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Chapter 16: Induction Motor

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FieldValue
SourceTheory and Calculation of Alternating Current Phenomena
Year1900
Section IDtheory-calculation-alternating-current-phenomena-1900-chapter-16
Locationlines 13649-16361
Statuscandidate
Word Count10739
Equation Candidates In Section0
Figure Candidates In Section4
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CHAPTER XVI. INDUCTION MOTOR. 151. A specialization of the general alternating-current transformer is the induction motor. It differs from the stationary alternating-current transformer, which is also a specialization of the general transformer, in so far as in the stationary transformer only the transfer of electrical energy from primary to secondary is used, but not the mechanical force acting between the two, and therefore primary and secondary coils are held rigidly in position with regard to each other. In the induction motor, only the mechanical force between primary and secondary is used, but not the transfer of electrical energy, and thus the secondary circuits closed upon themselves. Transformer and induction motor thus are the two limiting cases of the general alternating- current transformer. Hence the induction motor consists of a magnetic circuit interlinked with two electric
... and secondary is used, but not the transfer of electrical energy, and thus the secondary circuits closed upon themselves. Transformer and induction motor thus are the two limiting cases of the general alternating- current transformer. Hence the induction motor consists of a magnetic circuit interlinked with two electric circuits or sets of circuits, the primary and the secondary circuit, which are movable with regard to each other. In general a num- ber of primary and a number of secondary circuits are used, angularly displaced around the periphery of t ...
... rcuit reduced to primary system; if // = secondary current per circuit, fl= — = secondary current per circuit reduced to primary system ; if r^ = secondary resistance per circuit, rt = a2 r{ = secondary resistance per circuit reduced to primary system ; if x± = secondary reactance per circuit, xt = a2 x\ = secondary reactance per circuit reduced to primary system ; if £/ = secondary impedance per circuit, z1 = azz\ = secondary impedance per circuit reduced to primary system ; that is, the number of secondary circuits and of turns per secondary cir ...
... to retain secondary circuits in inductive relation to primary circuits and vice versa, in spite of their relative motion. The result of the relative motion between primary and secondary is, that the E.M.Fs. induced in the secondary or the motor armature are not of the same frequency as the E.M.Fs. impressed upon the primary, but of a frequency which is the difference between the impressed frequency 238 ALTERNATING-CURRENT PHENOMENA. and the frequency of rotation, or equal to the "slip," that is, the difference between synchronism and speed (in cycle ...
CHAPTER XVI. INDUCTION MOTOR. 151. A specialization of the general alternating-current transformer is the induction motor. It differs from the stationary alternating-current transformer, which is also a specialization of the general transformer, in so far as in the stationary transformer only the transfer of electrical energy from primary to secondary is used ...
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theory-calculation-alternating-current-phenomena-1900-fig-115EOG Fig. 115. 156. Thus far the diagram is essentially the same asline 14010
theory-calculation-alternating-current-phenomena-1900-fig-119ӣ> Fig. 119. Again, a maximum torque point and a maximum outputline 14959
theory-calculation-alternating-current-phenomena-1900-fig-120267 Fig. 120. 268 ALTERNATING-CURRENT PHENOMENA.line 14974
theory-calculation-alternating-current-phenomena-1900-fig-1221000 2000 3COO 4000 fiOOO fiOOO 7000 8000 Fig. 122. Voltampere output,line 15137
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