1987
DOI: 10.1109/tcs.1987.1086167
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Analysis of a symmetrically stabilized three-phase oscillator and some of its applications

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Cited by 8 publications
(2 citation statements)
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“…It can be shown that the following solution is a possible steady state solution of (4): X k = A c o s [ w t + ( k -l ) n / 2 + $ ] , k = 1,2,3,4(modulo4) ( 5 ) where A = 111~. On one hand ( 5 ) satisfies the linear conservative parts of (4), namely it satisfies (1). On the other hand it nulls the terms of the square brackets in (4).…”
Section: Introductionmentioning
confidence: 99%
“…It can be shown that the following solution is a possible steady state solution of (4): X k = A c o s [ w t + ( k -l ) n / 2 + $ ] , k = 1,2,3,4(modulo4) ( 5 ) where A = 111~. On one hand ( 5 ) satisfies the linear conservative parts of (4), namely it satisfies (1). On the other hand it nulls the terms of the square brackets in (4).…”
Section: Introductionmentioning
confidence: 99%
“…Except for the change of notation and a change arising from a different sign convention for the unperturbed terms, this is the solution found by Daboul et ai. 6 Note that (a) the coefficients of all the perturbation terms in equations (15a-c) are real, so there is no frequency (b) the unperturbed mode zl = A1 exp(j w , f ) , zo = 0, with a particular value of I A1 1, is a solution.…”
Section: Selection Rule For Terms Of Zrmentioning
confidence: 99%