The electric field in the lower part of the thundercloud plays a key role in developing the relativistic runaway electron avalanches (RREAs), which reaching and are registered on the Earth's surface as thunderstorm ground enhancements (TGEs). Different species of cosmic rays, which include electrons, positrons, muons, gamma rays, and neutrons, were directly or nondirectly modulated by the intracloud electric field and comprise multisensory messengers bringing information on the electric fields emerging in the thundercloud. Recently, we used the measurements of the near-surface (NS) electric field, the graupel fall, and the energy spectra of electrons and gamma rays to get insight into the charge structure of the lower dipole and to estimate the maximum electric field in the thundercloud (Chilingarian et al., 2021a(Chilingarian et al., , 2021c. We considered the depletion of the muon flux as an evidence of a large negative electric field in the lower part of the thundercloud, which accelerates electrons downward and initiates electron-gamma ray avalanches. As a basic configuration of the thundercloud charge structure, we accept a classical tripole (Kuettner, 1950). For a normal three-layered tripole, the lower positively charged region (LPCR) has a smaller size and smaller charge than the upper main layers, negatively (MN) and positively charged (MP). However, alternative charge configurations were reported (see Rust et al., 2005, and references therein) inverted polarity dipole (Nag & Rakov, 2012), i.e., charge regions having a positive charge above the negative one in the vertical distribution of charge. Such structures are rare and rather difficult to identify. In the famous work (Nag & Rakov, 2009), authors conclude that the occurrence of pronounced preliminary breakdown (PB) pulse train proves the existence of an unusually large LPCR.We outline two main scenarios (Chilingarian et al., 2020) supporting the origination of the large fluxes of electrons and gamma rays measured by the particle detectors and spectrometers located on the mountain altitudes. The first one is related to the large main negative charge above the detectors site at an altitude of