Studying the pulse regime in a reverberation chamber with a model based on image theory

Amador, Emmanuel; Lemoine, Christophe; Besnier, Philippe; Laisné, Alexandre

doi:10.1109/isemc.2010.5711330

Cited by 2 publications

(3 citation statements)

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“…A corresponding example is given in Table 1 and the explanation of the symbols is given in Table A1. The overshoot decreases with increasing QSS mean value, this is in agreement with Artz (2017). This indicates that in this case, with the appropriate choice of test parameters, over-testing will not occur.…”

Section: Resultssupporting

confidence: 85%

“…Table A1 lists all properties of interest. This algorithm works on a single chamber response, in contrast to Artz (2017) which needs to process a whole set of measurements first. The averaged downsampled envelope of the input signal s u,avg is designated as the input signal x and the averaged downsampled envelope of the chamber responseĝ u,avg is defined as the output signal y With the location of the quasi-steady state the amplitude is estimated.…”

Section: Signal Preprocessingmentioning

confidence: 99%

“…A large number of publications have already dealt with transient behaviour in RCs (Artz, 2017;Manicke and Krauthäuser, 2012;Krauthäuser and Nitsch, 2002;Amador et al, 2010).…”

Section: Introductionmentioning

confidence: 99%

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Approximation and analysis of transient responses of a reverberation chamber by pulsed excitation

2020

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Abstract. Reverberation chambers show transient behaviour when excited with a pulsed signal. The field intensities can in this case be significantly higher than in steady state, which implies that a transient field can exceed predefined limits and render test results uncertain. Effects of excessive field intensities of short duration may get covered and not be observable in a statistical analysis of the field characteristics. In order to ensure that the signal reaches steady state, the duration of the pulse used to excite the chamber needs to be longer than the time constant of the chamber. Initial computations have shown that the pulse width should be about twice as long as the time constant of the chamber to ensure that steady state is reached. The signal is sampled in the time domain with a sampling frequency according to the Nyquist theorem. The bandwidth of the input signal is determined using spectral analysis. For a fixed stirrer position, the reverberation chamber, wires, connectors, and antennas can jointly be considered as a linear time-invariant system. In this article, a procedure will be presented to extract characteristic signal properties such as rise-time, transient overshoot and the mean value in steady state from the system response. The signal properties are determined by first computing the envelope of the sampled data using a Hilbert transform. Subsequent noise reduction is achieved applying a Savitzky–Golay filter. The point where steady state is reached is then computed from the slope of the envelope by utilising a cumulative histogram. The spectral analysis is not suitable to examine the transient behaviour and determine the time constants of the system. These constants are computed applying the method of Prony, which is based on the estimation of a number of parameters in a sum of exponential functions. An alternative to the Prony Method is the Time-Domain Vector-Fit method. In contrast to the first mentioned variant, it is now also possible to determine the transfer function of the overall RC system. Differences and advantages of the methods will be discussed.

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Section: Resultssupporting

confidence: 85%

Section: Signal Preprocessingmentioning

confidence: 99%