CRYPTOGRAPHY.--PRESERVATION OF TELEGRAMS.

Optical telegraphy, by reason of its very principle, presents both the

advantage and inconvenience of leaving no automatic trace of the

correspondence that it transmits. The advantage is very evident in

cases in which an optical station falls into the hands of the enemy;

on the other hand, the inconvenience is shown in cases where a badly

transmitted or badly collated telegram allows an ambiguity to stand

subject to dispute. Moreover, in case of warfare between civilized

nations that have all the resources of science at their disposal,

there may be reason to fear lest one of the enemy's optical stations

substitute itself for the corresponding station, and take advantage of

the situation to throw confusion into the orders transmitted. The

remedy for this appears to reside in the use of cryptography and in

the exchange, at various intervals, of certain words that have been

agreed upon beforehand, and that the enemy is ignorant of.

As for the automatic preservation of telegrams, the problem has not

been satisfactorily solved. It has been proposed to connect the key of

the manipulator of the optical apparatus with the manipulator of an

ordinary Morse apparatus, thus permitting the telegram to be preserved

upon a band of paper. It is unnecessary to say that the space occupied

by a dispatch thus transmitted would be considerable; but this is not

what has stopped innovators. The principal objection resides in the

increase in muscular work imposed by this arrangement upon the

telegrapher. Obliged to keep his eye fixed intently at the receiving

telescope, while at the same time maneuvering the manipulator and

spelling aloud the words that he is receiving, the operator should

have a very sensitive manipulator at his disposal, and not be

submitted to mental or physical overtaxation. So the apparatus that

have been devised have not met with much success.

Two French officers, working independently, have hit upon the same

idea of receiving the indications transmitted by the vibration of the

luminous fascicle directly upon their travel. The method consists in

the use of that peculiar property of selenium of becoming a good

conductor under the action of a luminous ray, while in darkness it

totally prevents the passage of the electric current. Such

modification of the physical properties of selenium, moreover, occurs

without the perceptible development of any mechanical work. If, then,

in the line of travel of the luminous fascicle emitted by the optical

apparatus, or in a portion of such fascicle, we interpose a fragment

of selenium connected with the two poles of a local pile, it is easy

to see that the current from the latter will be opened or closed

according as the luminous ray from the apparatus will or will not

strike the selenium, and that the length of time during which the

current passes will depend upon the length of the luminous attacks. A

Morse apparatus interposed in this annexed circuit will therefore give

an automatic inscription of the correspondence exchanged. Such is the

principle. But, practically, very great difficulties present

themselves, these being connected with the rapid weakening of the

electric properties of the selenium, and with the necessity of having

recourse to infinitely small mechanical actions only. The problem is

nevertheless before us, and it is to be hoped that the perseverance of

the scientists who are at work upon it will some day succeed in

solving it.

Finally, we may call attention to the attempts made to receive the

luminous impression upon a band prepared with gelatino-bromide of

silver. In practice this band would unwind uniformly at the focus of

the receiving telescope, which would be placed in a box, forming a

camera obscura. The velocity of this band prepared for photographing

the signals would be regulated by clockwork. The experiments that have

been made have not given results that are absolutely satisfactory, by

reason of the length of the signals received and the mechanical

complication of the device.

Scientific American Supplement, No. 508, September 26, 1885 · 第 45 / 73 题