{'fraction_non_alphanumeric': 0.022397891963109356, 'fraction_numerical': 0.0, 'mean_word_length': 5.178861788617886, 'pattern_counts': {'":': 0, '<': 0, '<?xml version=': 0, '>': 0, 'https://': 0, 'lorem ipsum': 0, 'www.': 0, 'xml': 0}, 'pii_count': 0, 'substrings_counts': 0, 'word_list_counts': {'cursed_substrings.json': 0, 'profanity_word_list.json': 0, 'sexual_word_list.json': 0, 'zh_pornsignals.json': 0}}
Full-wave modelling of a counterpoise

This paper proposes a distinct approach for the modeling of a counterpoise. Instead of using either finite or infinite transmission line modeling based on quasi-TEM (transverse electromagnetic) wave propagation, a full-wave modeling of a counterpoise is presented. Initially, it is summarized the development of a full-wave model from the solution of the integral equation to determine to propagation constant, γ. One advantage of the full-wave modeling is related to direct determination of the electromagnetic field in the surrounding media. From the knowledge of γ an equivalent transmission line model is derived. Time-domain responses of the ground potential rise are obtained using the Numerical Laplace Transform.