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 81 of 497 (16%)
page 81 of 497 (16%)
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string. Conceive an ordinary light string to be fixed at one end and
shaken by the hand at the other; waves will pass over the string from the shaken to the fixed end. Certain reflections will occur from the fixed end. The amount of energy which can be sent in this case from the shaken to the fixed point is small, but if the string be loaded by attaching bullets to it, uniformly throughout its length, it now may transmit much more energy to the fixed end. [Illustration: MAIN ENTRANCE AND PUBLIC OFFICE, SAN FRANCISCO HOME TELEPHONE COMPANY Contract Department on Left. Accounting Department on Right.] The addition of inductance to a telephone line is analogous to the addition of bullets to the string, so that a telephone line is said to be _loaded_ when inductances are inserted in it, and the inductances themselves are known as _loading coils_. Fig. 35 shows the general relation of Pupin loading coils to the capacity of the line. The condensers of the figure are merely conventionals to represent the condenser which the line itself forms. The inductances of the figure are the actual loading coils. [Illustration: Fig. 35. Loaded Line] The loading of open wires is not as successful in practice as is that of cables. The fundamental reason lies in the fact that two of the properties of open wires--insulation and capacity--vary with atmospheric change. The inserted inductance remaining constant, its benefits may become detriments when the other two "constants" change. |
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