Survey
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Coupling between the Crust and the Ionosphere prior to Earthquakes 1,2 1 3,4 2 5 Friedemann Freund , Yvonne Cagle , Brian Shiro , Stuart Pilorz , Phillip Hollis-Watts , Chris Windsor 1. NASA Ames Research Center, 2. SETI Institute, 3. NOAA Pacific Tsunami Warning Center, 4. Astronauts4Hire, 5. Western Australia School of Mines (contact: [email protected]) Introduction. When tectonic stresses build up in the Earth’s crust prior to major earthquakes, electronic charge carriers are activated in the stressed rocks. The charge carriers of interest are defect electrons in the oxygen anion sublattice of rock-forming minerals, known as positive holes, symbolized by h• [1]. The h• have the remarkable ability to spread out of the stressed rocks into the surrounding unstressed rocks, traveling fast and far, meters in the laboratory, tens of kilometers in the field. Upon arrival at the Earth surface in sufficiently large numbers, they cause air molecules to become field-ionized, causing the injection of massive amounts of airborne ions at the ground-to-air interface, sometimes exclusively positive [2]. Atmospheric Effects. The air volume heavily laden with positive ions expands upward, probably to stratospheric heights, dragging along Earth’s ground potential (Figure 1). In response to the changing vertical electric field the ionospheric plasma responds by increasing the Total Electron Content (TEC) at its lower edge [3]. 5 toward the ionosphere, forming a distributed ion current through the mesosphere [4]. Likewise electrons will be accelerated downward from the lower edge of the ionosphere. These vertical currents will couple to the Earth’s magnetic field, forcing the ions and electrons onto spiraling trajectories. At some critical current density magneto-hydro-dynamic theory predicts that the smooth, distributed currents will break up into bunches, forming bubbles of higher charge densities separated by regions of lower charge densities or of opposite sign. This will result in strong electric fields causing electric discharges in the mesosphere. Ground Observations. Evidence for bursts of millisec discharges over regions of impending earthquake activity in SW Australia, Indonesia and the South Pacific – and over active volcanoes undergoing a Plinian eruption – has been obtained by Hollis-Watts at Perth, Australia, using a directional antenna recording signals over a wide frequency range, from 10 kHz to 1.3 GHz [5]. The signals and their polarization are consistent with mesospheric lightning strikes. Conclusion. We propose to use suborbital vehicles to traverse the mesosphere during times of such electric activity to measure (i) electric fields along the flight path, (ii) ion concentrations, (iii) electron concentrations. References. [1] Freund, F. T. (2010), Towards a unified solid state theory for pre-earthquake signals, Acta Geophysica, 58, 719-766. [2] Freund, F. T., et al. (2009), Air ionization at rock surface and pre-earthquake signals, J. Atmospheric Solar Terrestrial Physics, 71, 1824–1834. Figure 1: Injection of positive airborne ions at the • ground-to-air interface, due to stress-activated h charge carriers arriving at the Earth surface from below, and upward expansion of the ionized air, causing a response in the ionospheric plasma. We predict that positive air ions at the upper edge of the stratosphere will be accelerated upward [3] Liu, J. Y., et al. (2004), Pre-earthquake ionospheric anomalies registered by continuous GPS TEC measurements, Annales Geophysicae, 22, 1585-1593. [4] Pulinets, S., and K. Boyarchuk (2004), Ionospheric Precursors of Earthquakes, 350 pp., Springer, Heidelberg. [5] Pulinets, S., and P. Hollis-Watts (2003), P-H pulses - the new type of seismoelectromagnetic emission, Geophysical Research Abstr., 5, 07035.