This paper describes the use of the idea of natural time to propose a new method for characterizing the seismic risk to the world's major cities at risk of earthquakes. Rather than focus on forecasting, which is the computation of probabilities of future events, we define the term seismic nowcasting, which is the computation of the current state of seismic hazard in a defined geographic region.
Deep Dive into Natural Time, Nowcasting and the Physics of Earthquakes: Estimation of Seismic Risk to Global Megacities.
This paper describes the use of the idea of natural time to propose a new method for characterizing the seismic risk to the world’s major cities at risk of earthquakes. Rather than focus on forecasting, which is the computation of probabilities of future events, we define the term seismic nowcasting, which is the computation of the current state of seismic hazard in a defined geographic region.
Natural Time, Nowcasting and the Physics of Earthquakes:
Estimation of Seismic Risk to Global Megacities
John B Rundle1,2,3,4, Molly Luginbuhl1, Alexis Giguere1, Donald L. Turcotte3
1 Department of Physics
University of California, Davis, CA
2 Santa Fe Institute
Santa Fe, NM
3 Department of Earth and Planetary Science
University of California, Davis, CA
4 Open Hazards Group
Davis, CA
Abstract
Natural Time (โNTโ) refers to the concept of using small earthquake counts, for
example of M>3 events, to mark the intervals between large earthquakes, for example M>6
events. The term was first used by (Varotsos et al., 2005) and later by (Holliday et al.,
2006) in their studies of earthquakes. As we discuss in this paper, it is particularly useful
in describing complex stochastic nonlinear systems characterized by fat-tail statistics
rather than Gaussian normal statistics. In this paper we discuss ideas and applications
arising from the use of NT to understand earthquake dynamics. The usual end-user
applications of fault-based studies are often applied to risk of a particular geographic
location, so it seems best to start the analysis with that geographic region. Rather than
focus on an individual earthquake faults, we have found it more productive to focus on a
defined local geographic region surrounding a particular location. This local region is
considered to be embedded in a larger regional setting from which we accumulate the
relevant statistics. From this different philosophical point of view, we first discuss methods
to use NT, counts of small earthquakes, to evaluate the current state of a regional collection
of faults. We then use these concepts to first discuss the nucleation physics of large
earthquakes. We introduce the idea of nowcasting, a term originating from economics and
finance. The goal of nowcasting is to determine the current state of the fault system, or put
another way, the current state of progress through the earthquake cycle. This is in contrast
to forecasting, which is the calculation of probabilities of future large earthquakes. Finally,
we apply the nowcasting idea to the practical development of methods to estimate the
current state of risk for dozens of the worldโs seismically exposed megacities, defined as
cities having populations of over 1 million persons. We compute a ranking of these cities
based on their current nowcast value, and discuss the advantages and limitations of this
approach. We note explicitly that the nowcast method is not a model, in that there are no
free parameters to be fit to data. Rather, the method is simply a presentation of statistical
data, which the user can interpret.
2
Introduction
Natural time is a term first used by (Varotsos et al., 2005, 2011)and subsequently by
(Holliday et al., 2006). It builds on the idea that driven threshold systems such as
earthquake fault systems often display a power-law distribution of event sizes or
magnitudes. While these bursts of activity are observed at all scales, the largest events are
usually of most interest. For earthquakes, these largest events are the magnitude 6+
events that cause the most damage and injuries. Interspersed between these largest events
are many smaller events of varying sizes and magnitudes.
Taken together, these small and large events are distributed in a scale-invariant
power-law statistical distribution of magnitude. The Gutenberg-Richter magnitude-
frequency law (Gutenberg and Richter, 1942; Scholz, 1990) is a simple model of this
distribution which is found to be applicable over large spatial domains and over long time
intervals. The GR model has two parameters, a and b, which must be fit to the observed
data:
๐ฟ๐๐$% ๐= ๐โ๐๐
(1)
Here N is the number or frequency of earthquakes having magnitudes larger than M.
Typically, b ~ 1.
Over smaller spatial domains and shorter time intervals, the actual statistics of the
observed number or frequency of earthquakes can depart considerably from the simple
model (1). A good example is shown in Figure 1a,b . On the left in Figure 1a we see
Figure 1. a) Map of earthquakes having magnitude ๐โฅ6.5 near San Diego since 1970. Circle centered on San
Diego has radius ๐
= 400 km. b) GR number-magnitude statistics. The upper blue square symbols are all
earthquakes ๐โฅ3 for the region as a whole since 1970. The lower green circles are all earthquakes 3 โค๐< 6.5
since the last ๐โฅ6.5 earthquake, which was the M7.2 El Major-Cucapah earthquake on 4/4/2010.
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a map of a large region surrounding the city of city of San Diego, USA, between latitudes
24o N and 43o N Latitude, and between 128o W and 110o W Longitude. In the center of the
map is a circle of radius 400 km surrounding the city of San Diego. We then construct the
Gutenberg-Richter (GR) number-magnitude statistics in Figure 1b. The statistics
represented by th
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