Alternating Current Engineering Practically Treated
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In our eReader you can find the full English version of the book. Read Alternating Current Engineering Practically Treated 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 Alternating Current Engineering Practically Treated
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M. F. 's, EI, EH, E m, acting together in the armature circuit, and when added, proper consideration being given to THE REPULSION MOTOR.
the relative phases of each to the other, the vector sum must equal zero, since the brushes are short-circuited by an external wire of zero resistance. Another con- ception is that the e. M. F. Of rotation, E m, minus the back e. M. F. Of flux pulsation, E 1? gives a resulting e. M. F. , which, acting through the impedance of the secondary circuit, is entirely... consumed.
Thus, the equation of the secondary is E l + E n + E m = o, the various E's being computed as has been shown. Thus the fundamental equations of the repul- sion motor are: (1) o = IO C h 4. 44 ^n 10 h from which all the values of horse-power, torque, etc. , may be computed as has been illustrated in the case of Fig. 82.
the induction motor. The time phases of these vari- ous values are shown in the following figures. First, in Fig. 82 is shown for the primary the phase i86 ALTERNATING CURRENT ENGINEERING.
What to read after Alternating Current Engineering Practically Treated?
You can find similar books in the "Read Also" column, or choose other free books by Edward Brackett Raymond to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
M. F. 's, EI, EH, E m, acting together in the armature circuit, and when added, proper consideration being given to THE REPULSION MOTOR.
the relative phases of each to the other, the vector sum must equal zero, since the brushes are short-circuited by an external wire of zero resistance. Another con- ception is that the e. M. F. Of rotation, E m, minus the back e. M. F. Of flux pulsation, E 1? gives a resulting e. M. F. , which, acting through the impedance of the secondary circuit, is entirely... consumed.
Thus, the equation of the secondary is E l + E n + E m = o, the various E's being computed as has been shown. Thus the fundamental equations of the repul- sion motor are: (1) o = IO C h 4. 44 ^n 10 h from which all the values of horse-power, torque, etc. , may be computed as has been illustrated in the case of Fig. 82.
the induction motor. The time phases of these vari- ous values are shown in the following figures. First, in Fig. 82 is shown for the primary the phase i86 ALTERNATING CURRENT ENGINEERING.
What to read after Alternating Current Engineering Practically Treated?
You can find similar books in the "Read Also" column, or choose other free books by Edward Brackett Raymond to read onlineMoreLess
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