Electric Oscillations And Electric Waves With Application to Radiotelegraphy An
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11 3. 1416=7r 0. 333 2. 004 0. 13 3. 1416=ir 0. 273 2. 005 0. 15 3. 1416=*- 0. 223 2. 01 0. 20 3. 1416=7r 0. 135 2. 02 0. 29 3. 1416=7r 0. 055 2. 04 0. 40 3. 1416=7r . .. .. . 0. 0183 2. 10 0. 63 3. 1416=*- 0. 00184 2. 20 0. 89 3. 1416=*- 0. 00014 308 ELECTRIC OSCILLATIONS [CHAP. XVI Table HI. Resistanceless Line of Type III, with no Magnetic Leakage Retardation Angle of Current per Section, and Time Lag T of Current per Section. The Attenuation Constant is Zero Throughout LI = Series Inductan...ce per Loop L = Series Inductance per Coils C 2 = Shunt Capacity per Coil uVLiCt CO\/LC2
To quickly assess the difficulty of the text, read a short excerpt:
11 3. 1416=7r 0. 333 2. 004 0. 13 3. 1416=ir 0. 273 2. 005 0. 15 3. 1416=*- 0. 223 2. 01 0. 20 3. 1416=7r 0. 135 2. 02 0. 29 3. 1416=7r 0. 055 2. 04 0. 40 3. 1416=7r . .. .. . 0. 0183 2. 10 0. 63 3. 1416=*- 0. 00184 2. 20 0. 89 3. 1416=*- 0. 00014 308 ELECTRIC OSCILLATIONS [CHAP. XVI Table HI. Resistanceless Line of Type III, with no Magnetic Leakage Retardation Angle of Current per Section, and Time Lag T of Current per Section. The Attenuation Constant is Zero Throughout LI = Series Inductan...ce per Loop L = Series Inductance per Coils C 2 = Shunt Capacity per Coil uVLiCt CO\/LC2
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