1951
DOI: 10.1109/jrproc.1951.231835
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Some General Properties of Magnetic Amplifiers

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Cited by 12 publications
(1 citation statement)
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“…The impedance matrix of the perturbing element on the right side is, to second order: Zu = -R( 1 -,6!~) Z,a = R~n Z, 5 Also to second order, the circuit equations are LI + _b_ (1 + _!_ dp,) and a phase angle 1r /2. In a global fashion, this solution gives the full sweep of the behavior of the Van der Pol equation, subject only to the restriction that the perturbations remain pertyrbations, i.e., that too large values of the initial 1° be avoided.…”
Section: Examplesmentioning
confidence: 99%
“…The impedance matrix of the perturbing element on the right side is, to second order: Zu = -R( 1 -,6!~) Z,a = R~n Z, 5 Also to second order, the circuit equations are LI + _b_ (1 + _!_ dp,) and a phase angle 1r /2. In a global fashion, this solution gives the full sweep of the behavior of the Van der Pol equation, subject only to the restriction that the perturbations remain pertyrbations, i.e., that too large values of the initial 1° be avoided.…”
Section: Examplesmentioning
confidence: 99%