Ultra-Wideband, Short-Pulse Electromagnetics 2 1995
DOI: 10.1007/978-1-4899-1394-4_32
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Distortion of Fast Pulses by Non-Tem Effects in Coaxial Cables

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Cited by 6 publications
(6 citation statements)
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“…Therefore, for such nozzle geometry and an interrogation pulse with FWHM value of 0.5 ns, all the frequency components, from 0.913 GHz up to 2 GHz will create TE 11 mode microwaves. This TE 11 mode will be generated at imperfections in the nozzle, and will propagate with a different phase velocity interfering with the TEM mode [5]. It is this interference between the TEM and the TE 11 mode associated with the frequencies higher than fc which will give standing waves evidenced by the ringing effect.…”
Section: Design Methodologymentioning
confidence: 96%
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“…Therefore, for such nozzle geometry and an interrogation pulse with FWHM value of 0.5 ns, all the frequency components, from 0.913 GHz up to 2 GHz will create TE 11 mode microwaves. This TE 11 mode will be generated at imperfections in the nozzle, and will propagate with a different phase velocity interfering with the TEM mode [5]. It is this interference between the TEM and the TE 11 mode associated with the frequencies higher than fc which will give standing waves evidenced by the ringing effect.…”
Section: Design Methodologymentioning
confidence: 96%
“…Related to the characterization of the interrogation pulse in the frequency domain, as an example, in Fig.3, we present the Fast Fourier Transform of a positive Gaussian pulse V o (t) with a FWHM value of 0.5 ns. Related to the characterization of microwave propagation modes which can be present in coaxial transmission lines of different inner (d) and outer (D) diameters of the conductors, it is well known [5] that beyond the TEM mode with a cut-off frequency of 0 Hz, the next possible mode is TE 11 , which has a frequency cut-off: f c (GHz) =190.85/[(D+d)*Ɛ r 1/2 ], with D and d given in mm [5,6]. This cut-off frequency means that the entire frequency spectrum of the interrogation pulse should be below f c , if we want to preserve a clean TEM mode during pulse propagation along the chain.…”
Section: Design Methodologymentioning
confidence: 99%
“…We can view the coefficients s m,n as entries in an M × N matrix S M ×N matrix whose row and column indices range over 0 ≤ m < M, 0 ≤ n < N respectively. The DAC performs the mapping s n → p n (t) according to (10) where s n is the n th column of S M ×N . The Fourier transform of p n (t) in (10), which is required to carry out the waveform selection procedure, is…”
Section: A Uwb Pulse Generatormentioning
confidence: 99%
“…We assume in the sample computations done here that the transmission line behaves like an ideal all-pass filter across the measurement band and can be ignored. Distortion of ultra fast pulses in transmission lines has been studied [10] and results have shown that distortions do occur if precautions are not taken.…”
Section: Filtering In the Dacmentioning
confidence: 99%
“…Above TEM cutoff, higher order modes can contribute to the usable spectrum for short pulse, fast risetime signals if certain effects are ignorable or controlled for [119].…”
Section: Comparative Performancementioning
confidence: 99%