Cyclopedia of Telephony & Telegraphy Vol. 1 - A General Reference Work on Telephony, etc. etc. by Robert Millikan;Samuel McMeen;George Patterson;Kempster Miller;Charles Thom
page 114 of 497 (22%)
page 114 of 497 (22%)
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just discussed employs but a single electromagnet by which the initial
magnetization of the cores and also the variable magnetization necessary for speech reproduction is secured. The problem of the direct-current receiver has been attacked in another way by Ernest E. Yaxley, of the Monarch Telephone Manufacturing Company, with the result shown in Fig. 54. The construction in this case is not unlike that of an ordinary permanent-magnet receiver, except that in the place of the permanent magnets two soft iron cores _1-1_ are employed. On these are wound two long bobbins of insulated wire so that the direct current flowing over the telephone line will pass through these and magnetize the cores to the same degree and for the same purpose as in the case of permanent magnets. These soft iron magnet cores _1-1_ continue to a point near the coil chamber, where they join the two soft iron pole pieces _2-2_, upon which the ordinary voice-current coils are wound. The two long coils _4-4_, which may be termed the direct-current coils, are of somewhat lower resistance than the two voice-current coils _3-3_. They are, however, by virtue of their greater number of turns and the greater amount of iron that is included in their cores, of much higher impedance than the voice-current coils _3-3_. These two sets of coils _4-4_ and _3-3_ are connected in multiple. As a result of their lower ohmic resistance the coils _4-4_ will take a greater amount of the steady current which comes over the line, and therefore the greater proportion of the steady current will be employed in magnetizing the bar magnets. On account of their higher impedance to alternating currents, however, nearly all of the voice currents which are superposed on the steady currents, flowing in the line will pass through the voice-current coils _3-3_, and, being near the diaphragm, these currents will so vary the steady magnetism in the cores _2-2_ as to produce the necessary vibration of the diaphragm. |
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