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Vol 13, No 2 (2019)

Article

Hydrogeoseismological Research in Kamchatka: 1977–2017

Kopylova G.N., Boldina S.V.

Abstract

This paper is concerned with the main stages in the setting-up and technical development of a system specializing in physical and chemical parameters of groundwater at a network of wells and springs in the Petropavlovsk Geodynamic Test Area, Kamchatka. The focus is on a description of hydrogeochemical and hydrogeodynamic precursors to Kamchatka earthquakes (Мw = 6.6–7.8) that occur a few weeks to a few months before a seismic event, manifesting themselves in anomalous changes in chemical composition and groundwater level. The precursors are discussed in application to their use at specialized councils on earthquake prediction. It is shown that the system of automated observation of groundwater parameters at wells as developed at the Kamchatka Branch of the Geophysical Survey of the Russian Academy of Sciences (KB GS RAS) is capable of identifying hydrogeodynamic precursors of water level in near real time and of providing, in some particular cases, quantitative estimates of pre-seismic and coseismic of deformation in water-saturated rocks. This can be useful in geophysical monitoring and intermediate-term prediction of strong earthquakes for the Kamchatka region.

Journal of Volcanology and Seismology. 2019;13(2):71-84
pages 71-84 views

Using the Paratunsky Geothermal Field to Provide Heating for Kamchatka

Kiryukhin A.V., Zhuravlev N.B.

Abstract

The Paratunsky geothermal field has been in operation since 1964, mostly in a self-flowing mode, with a discharge rate of approximately 250 kg/s of thermal water at temperatures of 70‒90°С (47 MW, with the waste water having a temperature of 35°С). The water drawn from the field is used for local heating, spa heating, and for greeneries in the villages of Paratunsky and Termal’nyi (3000 residents). The potential market of thermal energy in Kamchatka includes Petropavlovsk-Kamchatskii (180 000 residents), Elizovo (39 000), and Vilyuchinsk (22 000). The heat consumption in the centralized heating systems for Petropavlovsk-Kamchatskii is 1 623 000 GCal per annum (216 MW). A thermohydrodynamic model developed previously is used to show that the Paratunsky geothermal reservoir can be operated in a sustainable mode using submersible pumps at an extraction rate of as much as 1375 kg/s, causing a moderate decrease in pressure (by no more than 8 bars) and temperature (by no more than 4°С) in the reservoir. Additional geothermal sources of heat energy may include the Verkhne-Paratunsky and Mutnovsky geothermal fields.

Journal of Volcanology and Seismology. 2019;13(2):85-95
pages 85-95 views

Volcanism and the Geochemistry of Soil and Vegetation in Kamchatka. Part 1. Some Geochemical Features of Near-Surface Volcanic Ashes

Zakharikhina L.V., Litvinenko Y.S.

Abstract

The common geochemical features of Kamchatka near-surface ashes (ashes that underlie surface organogenic soil horizons) include their depletion in most chemical elements compared with the average figures for volcanic rocks of the same composition and their relative enrichment in a narrow range of elements, mostly those which are typomorphic for basic rocks (Р, Mg, V, Cr, Cu, Zn, Zr, and Sb). Viewed upon the background of small variations in the concentrations of chemical elements in ashes from different areas in the peninsula, the range of their dominant elements is controlled by their petrochemical composition. The vigorous activity of Kamchatka’s Northern Group of Volcanoes has produced relatively higher concentrations of mobile forms of elements in the near-surface ashes of the Northern Province compared with the ashes found in the southern part of the peninsula.

Journal of Volcanology and Seismology. 2019;13(2):96-106
pages 96-106 views

The Evolution of Gas Hydrate Accumulations in Zones of Deep-Sea Mud Volcanoes

Sobisevich A.L., Suetnova E.I., Zhostkov R.A.

Abstract

This paper considers the evolution of gas hydrate accumulation that occurs at deep mud volcanoes. We present a mathematical model and results from numerical simulation of gas hydrate accumulation on the seafloor in deep-seated structures of submarine mud volcanoes. We made a quantitative study of how the depth of a feeding reservoir and the pressure in it can affect the evolution of gas hydrate accumulation at deep mud volcanoes. Numerical simulation showed that the hydrate saturation in zones of submarine mud volcanoes is not constant and its evolution is affected by the geophysical properties of the bottom (temperature gradient, porosity, permeability, and physical properties of the sediment) and by the depth of the feeding reservoir and the pressure in it, with the rate of hydrate accumulation being some tens or hundreds of times greater than that in sedimentary basins at passive continental margins.

Journal of Volcanology and Seismology. 2019;13(2):107-111
pages 107-111 views

The MW 7.8 Earthquake of July 17, 2017 off the Commander Islands and Other Large Earthquakes at the Western Segment of the Aleutian Island Arc

Rogozhin E.A., Dontsova G.Y., Zhukovets V.N., Lutikov A.I.

Abstract

This paper discusses the tectonic setting, seismological characteristics, and the aftershock process for the great (MW = 7.8) Near-Islands Aleutian earthquake of July 17, 2017 off the Commander Islands. Our analysis showed that the rupture zone as inferred from the distribution of aftershock epicenters in the shape of an elongate narrow zone approximately 400 km long completely covered the north slope of the Commander Islands uplift and was confined to the Bering Fault. The rupture zone involved this entire earthquake-generating area as far as a transverse structure west of the Near Islands group (Attu Island). The fault-plane solutions and the inferred displacements in the rupture zones of the main shock and of the largest foreshocks and aftershocks revealed the rupture to be a practically pure right lateral movement. The aftershock process of the July 17 earthquake was occurring at rather a sluggish pace for such a large earthquake. In addition, the process involved two other features to distinguish it from the aftershock processes of most Kuril–Kamchatka earthquakes: (1) a low release of the cumulative scalar seismic moment (M0cum aft), which amounted to between 0.75% and 1.0% of the mainshock seismic moment (M0me), according to several estimates; and (2) a very slow increase in the deficit of seismic moment (M0) release. At the same time, the duration of the quasi-stationary phase in the release of M0cum by aftershocks, which is estimated to have lasted approximately half a year and which occupied much of the entire duration of the aftershock process for this earthquake seems to be unusually long. These features in the aftershock process of the Near-Islands Aleutian earthquake of July 17, 2017 distinguish the process from those common to most large Kuril–Kamchatka earthquakes. Overall, the rupture zone can be regarded as a transform feature between two Benioff zones (The Aleutian and the Kuril–Kamchatka ones) rather than as a subduction event, as is typical of the two latter arcs.

Journal of Volcanology and Seismology. 2019;13(2):112-123
pages 112-123 views

Global Statistics of Aftershocks Following Large Earthquakes: Independence of Times and Magnitudes

Baranov S.V., Shebalin P.N.

Abstract

This paper considers the global statistics of times of largest aftershocks relative to the times of the corresponding main shocks. A large data set was used to show that the time-dependent distribution of largest aftershocks obeys a power law distribution. This is analogous to the Omori law for the sequence of all aftershocks. It is also shown that the times of the second, etc., largest aftershocks obey the same distribution. Thereby, we have confirmed the hypothesis that the times and magnitudes in an aftershock sequence are independent and make a good case for the Reasenberg–Jones representation of the aftershock process as a superposition of the Omori–Utsu law and the Gutenberg–Richter relation. Events that are smaller than the largest in an aftershock sequence show no delay relative to the largest event; this rejects the idea of the aftershock process as a direct failure cascade involving gradual transitions from larger to lesser scales, which imposes certain restrictions on the widely popular stochastic models of aftershock generation as branching processes. The above result is important in practice for prediction of aftershock activity and for assessing the hazard of large aftershocks.

Journal of Volcanology and Seismology. 2019;13(2):124-130
pages 124-130 views