Theory And Calculation of Transient Electric Phenomena And Oscillations 8

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Theory And Calculation of Transient Electric Phenomena And Oscillations 8
Charles Proteus Steinmetz
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(5) Zr = 1 inch = 2.54 cm.
Zi — Z2 = 16 cm.
A = 4.6 cm.« = 6.85 that of (1) to (4).
Table II gives the values of ro, n, rg, r2, Xo, Xi, xz, x^, ri + rz, r\ + r2, Xi + xz, x\ + x^y «, cos w, e and Zp, for / = 10* cycles.
Table III gives the values of ri + rz or ri + r2, 2, cos cu and 6, for/ * 60, 10*, 10«, 10«, 10^ cycles for the five kinds of conduc- tors.
96. It is interesting to compare in Table III, the constants of the first four conductors, as they have the same section, repre- senting ab
...out average section of transmission conductors, but represent two shapes, round wire and thin flat ribbon, and two kinds of material, copper — high conductivity and non-magnetic — and iron —magnetic material of medium conductivity.
As seen, the effect of conductor shape and conductor material is very great at machine frequencies, 60 cycles, but becomes small and almost negligible at extremely high frequencies. This is rather against the usual assumption.
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