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Can an electro-kinetic mechanism explain artificial earthquakes?

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Abstract

Researchers of the Joint Institute for High Temperatures of the Russian Academy of Sciences have carried out a large number of current injection experiments using a 4.2 km long dipole at the Bishkek Research Station in the Chu valley area of the Kyrgyz mountains (northern Tien Shan). The current is generated using Pulsed Magneto-Hydrodynamic (MHD) generators that can produce 2800 amperes at 1350 volts for up to 12.1 seconds. They have found that the number of earthquakes in the region within 150 km of the injection site increased by over 10 standard deviations of the background seismicity. The probability of this occurring by chance is only one in every thousand million million (10^15) measurements. It is certain, therefore, that we can generate earthquakes by current injection. However, no satisfactory physical mechanism for it currently exists. Paul Glover has suggested that an electro-kinetic mechanism may be the missing causal link. In his theory the injected current creates a three-dimensional electric field in the subsurface. The electro-kinetic mechanism uses the electric field to move the pore fluid at depth. If the pore fluid flows into a fault zone it may accumulate and transiently raise the pore fluid pressure within the fault zone. It is known that increases of pore fluid pressure within fault zones more than a critical pressure of 0.05 MPa are sufficient to trigger an earthquake if the fault has sufficient accumulated strain. Earthquakes are therefore possible while the pore fluid pressure is over the critical pressure. While the electro-kinetic drive has been well studied around the world, it is uncertain if the mechanism can provide fluid pressures sufficient to trigger earthquakes up to 150 km from the injection point. In this work we present two dimensional numerical modelling of the proposed coupled mechanism using a finite element approach and using the software package Comsol Multiphysics. The initial results are promising and indicate that (i) transient pressures greater than the critical pressure can be easily generated by the mechanism, (ii) the transient pressures in the model farther than 200 m from the electrodes can take values of up to 2 MPa (40 times the critical value), (iii) the transient pressures remain above the critical value up to 160 km from the dipole, which is consistent with the range of the field experiments. However, the modelling has only been able to generate the transient pressures quasi-instantaneously. There is a clear delay in the field experiment data of two days between current injection and earthquake occurrence. We cannot currently account for this in our modelling, although research is continuing.
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How to make artificial earthquakes
Guillaume Cyr and Paul Glover
Deep within the mountainous regions of
KyrgyzstanÎ ground-breaking experiments
are being carried out. The Russians are making
earthquakes. In a research project more akin to
that visited by Tintin in Syldavia than the real
world, scientists are using large pulsed MHD
generators to inject thousands of amperes of
current into the ground. The current causes
earthquakes to occur up to 150 km away. No
one knows the real mechanism that causes the
artificial earthquakes, but they are linked
inextricably to the injection of the electrical
current. Paul Glover, the professor of
petrophysics at Université Laval (Québec), has
suggested a mechanism, and it is the job of his
student Guillaume Cyr to model the
mechanism in order to see if it is capable of
producing pore fluid pressures sufficient to
trigger an earthquake. Pulsed magneto-hydrodynamic (MHD)
generators tap into the extremely high
magnetic fields generated by a moving
plasma to produce extremely high electrical
currents. The generators used to trigger
earthquakes can produce 2800 amperes at
1350 volts for up to 12.1 seconds, in other
words energies as high as 23 megajoules.
In the image Í, the three long tubes
generate the plasma and fire it through a
non-conducting cavity that is surrounded
by electrical coils housed in the large
circular enclosures. Effectively, this is
three pulsed MHD generators in parallel.
When the plasma moves at high speed
through the non-conducting cavity it
generates an extremely high magnetic field
perpendicular to the movement. The
magnetic field then generates a large
electrical current in the coils.
The Kyrgyz mountains south of Bishkek
in Kyrgyzstan.
A 1500 MA pulsed MHD generator at the
Kyrgyzstan site.
2
Viktor Novikov and his colleagues of the Institute for High Energy Densities of the Russian Academy of
Sciences have carried out a large number of current injection experiments using an approximately 5 km long
dipole at the Bishkek Research Station of the Russian Academy of Sciences in the Chu valley area of the Kyrgyz
mountains (northern Tien Shan). They found that the number of earthquakes in the region within 150 km of the
injection site increased by over 10 standard deviations (σ) of the background seismicityÐ. To put this in context,
statistics tells us that the number of earthquakes would exceed 3σ only once in every 400 samples (99.75%) if
the earthquakes are not related to the current injections. The probability of the signal being more than 10
standard deviations from the mean by chance is so minuscule, it would be expected to occur only once in every
1015 measurements (i.e., for only a few microseconds since the beginning of the universe, about 10 billion
years!).
The increase in the
earthquakes starts a few days
after each injection and
continues for about 5 more
daysÎ. The earthquakes
generally occur along
previously known fault zones
showing that the current
injection is triggering
slippage where there is
already accumulated strain
energy. Where earthquakes
are not distributed along
known fault zones, new fault
zones may be mapped. The
artificial earthquakes had
magnitudes up to mb=5
(Gutenberg-Richter).
What are the applications of artificial earthquakes? Each time an earthquake occurs some of the accumulated
strain energy is released. Hence if small controlled earthquakes can be generated in an area the strain
accumulation may be allayed, making the occurrence of a large destructive earthquake less likely. This is
analogous to an inoculation : the artificial generation of an attenuated earthquake or earthquakes protects against
a large quake just as the presence of a weak form of a disease allows the body to develop antibodies to fight the
attack of a dangerous disease. The difference is that here we are inoculating the earth! However, the logarithmic
nature of the scales for earthquake measurement implies that it would need over 172,000 artificial earthquakes of
mb=5 to protect against one destructive earthquake (mb=7), and that is clearly impractical. Maybe then the
technique could be used to trigger a large earthquake that is overdue, giving at least the advantage of knowing
when the earthquake will occur. Unfortunately this application is probably politically impossible. The real
advantage of the technique may be found at smaller scale, in the mapping of fault zones, and the triggering of
rock and mud slides that would otherwise remain a danger, and of course, in the understanding of the earthquake
process in general.
The smoking gun! Earthquakes occurring 2 to 7 days
after current injection.
3
At least, it would give us more of an insight into the earthquake process if we knew the mechanism that caused
the artificial earthquakes.
Professor Paul Glover of Université Laval in
Québec has suggested that an electro-kinetic
mechanism may be the missing causal link. In his
theory the injected current creates a three-
dimensional electric field in the subsurface. The
electro-kinetic mechanism uses the electric field
to move the pore fluid at depth. If the pore fluid
flows into a fault zone it may accumulate and
raise the pore fluid pressure within the fault zone.
It is known that increases of pore fluid pressure
within fault zones more than a critical pressure of
0.05 MPa are sufficient to trigger an earthquake if
the fault has sufficient accumulated strain. In the
graph of pore fluid pressure against time Í the
pore fluid pressure increases very quickly at a rate
τ+ because it is being driven by the electro-
kinetic drive and then decreases more slowly at a
rate τ- because the pressure dissipates passively.
Earthquakes are possible while the pore fluid
pressure is over a certain critical level.
While the electro-kinetic drive has
been confirmed in the Petrophysics
Laboratory of Université Laval and a
few other laboratories around the
world, it is uncertain if the mechanism
can provide fluid pressures sufficient
to trigger earthquakes up to 150 km
from the injection point. Guillaume
Cyr, a student at Université Laval has
been modelling the process
numerically. His two dimensional
models of the subsurface are created in
a software package Comsol
MultiphysicsÎ.
The theoretical variation of pore fluid pressure
caused by current injection
Model showing pore fluid pressures over 2 MPa (red) are generated to
the right of the first layer (500 m thick). Areas in white have pressures
greater than 2 MPa and surround each electrode of the injection dipole.
4
After defining the structure of the model he is able to solve the differential equations that describe fluid flow,
electrical flow, electro-kinetic coupling, mass balance and thermal effects in parallel on a finite element grid.
The modelling is still a work in progress. However early steady state solutions in a horizontally layered earth
indicate that pore fluid pressures over 3 MPa can be achieved easily with a current injection of 1500 amperes,
and that the pressure remains higher than the critical value of 0.05 MPa up to 150 km from the injection point.
We now know that sufficient fluid pressures can be generated using a steady state differential equation solution.
So far the modelling does not contain any information about how the fluid pressures vary with time. This is
actually extremely important because it may be that activating the pulsed MHD generator for only 10 seconds is
insufficient to obtain the steady state values. Solving these complex differential equations as a function of space
and time is an extremely complex task and represents the next step for M. Cyr. It is hoped that we will have
some initial solutions by December 2009.
Until then, we can confirm that plugging your electricity supply into your garden is not only dangerous, it will
not cause an earthquake – please do not try it at home.
... In a more academic sphere, the applications of the concepts described in this chapter are used for understanding the continental crust (e.g., Glover, 1996;Glover and Adám, 2008;Vine, 1992, 1995;Glover et al., 2000b;Yang, 2011) and oceanic crust (e.g., Baba, 2005;Gung et al., 2003;Key et al., 2013;Yoshino et al., 2008); the triggering of natural and synthetic earthquakes (e.g., Chelidze et al., 2003;Cyr et al., 2010); volcanic activity monitoring (e.g., ; the properties of lunar (e.g., Li et al., 2005), Martian (e.g., Carter et al., 2009), and asteroidal (e.g., Wittmann et al., 1999) materials; and soil science (e.g., Robinson et al., 2003;Peplinski et al., 1995). Counterintuitively, perhaps, some of the electrical conductivity models have been applied in fields as varied as catalysis research (e.g., Zhang and Catchmark, 2011) and food engineering (e.g., Jha et al., 2011;Jindal et al., 2013). ...
Chapter
The electrical properties of rocks and minerals vary over 20 orders of magnitude, yet can be measured in the laboratory to an accuracy of one part per billion. This remarkable combination makes electrical techniques extremely sensitive to the composition and texture of geomaterials. Furthermore, electric currents can be generated in rocks remotely, and the flow of currents can also be measured remotely. This is a key advantage that opens up the possibility that the electrical properties of rocks deep in the Earth may be measured. For example, remote monitoring is implemented at a small scale in downhole induction tools and deeper in the case of the magnetotelluric method. The recent rapid development of electrokinetic research produces the possibility that remote electrical measurements will be able to infer fluid flow deep in the Earth, such as encroachment of water towards a productive oil well or monitoring the emplacement of waste CO2 in carbon capture and storage reservoirs. Perhaps, the most impressive example of the importance of the electrical properties of rocks is the implementation of Archie's law. This law, which was published in 1942, has been used to measure and monitor all of the Earth's oil and gas reserves since its invention. Thanks to Archie's law, over 1.5 trillion barrels of oil reserves and 7.5 trillion standard cubic feet of gas have been quantified and produced, running the global economy for the last 70 years. In this chapter, the basic electrical theory of geomaterials is set out together with sufficient experimental and modeling results to show what controls their electrical properties. For the purposes of this chapter, we have taken electrical properties to cover steady-state and frequency-dependent electrical transport and polarization as well as those electrokinetic processes that link electrical flow to hydraulic flow. After a brief introduction, the basic theory of steady-state electrical flow in rocks is considered, including Archie's laws and other mixing models, but restricting ourselves to near-surface temperatures and pressures and hence to conduction occurring through the pore fluids that occupy the pores of the rock rather than by electronic conduction through the rock matrix. However, surface conduction is often significant in the near-surface regime, especially for shaley rocks and some soils. Hence, we consider the source, measurement, and modeling of surface conduction in the third section of the chapter. Theoretical advances that have been made since 1994 in the understanding of steady-state electrical transport are also fully covered. A significant section considers electrical polarization, electric permittivity, and the frequency-dependent properties of rocks. Finally, the steady-state and frequency-dependent electrokinetic properties of geomaterials are considered including factors affecting the streaming potential of near-surface rocks.
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