Abstract

AbstractBased on experimental results of recent years, this article presents a qualitative description of a possible mechanism (termed the Mechanism) covering the main stages of lightning initiation, starting before and including the initiating event, followed by the initial electric field change (IEC), followed by the first few initial breakdown pulses (IBPs). The Mechanism assumes initiation occurs in a region of ~1 km3 with average electric field E > 0.3 MV/(m·atm), which contains, because of turbulence, numerous small “Eth volumes” of ~10−4–10−3 m3 with E ≥ 3 MV/(m·atm). The Mechanism allows for lightning initiation by either of two observed types of events: a high‐power, very high frequency (VHF) event such as a Narrow Bipolar Event or a weak VHF event. According to the Mechanism, both types of initiating events are caused by a group of relativistic runaway electron avalanche particles (where the initial electrons are secondary particles of an extensive air shower) passing through many Eth volumes, thereby causing the nearly simultaneous launching of many positive streamer flashes. Due to ionization‐heating instability, unusual plasma formations (UPFs) appear along the streamers' trajectories. These UPFs combine into three‐dimensional (3‐D) networks of hot plasma channels during the IEC, resulting in its observed weak current flow. The subsequent development and combination of two (or more) of these 3‐D networks of hot plasma channels then causes the first IBP. Each subsequent IBP is caused when another 3‐D network of hot plasma channels combines with the chain of networks caused by earlier IBPs.

Highlights

  • Despite great efforts by the scientific community, there is still no generally accepted, qualitatively consistent mechanism of lightning initiation from the initiating event through the subsequent development to the beginning of a stepped leader (e.g., Rakov & Uman, 2003; Gurevich & Zybin, 2001; Dwyer & Uman, 2014)

  • As we show an narrow bipolar event (NBE) begins with a superposition of a large number of positive streamer flashes that occur in most of the Eth-volumes

  • From the point of view of the Mechanism, it is likely that precursors and 1169 isolated NBEs develop with the NBE-initiating event (IE) Mechanism, but their EE-volumes have only small 1170 Estr+-volumes, so that the 1171 development of large unusual plasma formations (UPFs) networks and bidirectional leaders cannot occur, thereby 1172 preventing initial breakdown pulses (IBPs) from occurring

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Summary

Introduction

Despite great efforts by the scientific community, there is still no generally accepted, qualitatively consistent mechanism of lightning initiation from the initiating event through the subsequent development to the beginning of a stepped leader (e.g., Rakov & Uman, 2003; Gurevich & Zybin, 2001; Dwyer & Uman, 2014) This situation is partly due to the exceptional complexity of the lightning phenomenon, which requires both experimental and theoretical knowledge about lightning itself, along with information from high-energy atmospheric physics, radio physics of atmospheric discharges, physics of turbulent multiphase charged aerosols, gas discharge physics at high pressure, and physics of long sparks.

Experimental and theoretical basis of the Mechanism
Conditions and Phenomena which the Mechanism Should Satisfy and Explain
Some Main Components of the Mechanism
Positive streamer flashes
The front and duration of a typical individual positive streamer flash
The first streamer flash of Figure
Length and conductivity of long streamers
Corona from hydrometeors producing the group of positive streamer flashes
The Mechanism
The Weak-IE Mechanism for lightning initiation
Comparison of Weak-IE
Findings
CONCLUSIONS
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