2015
DOI: 10.1007/s12046-015-0339-9
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Closed form of optimal current waveform for class-F PA up to fourth harmonic

Abstract: In this paper, rigorous analytical derivation of the coefficients of optimal current waveform for class-F power amplifier (PA) up to fourth harmonic (dc, 1st, 2nd and 4th harmonic) is presented. The coefficients of the optimal current waveform along with related maximum attainable efficiency are provided in closed form. The results obtained are also of interest for the inverse class-F, in the case when optimal voltage waveform consists of dc, 1st, 2nd and 4th harmonic.

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Cited by 3 publications
(4 citation statements)
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“…The waveform factors in this case are not easy to be determined analytically as those of the maximally flat waveform. A technique based on Fejer-Riesz's theorem of non-negative trigonometric polynomials together with the method of Lagrange multipliers can be employed to evaluate the waveform factors after converting the problem into an optimization one for maximizing γ V 1 [17,18]. The evaluated factors for the two cases are summarized in Table 1.…”
Section: Drain Voltage With Second and Third Harmonic Tuningmentioning
confidence: 99%
“…The waveform factors in this case are not easy to be determined analytically as those of the maximally flat waveform. A technique based on Fejer-Riesz's theorem of non-negative trigonometric polynomials together with the method of Lagrange multipliers can be employed to evaluate the waveform factors after converting the problem into an optimization one for maximizing γ V 1 [17,18]. The evaluated factors for the two cases are summarized in Table 1.…”
Section: Drain Voltage With Second and Third Harmonic Tuningmentioning
confidence: 99%
“…where ( =0) is given by (8). For the prescribed conduction angle, parameter ( =0) is a function of 0( ) only, which implies that ( , =0) is also a function of 0( ) only.…”
Section: Optimal Current Waveform Of Class-f and Inverse Class-f Pamentioning
confidence: 99%
“…which further implies that optimal waveform of type ( , =0) ( ) is continuous; that is, it is of type (6). After substitution of (12) into (8) and solving the resulting equation, we obtain parameter of continuous waveform of type (6) that satisfies condition ( ) = 0, which we denote by ( =0)cont . This parameter is a function of conduction angle only:…”
Section: Optimal Current Waveform Of Class-f and Inverse Class-f Pamentioning
confidence: 99%
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