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<v Speaker 1>Section thirty one of the Science History of the Universe,

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<v Speaker 1>Volume three. This is a LibriVox recording. All LibriVox recordings

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<v Speaker 1>are in the public domain. For more information or to volunteer,

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<v Speaker 1>please visit LibriVox dot org. Recording by Emelia Chesley, The

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<v Speaker 1>Science History of the Universe, Volume three, edited by Francis

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<v Speaker 1>rold Wheeler. Electricity, Chapter eleven Wireless Telegraphy, Part one. Professor

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<v Speaker 1>Henry of Princeton University was the first to show the

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<v Speaker 1>oscillatory character of the discharge of a Leyden jar. This

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<v Speaker 1>single loud spark, which to the eye seems to pass

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<v Speaker 1>in one direction across the gap, is really a quick

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<v Speaker 1>succession of current surges, first one way and then the other,

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<v Speaker 1>and has its mechanical analogy in the pendulum at the outset.

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<v Speaker 1>It may be well to analyze this spark discharge, as

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<v Speaker 1>it is still the most mos prominent means of radiating

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<v Speaker 1>the electric waves used to transmit signals. Suppose this pendulum

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<v Speaker 1>analogy of the spark discharge between two spheres be taken,

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<v Speaker 1>and the similarity of the two actions noted. If a

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<v Speaker 1>heavy pendulum be drawn back by means of a light fiber,

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<v Speaker 1>it will finally strain the fiber to such an extent

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<v Speaker 1>as to cause it to break. The pendulum, being suddenly released,

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<v Speaker 1>gradually acquires motion, which is accelerated until its lowest position

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<v Speaker 1>is reached, after which it is retarded just as it

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<v Speaker 1>was accelerated, and stops at about the same height at

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<v Speaker 1>which it started. The process is then repeated, but in

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<v Speaker 1>the opposite direction. Now compare the action on the two

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<v Speaker 1>charged spheres. The pressure in the dielectric surrounding the spheres

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<v Speaker 1>is gradually raised until it suddenly gives way, there being

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<v Speaker 1>a flow of current from the positive to the negative sphere,

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<v Speaker 1>which current gradually increases and is greatest at the instant

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<v Speaker 1>when bold dielectrics are at the same potential, just as

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<v Speaker 1>the motion of the pendulum was greatest at its lowest position.

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<v Speaker 1>The current then begins to decrease and finally stops when

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<v Speaker 1>the dielectric is again strained to about the same potential

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<v Speaker 1>it had at first, but reversed indirection. The current then

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<v Speaker 1>starts back again, just as the pendulum again required motion. Now,

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<v Speaker 1>let it be considered what goes on in the space

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<v Speaker 1>surrounding this action. A current is always surrounded by a

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<v Speaker 1>field of magnetic force, which field is proportional to the

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<v Speaker 1>strength of the current. As this current between the two

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<v Speaker 1>spheres increases, there is therefore sent out an increasing magnetic

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<v Speaker 1>field which is radiated into space, reaching a maximum and

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<v Speaker 1>again decreasing with the current. But while the current increases,

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<v Speaker 1>the electrostatic strain about the sphere decreases, thus sending out

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<v Speaker 1>an electrostatic wave, which again increases as the current decreases.

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<v Speaker 1>It will thus be seen that as these surges take place,

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<v Speaker 1>alternate electromagnetic and electrostatic waves are radiated into space. Why

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<v Speaker 1>do not these surges keep on forever? Mainly because the

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<v Speaker 1>current in its flow across the gap encounters a resistance, and,

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<v Speaker 1>instead of converting all its energy into magnetic waves, loses

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<v Speaker 1>a portion as heat at each surge. This corresponds to

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<v Speaker 1>oscillating the pendulum in a liquid or viscous material, the

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<v Speaker 1>energy of its motion soon being converted into heat. So

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<v Speaker 1>much for the creation of these waves, But how may

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<v Speaker 1>their passage through space be detected? One way is by

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<v Speaker 1>catching them on a wire. What is the manner of

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<v Speaker 1>the catching? If a wire be placed so that it

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<v Speaker 1>cuts the wave transversely to its line of motion, it

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<v Speaker 1>is clear that the moving magnetic wave will induce in

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<v Speaker 1>it an electromotive force. As these waves follow in rapid succession,

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<v Speaker 1>a series of alternating electromotive forces is set up in

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<v Speaker 1>the wire. These oscillatory currents are sometimes called jigs. How

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<v Speaker 1>these jig currents make their presence known varies with the

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<v Speaker 1>style of wave detector used Before entering upon the history

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<v Speaker 1>of this spark telegray, as the Germans call it, it

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<v Speaker 1>may be well to review some of the experiments which

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<v Speaker 1>preceded this system. In eighteen thirty eight, Professor Joseph Henry

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<v Speaker 1>of Princeton, making with an electrical machine and leydingjar a

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<v Speaker 1>one inch spark in the top room of his residence,

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<v Speaker 1>set up induced currents in the cellar of the same building.

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<v Speaker 1>Professor Morse, however, was probably the first to successfully transmit

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<v Speaker 1>signals without wire. On December sixteenth, eighteen forty two, he

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<v Speaker 1>sent a wireless telegram across a canal eighty feet wide,

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<v Speaker 1>and in November eighteen forty four, L. D. Gale, acting

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<v Speaker 1>under instructions from Professor Morse, made wireless signals across the

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<v Speaker 1>Susquehanna River at Havre de Grace, a distance of nearly

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<v Speaker 1>one mile. In the latter experiment, mister Gale used as

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<v Speaker 1>a source of energy six pairs of plates in the

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<v Speaker 1>form of a galvanic battery. He found that the best

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<v Speaker 1>results were obtained when on each side of the river

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<v Speaker 1>two plates were immersed near its bank and worked connected

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<v Speaker 1>by an insulated wire stretched along each shore for a

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<v Speaker 1>distance three times as great as that which measured either

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<v Speaker 1>path of the crossing signals. A few years later, James Lindsay,

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<v Speaker 1>a Scotchman, repeated Morse's experiments, but without knowing of them.

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<v Speaker 1>In eighteen fifty nine he read a paper before the

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<v Speaker 1>British Association on the subject of telegraphing without wires, and

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<v Speaker 1>among his hearers were Faraday and Lord Kelvin. A method

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<v Speaker 1>of signaling without wires by means of the inductive effect

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<v Speaker 1>of two parallel circuits was successfully used by Sir William

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<v Speaker 1>Preece in eighteen eighty two. The principle of this method

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<v Speaker 1>is as follows. If two loops of wire are placed

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<v Speaker 1>parallel to each other, and an intermittent current is passed

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<v Speaker 1>through one of them, waves of magnetic flux are sent

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<v Speaker 1>out portions of which thread the second loop, and by

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<v Speaker 1>their fluctuations produce currents in it, which may be detected

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<v Speaker 1>by a telephone or other device. The strength of such

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<v Speaker 1>signals falls off very rapidly from the source, and such

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<v Speaker 1>a system can only be made to operate over short distances.

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<v Speaker 1>Priests constructed two parallel lines, one on the English coast

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<v Speaker 1>and one on the Isle of Wight, the arrangement of

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<v Speaker 1>which is shown in Fig. Forty eight. It will be

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<v Speaker 1>seen that the loop from which the waves emana is

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<v Speaker 1>formed by the line, wire and the Earth. The crowning achievement, however,

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<v Speaker 1>was the work of Hertz, whose early death deprived the

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<v Speaker 1>world of the aid of a most powerful brain. In

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<v Speaker 1>eighteen eighty six, Hertz discovered that if a loop of

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<v Speaker 1>wire having a small air gap left in it were

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<v Speaker 1>placed at a distance from a spark discharge of a

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<v Speaker 1>Leyden jar minute sparks would pass across the air gap

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<v Speaker 1>of the loop, thus indicating the presence of electric waves.

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<v Speaker 1>He subsequently made a very complete study of the behavior

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<v Speaker 1>of these waves, and thus gave a tremendous impetus to

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<v Speaker 1>the development of wireless telegraphy. Second to the work of

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<v Speaker 1>Hertz is that of Sir Oliver Lodge, who, in eighteen

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<v Speaker 1>eighty nine to descis discovered the effect of electrical waves

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<v Speaker 1>on the breaking down of the electrical resistance of two

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<v Speaker 1>knobs barely in contact, which discovery resulted in the first

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<v Speaker 1>means used to detect the presence of electrical waves, the coherer.

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<v Speaker 1>The development of wave detectors is an important chapter for

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<v Speaker 1>these instruments. Professor Fleming has suggested the use of the

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<v Speaker 1>word simoscope as a general term including all classes of

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<v Speaker 1>wave detectors. A great number of these have been invented,

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<v Speaker 1>but they may all be included under the following classes.

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<v Speaker 1>One spark seymoscopes, two contact cymoscopes, three thermal cymoscopes, four

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<v Speaker 1>magnetic cymoscopes, five electrolytic cymoscopes, six electrodynamic cymoscopes, and seven

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<v Speaker 1>vacuum tube cymoscopes. The first cymoscope invented was that used

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<v Speaker 1>by Hertz in his investigation of electrical waves, and belongs

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<v Speaker 1>to the first class. Resisted merely of a ring broken

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<v Speaker 1>at one point and arranged so that the gap might

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<v Speaker 1>be adjusted by means of a micrometer screw. Tiny sparks

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<v Speaker 1>across this gap indicated the presence of waves. Since the

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<v Speaker 1>electromotive force required to produce a spark across even a

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<v Speaker 1>small gap is very considerable. It will be obvious that

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<v Speaker 1>such a detector could only operate at a short distance,

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<v Speaker 1>and would therefore be useless for the purpose of signaling.

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<v Speaker 1>The next invention, made in eighteen ninety was the Bramley

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<v Speaker 1>Coherer Fig. Forty nine, which consisted of a small glass

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<v Speaker 1>tube containing two metallic plugs and separated by a gap

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<v Speaker 1>partially filled with metallic fillings. This is an example of

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<v Speaker 1>the second class. The metallic fillings, when loosely packed, offer

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<v Speaker 1>a very high resistance to the passage of current through them,

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<v Speaker 1>but the presence of waves breaks down their contact resistance,

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<v Speaker 1>which continues after the waves have ceased. In order to

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<v Speaker 1>again restore their resistance, they must be tapped or shaken,

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<v Speaker 1>an operation known as decoherence. It is obvious that such

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<v Speaker 1>an apparatus may be used like a key in a

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<v Speaker 1>telegraph circuit, a key operated by electrical waves, and may

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<v Speaker 1>therefore be used to operate a telegraphic instrument. Such was

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<v Speaker 1>the first device used. It was defective, however, in that

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<v Speaker 1>it was necessary to tap it after each signal. Decoherence

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<v Speaker 1>was not certain. It required frequent adjustment, and the result

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<v Speaker 1>was often a confused lot of signals. Many arrangements of

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<v Speaker 1>loose contacts were tried, and the coherer was improved by Marconi, Lodge,

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<v Speaker 1>Braun and others. One of the principal troubles being the

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<v Speaker 1>operation of decoherence. Most of the inventors sought to develop

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<v Speaker 1>a coherer which could be self restoring, and a number

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<v Speaker 1>of successful types were invented. One of these was the

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<v Speaker 1>Hughes coherer, employing carbon granules placed between iron plugs. The

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<v Speaker 1>most perfect and successful of all these is, however, that

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<v Speaker 1>devised by Sir Oliver Lodge and doctor Muirhead and used

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<v Speaker 1>in the Lodgemere Head system, as shown in figure fifty.

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<v Speaker 1>It consists of a steel disk slightly separated from a

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<v Speaker 1>globule of mercury by a film of oil. The disc

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<v Speaker 1>being arranged to rotate slowly. The presence of waves breaks

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<v Speaker 1>down the oil film and establishes contact with the mercury,

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<v Speaker 1>which contact immediately breaks upon the cessation of the waves.

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<v Speaker 1>A siphon recorder placed in the series with the symoscope

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<v Speaker 1>is used to record the message. Although a number of

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<v Speaker 1>forms of magnetic style of detector were devised. It was

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<v Speaker 1>not until nineteen o two that a successful working apparatus

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<v Speaker 1>was produced. For some time before that, it was known

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<v Speaker 1>that the oscillating currents received would annull wholly or in part,

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<v Speaker 1>the magnetic hysteresis of iron when passed through a coil

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<v Speaker 1>surrounding the iron. Hysteresis acts like molecular friction, so that

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<v Speaker 1>when a magnetizing current is passed through a coil surrounding

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<v Speaker 1>an iron core, the magnetization does not increase and decrease

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<v Speaker 1>with the current in the coil, but lags behind it.

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<v Speaker 1>If another coil be placed around this core and the

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<v Speaker 1>oscillating currents passed through it, this hysteresis will be suddenly

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<v Speaker 1>removed and the magnetism in the core will suddenly change

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<v Speaker 1>in value. This sudden change could be detected by a

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<v Speaker 1>third coil surrounding the core and connected to a telephone receiver,

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<v Speaker 1>resulting in a sudden click. This was the principle of

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<v Speaker 1>which Marconi made use in his magnetic detector, and which

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<v Speaker 1>he has used in his long distance experiments. The arrangement

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<v Speaker 1>is shown in Fig. Eighteen. It consists of a band

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<v Speaker 1>of iron wires passing through two coils, one carrying the

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<v Speaker 1>jig currents and one connected to the telephone. The wires

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<v Speaker 1>are magnetized by two permanent magnets, and as they move

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<v Speaker 1>under that portion where the two poles meet, the magnetic

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<v Speaker 1>flux in them undergoes a reversal. Which reversal, however, always

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<v Speaker 1>takes place at the same point until the jig currents pass,

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<v Speaker 1>when the flux is suddenly shifted backward, causing a sound

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<v Speaker 1>in the telephone. These detectors have come into very general

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<v Speaker 1>use on account of their convenience, sensitiveness, and adaptation to

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<v Speaker 1>rapid signaling. In nineteen o one, doctor Lee de Forest

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<v Speaker 1>patented a detector which depends for its operation on the

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<v Speaker 1>disruption of the minute metallic bridges or trees, which form

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<v Speaker 1>under suitable conditions between the electrodes of an electrolytic cell.

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<v Speaker 1>The apparatus, called a responder, consists in a glass tube

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<v Speaker 1>similar to that of a coherer, in which are fitted

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<v Speaker 1>two electrodes, preferably of tin. The space between the electrodes,

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<v Speaker 1>about one sixty fourth of an inch, is filled with

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<v Speaker 1>a viscous semiconducting liquid such as glycerine, with a small

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<v Speaker 1>admixture of water, together with some peroxide of lead as

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<v Speaker 1>a depolarizer to prevent the excessive evolution of gas. When

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<v Speaker 1>a cell of suitable voltage is connected across this responder,

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<v Speaker 1>metallic trees or bridges are formed which make a path

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<v Speaker 1>of low resistance. But upon the passage of the jig currents,

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<v Speaker 1>these trees are broken down and the circuit broken, producing

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<v Speaker 1>a sound in a telefe phone receiver. Immediately upon the

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<v Speaker 1>cessation of the jig currents, however, these trees again establish themselves.

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<v Speaker 1>Another very successful and extremely sensitive detector was invented by

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<v Speaker 1>Fessenden and Friedland and consists of a small platinum cathode

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<v Speaker 1>containing nitric acid with a minute anode of platinum wire

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<v Speaker 1>one ten thousandth of an inch in diameter. This little

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<v Speaker 1>electrolytic cell, when polarized to the critical point by being

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<v Speaker 1>connected to a battery, is remarkably sensitive to jig currents.

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<v Speaker 1>It has been employed by Festenden in his transatlantic experiments.

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<v Speaker 1>Many other detectors have been developed which have operated successfully,

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<v Speaker 1>but those described are used most generally. It would not

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<v Speaker 1>be possible, in a few words, to give a comprehensive

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<v Speaker 1>idea of the various systems in use, as many important

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<v Speaker 1>improvements which have been made in the last ten years.

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<v Speaker 1>Those systems which have attained commercial importance are the Marconi,

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<v Speaker 1>the Festen d, the de Forest, the slaviy arco and

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<v Speaker 1>the Lodgemere head. The greatest differences are usually found in

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<v Speaker 1>the receiving apparatus. The first system used by Marconi employed

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<v Speaker 1>the coherer as a wave detector and the room wharf

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<v Speaker 1>coil to produce the sparks from which the waves were radiated.

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<v Speaker 1>The diagrammatic arrangement of the sending and receiving apparatus is

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<v Speaker 1>shown in Fig. Fifty two, T being the coherer and

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<v Speaker 1>l the telegraphic relay. Experiments with this form of apparatus

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<v Speaker 1>were first made in eighteen ninety six in England, where

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<v Speaker 1>Marconi went to obtain the assistance of Sir William Priest.

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<v Speaker 1>These experiments were so successful that trials were made during

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<v Speaker 1>the next year, at each of which something new was learned,

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<v Speaker 1>whereby the distance of transmission was increased. From some of

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<v Speaker 1>these experiments, Marconi worked out the effect of the height

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<v Speaker 1>of the antenna or aerial wire on the distance of transmission.

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<v Speaker 1>In August eighteen ninety seven, Marconi organized a company known

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<v Speaker 1>as the Wireless Telegraph and Signal Company with a capital

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<v Speaker 1>of five million dollars. In June eighteen ninety seven, Marconi

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<v Speaker 1>went to Rome, and, after having undertaken in this city

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<v Speaker 1>at the instigation of the Minister of Marine several experiments

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<v Speaker 1>from one floor to another with a conductor three yards

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<v Speaker 1>in height, was invited by the Honorable Brin, Minister of Marine,

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<v Speaker 1>to undertake in the presence of a select commission composed

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<v Speaker 1>of officers who were specialists belonging to the Royal Marines,

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<v Speaker 1>some fresh experiments. The place chosen was the Gulf of Spitzia.

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<v Speaker 1>The experiments took place between the eleventh and eighteenth of

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<v Speaker 1>July eighteen ninety seven. The apparatus made use of for

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<v Speaker 1>transmitting and receiving was similar to those employed on the

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<v Speaker 1>Bristol Channel, that is to say, aerial wires ending above

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<v Speaker 1>in metallic sheets. The coil was less powerful than that

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<v Speaker 1>used in the former case, giving sparks ten inches in

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<v Speaker 1>length only. The apparatus was located during the entire series

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<v Speaker 1>of experiments in the electrical laboratory of Saint Bartholomew and

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<v Speaker 1>bore an aerial line about seventy five feet in height,

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<v Speaker 1>which was afterward prolonged to ninety terminating in a square

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<v Speaker 1>metal sheet of about eight feet in the side. On

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<v Speaker 1>the first three days, the eleventh, twelfth, and thirteenth of July,

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<v Speaker 1>the experiments were executed on land, which gave very good

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<v Speaker 1>results up to a distance of three and a half

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<v Speaker 1>kilometers or say two miles. On the fourteenth of July,

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<v Speaker 1>the receiver was set up on board a tug having

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<v Speaker 1>a mast about fifty feet in height, which bore an

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<v Speaker 1>aerial wire of equal length ending in a sheet about

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<v Speaker 1>eight feet in the side. The transmitting station was bound

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<v Speaker 1>to carry out the following instructions ten minutes after the

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<v Speaker 1>start of the tug. It was to send for fifteen

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<v Speaker 1>minutes dots and dashes at intervals of ten seconds, then

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<v Speaker 1>transmit a phrase, maintaining between each signal and interval of

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<v Speaker 1>ten seconds. Then to suspend transmission four in an interval

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<v Speaker 1>of five minutes, after which it should go through the

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<v Speaker 1>same round, but with intervals of five seconds instead of

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<v Speaker 1>ten between each signal. The tug having started from the

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<v Speaker 1>little port of Saint Bartholomew, the receiver registered some signs

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<v Speaker 1>even before transmission had begun on land, a fact due

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<v Speaker 1>doubtless to extraneous causes. She directed her course toward the

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<v Speaker 1>western mouth of the Mole and continued to receive signals,

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<v Speaker 1>not however, in the order and in the intervals that

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<v Speaker 1>had been pre arranged, but much more frequently. The sky

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<v Speaker 1>was covered with stormy clouds, and in the distance lightning

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<v Speaker 1>was frequent. Hence it was surmised that beside the signals

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<v Speaker 1>that were really transmitted, others, due to atmospheric influence, were

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<v Speaker 1>impressing themselves, which rendered the strip of paper on which

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<v Speaker 1>they were registered illegible. On again repeating these experiments, after

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<v Speaker 1>the storm clouds had disappeared, correspondence came out very clearly,

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<v Speaker 1>up to a distance of five thousand, five hundred meters

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<v Speaker 1>nearly three miles with a tug stationary. The tug was

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<v Speaker 1>again put in motion so as to interpose between itself

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<v Speaker 1>and the station of Saint Bartholomew, the point called La Castagne,

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<v Speaker 1>in order to ascertain what effect such a screen would

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<v Speaker 1>have on signaling. The signals ceased as soon as the

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<v Speaker 1>obstacle intervened to recommence on the tug being moved from

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<v Speaker 1>its influence. On the return journey, the messages continued to

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<v Speaker 1>come out clear and exact. On the seventeenth of July,

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<v Speaker 1>trials were made from the same stations of Saint Bartholomew

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<v Speaker 1>to the armored ship San Martino, anchored at a distance

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<v Speaker 1>of about one on three quarter miles from the transmitting station,

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<v Speaker 1>the aerial conductor of which had been carried to a

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<v Speaker 1>height of about forty yards, while the ship bore at

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<v Speaker 1>the receiver an aerial line first of twenty and then

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<v Speaker 1>of thirty yards in height. Transmission succeeded perfectly independent of

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<v Speaker 1>the position of the coherer and the receiver, that is

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<v Speaker 1>to say, even if they were screened at the sending

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<v Speaker 1>station and surrounded by metallic masses under cover or placed

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<v Speaker 1>below the waterline in the ship. End of Section thirty one.
