubes are provided, respectively, for absorbing the beam after it has

passed through the disperse system and for giving a dark background for

observing the Tyndall beam. Methods of standardization are given in the

_Journal of the American Chemical Society_, =41=, 299.

A third method for analyzing smokes consists in the use of an

electrical precipitator. This apparatus consists essentially of

a modified Cottrell Precipitator, with a central wire as cathode

surrounded by a cylindrical foil as anode (Fig. 90). The smoke to

be analyzed is drawn through the apparatus at a known rate, and the

particles of smoke precipitated on the foil by means of a high voltage,

direct current. The determination of concentration is made by weighing

the foil before and after precipitation.

APPARATUS FOR SMOKE PRODUCTION

SMOKE BOX

The smoke box was developed for the Navy for use when it was desirable

to have the smoke screen generated away from the ship. (The smoke

funnel, described later, was operated on board ship). The float

consists of an iron container (holding the smoke mixture) surrounded

by an iron float to support the apparatus when it is thrown into the

water (Fig. 91). The iron container consists of a cylinder 22 inches

high and 10 inches in diameter. One inch holes are bored 1½ inches

from the top of this cylinder, from which the smoke is emitted. The

iron float is about 2 feet in diameter and 8 inches deep. This box

holds approximately 100 pounds of smoke mixture, and is so constructed

that it will float one hour. When ignited, the mixture burns 9 to 9½

minutes. The smoke produced has a T. O. P. of about 1900. Fig. 92 shows

the Navy Smoke Box in action.

[Illustration: FIG. 91.—Navy Smoke Box.]

[Illustration: FIG. 92.—Navy Smoke Box in Action.]

SMOKE CANDLE

Smoke candles are used for producing a cloud of smoke for screening

purposes in or behind the lines. They are made by packing about

three pounds of the modified Berger Mixture in a container (Fig. 93)

(galvanized can 5¼ inches by 3½ inches) and are lighted by means of the

match head type of ignition. Smoke is given off at a uniform rate for

about 4 minutes, forming a dense, fog-like cloud which hangs low (Fig.

94). This smoke is absolutely harmless, and can be breathed without

discomfort. The obscuring power is high and, with a favorable wind, a

small number of the candles will produce a screen sufficiently dense to

allow operations to be carried out unseen by the enemy.

[Illustration: FIG. 93.—B. M. Smoke Candle.]

SMOKE GRENADE

The smoke grenade is also designed for use in trench and field warfare,

where it is desired to produce a dense smoke screen. It is made by

packing 340 grams of the standard smoke mixture in an ordinary light

metal gas grenade. Around the top of the grenade are vents closed by

a zinc strip. The ignition is caused by the standard bouchon when the

grenade is thrown. The heat of the reaction burns through the zinc

strip and a dense cloud of smoke is evolved for 45 seconds.

[Illustration: FIG. 94.—Smoke Cloud from B. M. Candle.]

Stannic chloride has also been used extensively in hand grenades, as

it gives a very disagreeable cloud of smoke upon detonation. Due to

the high prices and urgent need of tin for other purposes, silicon

tetrachloride was substituted for tin tetrachloride towards the close

of the war. A mixture of silicon tetrachloride and chloropicrin was

also used. This not only gives a very good smoke cloud, but combines

with it the toxic properties of the chloropicrin cloud.

The method of firing the smoke grenade is the same as that of any

grenade using the same type of bouchon. Usually the grenade is grasped

in the hand for throwing in such a manner that the handle of the

bouchon is under the fingers. The safety clip is pulled out with the

other hand and the grenade is thrown with an overhand motion. When the

grenade leaves the hand, the handle of the bouchon flies off, allowing

the trigger to hit the cap which ignites the fuse.

The white phosphorus combined hand and rifle grenade became the

standard smoke grenade by the end of the war. Stannic chloride was used

to clear out dugouts, but not as a smoke producer.

STOKES’ SMOKE SHELL

[Illustration: FIG. 95.—Stokes’ Smoke Shell.]

The Stokes’ smoke shell was perfected to furnish a means of maintaining

the best possible smoke screen at long ranges by means of an easily

portable gun. The 3-inch Stokes shell, as adapted for combustion

smokes, weighs about 13 pounds and contains about 4 pounds of standard

smoke mixture. This shell is designed to produce a continuous screen

over a period of 3 to 4 minutes.

LIVENS SMOKE DRUM

The Livens smoke drum was designed for use with the 8-inch Livens

projector, so as to produce a smoke screen of large volume and long

duration at long ranges. The drum, as adapted for combustion smokes,

weighs 17.5 pounds empty and 49 pounds loaded. The smoke-gas mixture

was specially adapted for use in the Livens drum.

[Illustration: FIG. 96.—Livens Smoke Bomb.]

Smoke mixtures in Livens were never used to any considerable extent

in the war and it is questionable if they ever will be. A Livens can

usually only be fired once before resetting, hence Stokes mortars are

used whenever possible.

SMOKE FUNNEL

The smoke funnel was developed for the production of a white smoke

cloud from the stern of a vessel. The smoke producing materials are

liquid ammonia and silicon tetrachloride, with carbon dioxide as a

compressing medium. This is the most satisfactory compressing medium,

because: (1) The silicon tetrachloride is forced out at nearly constant

pressure. (2) The carbon dioxide is easily compressed to a liquid and

can be handled in this form. Further, it has a vapor pressure of 800

pounds at 60° F., and a cylinder can be nearly emptied without loss

in efficiency. (3) Carbon dioxide is sufficiently soluble in silicon

tetrachloride to cause the latter to effervesce and thus materially aid

in its evaporation on spraying. (4) Liquid carbon dioxide, behaving in

a manner similar to liquid ammonia, affords a means for the silicon

tetrachloride to “keep pace” with the ammonia, under changes in

temperature, and thus ensures a more nearly neutral, and therefore the

most effective, smoke.

[Illustration: FIG. 97.—Navy Smoke Funnel.]

The smoke funnel proper consists of an open end cylinder, about 2 feet

in diameter and 7 feet long, mounted in a horizontal position on an

angle iron frame. At one end is an 18-inch fan securely fastened to the

cross supports. This fan is operated by hand, through gears giving a

ratio of about 30 to 1. The silicon tetrachloride enters the cylinder

through a pipe, which terminates in four spray nozzles, while the

ammonia enters through a single nozzle. The air forced into the funnel

serves to hydrolyze the silicon tetrachloride and mixes the vapors. The

resulting reaction evolves a dense white cloud of very large volume and

high obscuring power. One set of cylinders is capable of maintaining

this cloud for over 30 minutes. Under normal conditions the discharge

is at the rate of 2 pounds of silicon tetrachloride to 1 pound of

ammonia. To stop the smoke, the silicon tetrachloride is closed first,

the ammonia allowed to run about half a minute, and the fan is shut off

last.

[Illustration: FIG. 98.—Navy Smoke Funnel in Operation.]

SMOKE KNAPSACK

The smoke knapsack furnishes a portable apparatus for smoke production.

The gross weight is about 70 pounds; when in operation it gives a dense

white smoke for about 15 minutes. The operation may be intermittent

or continuous and the quantity of smoke is sufficient to completely

hide one platoon of men in skirmish formation with a 5-mile per hour

enfilade wind. The apparatus consists of two steel tanks about 26

inches in height and 6 inches in diameter. From the side of each tank,

but near the bottom, extends a short pipe on which is placed a suitable

valve. A flexible armored hose connects the valve to a short length of

pipe which is equipped with spray nozzle. The cylinders are charged

with silicon tetrachloride and ammonia under pressure. The valves may

be operated with the left hand, while the sprayer apparatus is held in

the right. The release buckles are within easy reach of both hands.

SHELL

While many special devices have been developed by means of which the

gas troops and infantry are able to set up smoke clouds on short

notice, the smoke shell, fired by the artillery, always played an

important part in this work. In the same way that a large number of the

poison gases were adapted to artillery use, so were most of the smoke

producing substances.

As a filler for smoke shell, phosphorus easily ranks first, and is

approached only by sulfur trioxide in very humid weather. A rough

approximation to the relative values of some of its rivals is given in

the following table:

White phosphorus 100

Sulfur trioxide 60-75

Stannic chloride 40

Titanium chloride 25-35

Arsenic chloride 10

Comparison of the value of different forms of phosphorus for shell

purposes has invariably pointed to the superiority of the white

variety. Mixtures of white and red (2 to 1) have also proved effective.

A complete barrage over a front of 200 yards can be established in from

40 seconds to 1 minute and maintained by firing a salvo followed by

battery fire of 3 seconds. Four 4.5-inch howitzers could maintain an

effective barrage over a front of 1000 yards. The influence of sunshine

is very marked, as in moist, cool weather one shell every 15 seconds is

sufficient.

[Illustration: FIG. 99.—Smoke Screen for Tanks.]

SCREENING TANKS

Tests have demonstrated (see Fig. 99) that successful smoke screens for

tanks may be produced by spraying oleum into the exhaust. On a 7-ton

tank of the Renault type (40 H. P.) 110 cc. per minute produced a large

volume of smoke, which had excellent covering power, and which could be

made intermittent or continuous at will.

The same method may be applied to aeroplanes, and to ships. It is

calculated that a cylinder containing 300 pounds of 20 per cent oleum

will maintain a smoke screen on a ship for a period of 15 minutes,

if oleum is used at the rate of 23.6 pounds per minute. Since the

cylinders may be arranged in batteries, the screen may be continued

for any period of time. The Tank Corps rather favor phosphorus rifle

grenades for producing a smoke screen at a distance from the tank.

PURPOSE OF SMOKE SCREEN

Smoke screens may be employed with one or more of the following objects

in view:

(1) To mask known enemy observation posts and machine gun nests; to

conceal the front and flanks of attacking troops, concentration of guns

and tanks, roads and concentration points; to blind the flashes of

batteries in action and to hamper aerial observations.

(2) As a feint to draw the enemy’s attention to a front on which no

attack is being made, so as to hold his troops to their trenches, or to

induce him to expend ammunition needlessly and to put down a barrage in

the wrong place.

(3) To simulate gas and force the enemy to wear his mask. Gas should

occasionally be mixed with smoke, to impress upon him the belief that

it is never safe to remain in a smoke cloud without wearing his mask.

(4) In rolling or mountainous country, to fill valleys with smoke and

thereby conceal the advance from all observation, including aerial.

(5) To cover the construction of bridges, trenches, etc., in the face

of the enemy.

THE TACTICAL VALUE OF SMOKE

The pall of smoke that hung over every battlefield of the Civil

War made a profound impression upon Fries when, as a boy, he first

read of those battles. However, practically every reference made

to smoke treated it as a nuisance. It obscured the field of vision

and interfered with troop movements as well as with the aiming and

firing of rifles and cannon, though due to their short range this

was not so serious as it would be nowadays. Nevertheless so deeply

was this interference appreciated that the most earnest efforts were

made to discover a smokeless powder. This, as the world well knows,

was developed with great efficiency during the latter part of the

nineteenth century. With the development of the smokeless powders

came also a better understanding of the action of powder, whereby the

velocity of projectiles, and consequently the range and accuracy, were

greatly increased. This increased range and accuracy of guns forced a

consideration of protection,—and concealment is one form of protection.

The Navy would appear to have been the first branch of the American

forces to realize how valuable a smoke screen may be. Thus Fries, in

August, 1913, had the interesting experience of witnessing a week’s

maneuvers at the eastern entrance to Long Island Sound between the

Navy and the Coast Artillery. During that week the Navy carried out

extensive experiments with smoke screens both by day and by night. The

smoke in all cases was generated by smothering the fires on destroyers

or other ships, thus causing dense clouds of black smoke to be given

out from the funnels.

After the World War had been in progress some time and particularly

about the time the United States entered it, a determined search was

begun for more efficient smokes and more efficient smoke producers.

In the Navy, smoke screens were expected to be established by small

craft behind which larger vessels could maneuver for position and

range. These screens were also established for the purpose of cutting

off the view of enemy submarines or other vessels, thus allowing

merchant ships or even warships when injured or outclassed to escape.

The Army was much slower to appreciate the value of smoke. In fact,

apparently no army really realized the value of a smoke screen until

after gas warfare became an accomplished fact. As is well known, the

evaporation of the large quantity of liquid used in wave attacks

caused a cloud of condensed moisture. This is what gave rise to the

designation “cloud attack.”

English regulations for defense against gas in the early days called

for every man and animal to stand fast upon the approach of a gas cloud

and remain quiet until the cloud had passed. Thus casualties were

reduced to a minimum and the English were fresh to receive the attack

that was frequently launched immediately after the cloud had passed.

The Germans finally thought of the plan of sending over a fake gas

attack. In that way they simply produced a smoke cloud that looked like

a gas attack. Naturally the English stood fast as before. The Germans

attacking in the fake cloud naturally caught the British at a complete

disadvantage with consequent disastrous results to the latter.

But that was a game at which two could play. About this time the

value of white phosphorus for producing a smoke screen was taken up

by the British and large numbers of 4-inch Stokes mortar shells were

filled for that purpose. All armies then began to experiment with

smoke producing materials. Most of these were liquid. Of them all, as

has been stated before, white phosphorus, a solid, proved the best.

Toward the close of the war these smoke screens began to be used to

a considerable extent for the purposes given above. No one who has

engaged in target practice and encountered a fog, or who has hunted

ducks and geese in a fog needs to be told of the difficulty of hitting

an object he cannot see.

The First Gas Regiment proved its worth and won everlasting glory by

using the Stokes’ mortars of the British with their phosphorus bombs

for attacking machine gun nests. The white phosphorus in that case had

a double effect. It made a perfect smoke screen, thereby making the

German machine gun shots simply shots in the dark, while at the same

time the burning phosphorus forced the gunners to abandon their guns

and surrender. Thus phosphorus played and will play in the future the

double rôle of forming a defensive screen and of viciously attacking

enemy troops. This phosphorus, which catches fire spontaneously, burns

wet or dry, total immersion in water alone sufficing to put it out.

This means of extinguishing the flames being almost totally absent on

the battlefield, it can be truthfully said that burning phosphorus is

unquenchable. The burns are severe and difficult to heal. For these

reasons white phosphorus will be used in enormous quantities in any

future war.

All armies have begun to realize this value of smoke. In the future it

will be the infantryman’s defense against all forms of weapons and it

will be used on every field of battle, by every arm of the service and

at all times, day or night. It is even more effective in shutting out

the light from searchlights, star bombs and similar illuminants for

use in night attacks than it is in daylight. With this straight use of

smoke for protection will go its use along with poisonous gases. Every

smoke cloud will be poisonous or non-poisonous at the will of the one

producing the cloud, and this will be true whether it is produced from

artillery shell, mortar bombs, hand grenades, smoke candles or other

apparatus. Thus smoke and gas together will afford a field for the

exercise of ingenuity greater than that of all other forms of warfare.

The only limitation to the use of smoke and gas will be the lack of

vision of commanders and the ignorance of armies.

Proper recognition and aid given to chemical warfare development

and instruction in peace are the only methods of overcoming these

limitations. In this, as in all other development work, the most

serious obstacle comes from the man who will not see, whether it be

from a lack of intelligence, laziness or inbred opposition to all forms

of advancement.

Chemical warfare · 第 13 / 23 章