FIG. 56.--ELECTROMAGNETS OF RELAY, AND THEIR EFFECTS.

Take from an ordinary relay a coil, with its iron core, half the

electromagnet, so to speak, without any yoke or armature. Connect it

up as described, and observe the throw given to the galvanometer. The

amount of throw obtained from the single coil was taken as unity, and

all others were compared with it. If you join up two such coils as

they are usually joined, in series, but without any iron yoke across

the cores, the throw was 17. Putting the iron yoke across the cores,

to constitute a horseshoe form, 496 was the throw; that is to say, the

tendency of this electromagnet to retard the current was 496 times as

great as that of the simple coil. But when an armature was put over

the top, the effect ran up to 2,238. By the mere device of putting the

coils in parallel, instead of in series, the 2,238 came down to 502, a

little less than the quarter value which would have been expected.

Lastly, when the armature and yoke were both of them split in the

middle, as is done in fact in all the standard patterns of the British

postal telegraph relays, the throw of the galvanometer was brought

down from 502 to 26. Relays so constructed will work excessively

rapidly. Mr. Preece states that with the old pattern of relay having

so much self-induction as to give a galvanometer throw of 1,688, the

speed of signaling was only from 50 to 60 words per minute, whereas,

with the standard relays constructed on the new plan, the speed of

signaling is from 400 to 450 words per minute. It is a very

interesting and beautiful result to arrive at from the experimental

study of these magnetic circuits.

SHORT CORES _versus_ LONG CORES.

In considering the forms that are best for rapid action, it ought to

be mentioned that the effects of hysteresis in retarding changes in

the magnetization of iron cores are much more noticeable in the case

of nearly closed magnetic circuits than in short pieces.

Electromagnets with iron armatures in contact across their poles will

retain, after the current has been cut off, a very large part of their

magnetism, even if the cores be of the softest of iron. But so soon as

the armature is wrenched off, the magnetism disappears. An air gap in

a magnetic circuit always tends to hasten demagnetizing. A magnetic

circuit composed of a long air path and a short iron path demagnetizes

itself much more rapidly than one composed of a short air path and a

long iron path. In long pieces of iron the mutual action of the

various parts tends to keep in them any magnetization that they may

possess; hence they are less readily demagnetized. In short pieces,

where these mutual actions are feeble or almost absent, the

magnetization is less stable, and disappears almost instantly on the

cessation of the magnetizing force. Short bits and small spheres of

iron have no magnetic memory. Hence the cause of the commonly received

opinion among telegraph engineers that for rapid work electromagnets

must have short cores. As we have seen, the only reason for employing

long cores is to afford the requisite length for winding the wire

which is necessary for carrying the needful circulation of current to

force the magnetism across the air gaps. If, for the sake of rapidity

of action, length has to be sacrificed, then the coils must be heaped

up more thickly on the short cores. The electromagnets in American

patterns of telegraphic apparatus usually have shorter cores, and a

relatively greater thickness of winding upon them, than those of

European patterns.

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Scientific American Supplement, No. 787, January 31, 1891 · 第 38 / 71 题