The Application of Hyperbolic Functions to Electrical Engineering Problems Bein
The Application of Hyperbolic Functions to Electrical Engineering Problems Bein
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In our eReader you can find the full English version of the book. Read The Application of Hyperbolic Functions to Electrical Engineering Problems Bein Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book The Application of Hyperbolic Functions to Electrical Engineering Problems Bein
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, of which by (23), page 15, the sending-end resistance at A when grounded at B is R M = z o tanh 140688 = 1273'633 ohms . . . (56) Proceeding in this way, we should find that in every respect the artificial line would behave in the steady state exactly like a real smooth line of surge-resistance z and angle Su hyps. Along and within the artificial line, the distribution of potential, current, resistance, power and energy would not be the same as in the corresponding smooth line; except at sect...ion junctions, where the agreement would be complete, each section being the external counterpart of a smooth line having a surge-resistance V 1 + 1= 2 J V^fp ohms L (57) and an angle = 2 u = 2 sinh-' ( 9 >) = 2 sinh-' ('J - ')hyps. L (58) which means that each section of artificial line is the equivalent T of the corresponding section of actual smooth line. See page 35, where // = r 1 /2.
If each T-section of the artificial line, in the case considered, represented 100 km. Of actual smooth line ; then the actual line of 400 km.
What to read after The Application of Hyperbolic Functions to Electrical Engineering Problems Bein?
You can find similar books in the "Read Also" column, or choose other free books by Arthur E Arthur Edwin Kennelly to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
, of which by (23), page 15, the sending-end resistance at A when grounded at B is R M = z o tanh 140688 = 1273'633 ohms . . . (56) Proceeding in this way, we should find that in every respect the artificial line would behave in the steady state exactly like a real smooth line of surge-resistance z and angle Su hyps. Along and within the artificial line, the distribution of potential, current, resistance, power and energy would not be the same as in the corresponding smooth line; except at sect...ion junctions, where the agreement would be complete, each section being the external counterpart of a smooth line having a surge-resistance V 1 + 1= 2 J V^fp ohms L (57) and an angle = 2 u = 2 sinh-' ( 9 >) = 2 sinh-' ('J - ')hyps. L (58) which means that each section of artificial line is the equivalent T of the corresponding section of actual smooth line. See page 35, where // = r 1 /2.
If each T-section of the artificial line, in the case considered, represented 100 km. Of actual smooth line ; then the actual line of 400 km.
What to read after The Application of Hyperbolic Functions to Electrical Engineering Problems Bein?
You can find similar books in the "Read Also" column, or choose other free books by Arthur E Arthur Edwin Kennelly to read onlineMoreLess
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