Wednesday, July 25, 2012

Attenuation in Different Directions

Attenuation in Different Directions

Epicentral distances have been measured along different directions and it is observed that the distance for the same isoseist is often different in different directions. Fig.2 shows the attenuation of three different earthquakes in different directions. From Fig.2, for 1885 Bengal earthquake it is observed that the intensity in the direction west shows much smaller attenuation. For 1930 Dhubri earthquake, South and S450W directions represent greater attenuation. For 1918 Srimangal earthquake, S450W and east directions show greater attenuation. So the directions affecting Bangladesh (see Fig.3) in general show greater attenuation than some other directions.
                           Figure 2: Attenuation of different earthquakes in different directions.

Development of Attenuation Law
For the establishment of Intensity-attenuation relationship, seven earthquakes have been selected as mentioned earlier. Because of the directional difference in intensity attenuation (Fig.2), directions have been chosen which are affecting Bangladesh mainly. Six out of seven earthquakes have been considered for which average epicentral distances along these directions are determined for each isoseismal. Chosen directions for these earthquakes are shown in Fig.3.



 

 Figure 3   Directions considered for determining average epicentral distances of isoseismals for six earthquakes (except 1897 Assam earthquake)

Table 1 presents the epicentral distance data considered for different isoseismals of different intensities (MMI scale). Also shown are relevant earthquake data (date, epicenter location and depth, and magnitude). The epicentral distance data for 1897 Assam earthquake is taken from the average radius data given by Ambraseys and Bilham (2003), since the isoseismals are of very irregular shape (Fig.1a). The directional average distance of the isoseismals from the epicenter is estimated for the other six earthquakes. The Table 1 data is used for developing attenuation law.

Table 1: Epicenter location and mean directional epicentral distance data of selected earthquakes:


No.

Date
Earthquake Epicenter

M

Depth
(km)
Mean Directional* Epicentral Distance (km) of Isoseismals for Different Intensities (MMI)
Lat.
Long.
III
IV
V
VI
VII
VIII
IX
X
1
14/07/1885
24.70N
89.55E
7.0
72
403
-
238
-
88
-
-
-
2
12/06/1897
25.84N
90.38E
8.1
60
-
576
381
250
172
75
-
-
3
08/07/1918
24.25N
91.80E
7.6
14
-
-
119
74
-
39
-
18
4
02/07/1930
25.95N
90.04E
7.1
60
-
-
233
139
-
58
16
-
5
08/07/1945
25.8N
92.3E
6.7
-
-
260
185
105
-
-
-
-
6
15/04/1964
21.7N
88E
5.5
36
162
90
50
-
-
-
-
-
7
22/07/1999
21.61N
91.96E
5.1
10
-
-
17
8
4
-
-
-
* Epicentral distance of isoseismals for 1897 earthquake is taken not on directional basis due to irregular shape of isoseismal, but from tabulated average values given by Ambraseys and Bilham (2003)


Attenuation Model 1 (Using Epicentral Distance)

The attenuation law for intensity is assumed to be of the standard form of Eq.(1):
I=a+b*(M)+c*(R)+d*log(R)+σP                                                                  (1)
where a, b, c, d are coefficients, M is the earthquake magnitude (Richter scale or equivalent), R is the mean epicentral distance, I is the intensity (MMI), σ is the standard deviation of I. The constant P takes a value zero for 50 percent probability that the parameter will exceed the real value and one for 84 percent probability.

Then coefficients a,b,c,d are determined by fitting Eq.(1) to the earthquake data set M and selected (I, R) pairs listed in the Table 1. The regression analysis is performed using a program developed in Matlab 7.0, details of which is given by Islam (2009). The data set consists of 25 (I, R) pairs for seven earthquake events. The following equation is obtained for Attenuation Model 1 using epicentral distance:
I=1.0249+1.4863*(M)-0.0042*(R)-2.4518*log(R)+1.001P                          (2)
with standard deviation σ = 1.001

Attenuation Model 2 (Using Hypocentral Distance)

Eq.1 can also be used with hypocentral distance replacing epicentral distance. Considering focal depth, the hypocentral distances are calculated for use in the regression analysis. The 1945 Mikirhills earthquake was excluded from the data set due to unavailability of focal depth. The following equation is obtained for Attenuation Model 2 using hypocentral distance Rhyp:
I=1.9626+1.4906*(M)-0.0042*( Rhyp)-2.826*log(Rhyp) + 1.0812P               (3)
 with standard deviation σ = 1.0812

Validation of Attenuation Models with Field Data

The attenuation equations are validated by comparing predicted intensities with the earthquake data of Table 1. Fig.4 presents comparison for all earthquakes except Moheshkhali earthquake. The comparison yields reasonably good agreement for all earthquakes except for 1918 Srimangal earthquake. The difference is appreciable at larger distances, and the models overestimate the intensity. The Srimangal earthquake with shallow focal depth has relatively faster attenuation compared to other earthquakes which could not be represented well by the models.
Figure 4: Comparison of developed attenuation models with field intensity values
Figure 4: Comparison of developed attenuation models with field intensity values (continued)

Model 1 and Model 2 yield quite close results. Only at shorter distances for 1930 Dhubri earthquake, Model 2 underpredicts intensity significantly.