講師 中谷正生(東京大学地震研究所)
題目 直球勝負—地震予知。

最も単純な地震サイクルのシナリオを基本に、「こういうことがextraにあってくれたら短期予知ができるだろう」というシナリオと、そのシナリオにあう観測事実を4つほどお話しします。準備過程の大きさということにこだわりながら考えます。

1. Introduction -long-term prediction

  Abundant evidence shows that earthquakes are unstable slip repeating on existing weak planes in the earth’s topmost part, which is too cold (<300C) to deform stably. An earthquake occurs when the stress on the weak plane, which increases slowly due to plate motion, reaches the frictional strength. The earthquake (i.e. slip) relaxes the stress over the slipped area, hence we know that there will be some time before the next earthquake involving the whole slipped area. Although numerous small earthquakes can occur anytime on the weak plane using a stress accumulation of small spatial scale, their summed effect on the average stress over the area of the large earthquake is negligible. In addition, we know where the major weak planes are located geographically, (plate boundaries and mature faults within a plate). These understandings leads to the following long-term earthquake prediction. Large earthquakes occur only where large earthquakes occurred before. After a large earthquake happens in one place, the next large one would not occur for, say, at least 50% of the average repetition time at that locality. 

 

2. Hopes for short-term prediction.

  The average repetition interval is of order 100 years for plate boundaries and 1000-10000 years for intra-plate faults. This is the time for accumulating ~10 MPa of stress (difference between static friction and dynamic friction). If we want to predict a plate-boundary earthquake with, say, 1-year accuracy, we need to know the strength and the current stress level with an accuracy of 0.1MPa, which way we do not know. So, we hope that Mother Nature has something more in favor of us, which we call ‘earthquake preparation processes’. Hopes are classified as: A) Material of the weak plane may come into a funny state (or even breaks and slips partially) when the stress comes very close to the strength. B) Strength may be decreased (over a large spatial scale) by an external factor pretty quickly. C) Stress accumulation mechanism may behave in a more complex way than steadfast loading at a constant rate. Maybe, it accelerates at one point of time, quickly raising the stress on the faults to its strength.

  In this talk, I would like to discuss how possible preparation processes cause ‘precursory anomalies of large earthquakes’. Statistical significance of each type of anomaly is in grey-zone. However, each earthquake can take different paths to the final failure, so taking statistics for ‘earthquakes in general’ is not the most productive thing to do. My approach is rather to look for physically plausible preparation processes, betting on that many earthquakes do not occur all the sudden at the critical stress level. 

 

3. Concrete models of earthquake preparation processes.

In the talk, observations attributable to the following scenarios will be presented.

A) Failure of inhomogeneous materials, including frictional slip, is invariably preceded by changes of the state of the material, which is often an inevitable part of the physical process toward the final failure. An explosive increase of micro cracks is a typical precursory change, which can induce many observable anomalies, amplified by resultant groundwater flow.

A’) The above precursory processes start when the local stress approaches the local strength. However, it is not realistic to expect this occurs simultaneously all over the extent of the eventual rupture plane of the coming large earthquake (say, 20 km x 100 km). It would be more realistic to assume that precursory failure occurs in a limited part (called earthquake nucleus) of the future rupture plane and the rest of the rupture occurs by a sudden increase caused by dynamic rupture expanding from the nucleus. Rupture mechanics guarantees that nuclei grow spontaneously (i.e. without further increase of the applied stress, thus within a time period much shorter than the repetition interval) but quasi-stationarily to a certain size. The critical question for prediction is whether the size of nucleus and that of the final rupture are correlated.

B) The above scenarios are beautiful in that the preparation processes are inevitable part of the physical process to final failure. However, Mother Nature may be less interesting but more favorable for us. For example, if high-pressure fluid is injected into the pores on the weak plane, its strength drops. A 1 MPa increase of fluid pressure causes ~0.7MPa drop of strength, easily affecting the earthquake occurrence. An advantage of this scenario is that strength can be decreased quasi-simultaneously all over the extent of the future rupture plane. (More like, the dimension of the weakened part decides the size of the coming earthquake.) Note that many reported precursory anomalies require that preparation process occurring over a wide area comparable to the final rupture.

C) Stress accumulation on the weak plane seems to be caused by a stable slip of the deeper extension of the plane. If it accelerates at some time, this can be the time for earthquake. Rapid loading by a nearby occurrence of large earthquake can have the same effect.

 

Conclusion

In my opinion, short-term prediction is possible only if earthquake is preceded by special preparation processes beyond just an increase of stress at a constant rate. It is physically plausible, though otherwise is also plausible. Useful preparation processes are those that scale with the size of final failure.

 

References

Scholz, 2002, The mechanics of Earthquakes and Faults (2nd ed.), Cambridge Univ. Press.