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Chapter 10: Mutual Inductance

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FieldValue
SourceTheory and Calculation of Transient Electric Phenomena and Oscillations
Year1909
Section IDtheory-calculation-transient-electric-phenomena-oscillations-chapter-32
Locationlines 10475-12216
Statuscandidate
Word Count5572
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CHAPTER X. MUTUAL INDUCTANCE. 82. In the preceding chapters, circuits have been considered containing resistance, self-inductance, and capacity, but no mutual inductance; that is, the phenomena which take place in the circuit have been assumed as depending upon the impressed e.m.f. and the constants of the circuit, but not upon the phenomena taking place in any other circuit. Of the magnetic flux produced by the current in a circuit and interlinked with this circuit, a part may be interlinked with a second circuit also, and so by its change generate an e.m.f. in the second circuit, and part of the magnetic flux produced by Fig. 38. Mutual inductance between circuits. the current in a second circuit and interlinked with the second circuit may be interlinked also with the first circuit, and a change of current
... h other symmetrically, or reduced thereto; that is, where the mutual inductance is due to coils enclosed in the first circuit, interlinked magnetically with coils enclosed in the second circuit, as the primary and the secondary coils of a transformer, or a shunt and a series field winding of a generator, 144 TRANSIENT PHENOMENA the two coils are assumed as of the same number of turns, or reduced thereto. ri, No. turns second circuit If a = — = — =rr— — - -- : - r— , the currents in the nA No. turns first circuit second circuit are multiplied, ...
... , self-inductance, and capacity, but no mutual inductance; that is, the phenomena which take place in the circuit have been assumed as depending upon the impressed e.m.f. and the constants of the circuit, but not upon the phenomena taking place in any other circuit. Of the magnetic flux produced by the current in a circuit and interlinked with this circuit, a part may be interlinked with a second circuit also, and so by its change generate an e.m.f. in the second circuit, and part of the magnetic flux produced by Fig. 38. Mutual inductance between ci ...
... hen generates an e.m.f. in the first circuit. Diagrammatically the mutual inductance between two circuits can be sketched as shown by M in Fig. 38, by two coaxial coils, while the self-inductance is shown by a single coil L, and the resistance by a zigzag line. 141 142 TRANSIENT PHENOMENA The presence of mutual inductance, with a second circuit, introduces into the equation of the circuit a term depending upon the current in the second circuit. If i^ = the current in the circuit and r1 = the resistance of the circuit, then r^\ = the e.m.f. consum ...
... it, we have di L{j± = e.m.f. consumed by the inductance, ctt where, t = time. If instead of time t an angle 6 = 2 nft is introduced, where / is some standard frequency, as 60 cycles, di x. 3^ = e.m.f. consumed by the inductance, au where x1 = 2 nfL^ = inductive reactance. If now M = mutual inductance between the circuit and another circuit, that is, number of interlinkages of the circuit with the magnetic flux produced by unit current in the second circuit, and i2 = the current in the second circuit, then M—~= e.m.f. consumed by mutual in ...
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