predicting ground motion from earthquakes
TRANSCRIPT
Predicting Ground Motion from Earthquakes
“If we know where a major earthquake is likely to occur, how large will the ground
motion be at a particular site?”
Art McGarr
Summary of Strong Ground Motion from Earthquakes
• Measured using PGA, PGV, pseudo-spectral acceleration or velocity PSA or PSV, and intensity.
• Increases with magnitude.
• Enhanced in direction of rupture propagation (directivity).
• Generally decreases with epicentral distance.
• Low-velocity soil site gives much higher ground motion than rock site. Vs30 is a good predictor of site response.
Call them “Ground-Motion Prediction Equations”
• “Attenuation Equations” is a poor term– They describe the INCREASE of amplitude
with magnitude at a given distance– They describe the CHANGE of amplitude
with distance for a given magnitude (usually, but not necessarily, a DECREASE of amplitude with increasing distance).
Ground Motion Prediction Equations
• Empirical regressions of recorded data• Estimate ground shaking parameter (peak ground
acceleration, peak velocity, spectral acceleration or velocity response) as a function of
(1) magnitude
(2) distance
(3) site• May consider fault type (strike-slip, normal,
reverse)
Developing EquationsDeveloping Equations• When have data (rare for most of the world):
– Regression analysis of observed data
• When adequate data are lacking: – Regression analysis of simulated data (making use of motions
from smaller events if available to constrain distance dependence of motions).
– Hybrid methods, capturing complex source effects from observed data and modifying for regional differences.
Observed data adequate for regression exceptclose to large ‘quakes
Observed data not adequate for regression, use simulated data
1 10 100 1000
5
6
7
8
Mom
ent
Mag
nitu
de
Used by BJF93 for pga
Western North America
1 10 100 1000
5
6
7
8
Distance (km)
Mom
ent
Mag
nitu
de
AccelerographsSeismographic Stations
Eastern North America
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What to use for the Predictor Variables?
• Moment magnitude
• Some distance measure that helps account for the extended fault rupture surface (remember that the functional form is motivated by a point source, yet the equations are used for non-point sources)
• Site terms
• Maybe style of faulting
How does the motion depend on magnitude?
• Source scaling theory predicts a general increase with magnitude for a fixed distance, with more sensitivity to magnitude for long periods and possible nonlinear dependence on magnitude
• Of the many magnitude scales, which is the most useful for ground motion prediction?
Moment Magnitude
• Best single measure of overall size of an earthquake
• Can be determined from ground deformation or seismic waves
• Can be estimated from paleoseismological studies
• Can be related to slip rates on faults
10-1 1 101 1020.01
0.1
1.0
10
100
Frequency (Hz)
Fou
rier
acce
lera
tion
spec
trum
(cm
/sec
)
M 5 to 8 in steps of 0.5
R = 20 km
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4 5 6 7 80.1
1
10
100
1000
M
PS
A(c
m/s
ec2)
R = 20 km
T = 0.20 sec
T = 1.0 sec T = 2.0 sec
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How does the motion depend on distance?
• Generally, it will decrease (attenuate) with distance
• But wave propagation in a layered earth predicts more complicated behavior (e.g., increase at some distances due to critical angle reflections (“Moho-bounce”)
• Equations assume average over various crustal structures
• Many different measures of distance
Path effects• Wave types
– Body (P, S)– Surface (Love, Rayleigh)
• Amplitude changes due to wave propagation– Geometrical spreading (1/r in uniform media, more rapid decay for
velocity increasing with depth)– Critical angle reflections– Waveguide effects
• Amplitude changes due to intrinsic (conversion to heat) and scattering attenuation [exp(-kr)]
CharacteristicsCharacteristics of Data
• Change of amplitude with distance for fixed magnitude
• Change of amplitude with magnitude after removing distance dependence
• Site dependence
• Scatter
"It is an easy matter to select two stations within 1,000 feet of each other where the average range of horizontal motion at the one station shall be five times, and even ten times, greater than it is at the other”
John Milne, (1898, Seismology)
Spatial VariabilitySpatial Variability
What functional form to use?
• Motivated by waves propagating from a point source
• Add more terms to capture effects not included in simple functional form
People have known for a long time thatPeople have known for a long time thatmotions on soil are greater than on rockmotions on soil are greater than on rock
• e.g., Daniel Drake (1815) on the 1811-1812 New Madrid sequence:
•
– "The convulsion was greater along the Mississippi, as well as along the Ohio, than in the uplands. The strata in both valleys are loose. The more tenacious layers of clay and loam spread over the adjoining hills … suffered but little derangement."
Site Classifications for Use WithSite Classifications for Use WithGround-Motion Prediction EquationsGround-Motion Prediction Equations
• Rock = less than 5m soil over “granite”, “limestone”, etc.• Soil= everything else
2. NEHRP Site Classes
3. Continuous Variable (V30)
1. Rock/Soil
620 m/s = typical rock
310 m/s = typical soil
1 10 100 1000
5
6
7
8
Distance (km)
Mom
ent
Mag
nitu
de
valid region for using BJF equations
Western North America (used by BJF93, 97 for pga)
1 10 100 1000
5
6
7
8
Distance (km)
World (NGA, with BA exclusions)
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Includes02 Denali Fault (M 7.9)99 Chi-Chi (M 7.6)99 Kocaeli (M 7.5)78 Tabas (M 7.4)86 Taiwan (M 7.3)99 Duzce (M 7.1)
10-1 1 101 102
10-1
1
Distance (km)P
ea
kA
cce
lera
tion
(g)
NEHRP Class DM 5.5
M 6.5
M 7.5
1 101 102
1
101
102
Distance (km)
5%
da
mp
ed
PS
V(c
m/s
)
NEHRP Class DM 5.5
M 6.5
M 7.5
T = 0.3 sec
1 101 102
101
102
Distance (km)
5%
da
mp
ed
PS
V(c
m/s
)
NEHRP Class DM 5.5
M 6.5
M 7.5
T = 1.0 sec
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A&S, sS, Vs=600
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PG
A (
g)
Rupture Distance (km)
5
5.5
6
6.5
7
7.5
M8, AR=2
M8, AR=4
M8, AR=8
M8, AR>15
0 20 40 60 80 1000
0.2
0.4
0.6
0.8
1
1.2
djb
peak
horiz
onta
lac
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ratio
n(g
)
BJF93, random, NEHRP D, M=7.0shaded: median/10 , median*10
0.1 1 10 100
0.1
0.2
0.3
1
djb
BJF93, random, NEHRP D, M=7.0shaded: median/10 , median*10
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Ground-Motion Prediction EquationsGround-Motion Prediction Equations
Gives mean and standard deviation of response-spectrum ordinate (at a particular frequency) as a function of magnitude distance, site conditions, and perhaps other variables.
10-1 1 101 102
0.01
0.1
1.0
Shortest Horiz. Dist. to Map View of Rupture Surface (km)
La
rge
rH
ori
zon
talP
ea
kA
cce
l(g
)
1992 Landers, M = 7.31994 NR, M=6.7 (reduced by RS-->SS factor)Boore et al., Strike Slip, M = 7.3, NEHRP Class D_+
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0.1 0.2 1 21
101
102
Period (sec)
Pse
udo
Rel
ativ
eV
eloc
ity(c
m/s
)
Mechanism: strike slipMechanism: reverse slip
SoilM = 7.5
D = 0 km
D = 10 km
D = 20 km
D = 40 km
D = 80 km
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0.1 1 10 100
10
100
1000
10000
Rjb (set values less than 0.1 to 0.1 km)
PS
A(c
m/s
ec2)
Chi-Chi (M 7.6)Loma Prieta (M 6.9)Northridge (M 6.7)
T = 0.1 sec
0.1 1 10 100
Rjb (set values less than 0.1 to 0.1 km)
Chi-Chi (M 7.6)Loma Prieta (M 6.9)Northridge (M 6.7)
T = 2 sec
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Chi-Chi data are low at short periods(note also scatter, distance dependence)
Illustrating distance and magnitude dependence
Mexico City ・ 350 km from earthquake epicenter ・ 9000 deaths ・ collapse of 371 high rise structures, especially 10-14 story
buildings
Mexico City Acceleration Response Spectrum
Recorded data
Expected ground motions
Resonance Period of10 to 14 story buildings
PGA generally a poor measure of ground-motion intensity. All of these time series have the same PGA:
0 50 100 150-0.2
-0.1
0
0.1
0.2
Acc
eler
atio
n(g
) Peru, 5 Jan 1974, Transverse Comp., Zarate
M = 6.6, rhyp = 118 km
0 50 100 150-0.2
-0.1
0
0.1
0.2
Acc
eler
atio
n(g
) Montenegro, 15 April 1979, NS Component, Ulcinj
M = 6.9, rhyp = 29 km
0 50 100 150-0.2
-0.1
0
0.1
0.2A
ccel
erat
ion
(g) Mexico, 19 Sept. 1985, EW Component, SCT1
M = 8.0, rhyp = 399 km
0 50 100 150-0.2
-0.1
0
0.1
0.2
Time (sec)
Acc
eler
atio
n(g
) Romania, 4 March 1977 EW Component, INCERC-1M = 7.5, rhyp = 183 km
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Period (sec)
Peru (M=6.6,rhyp=118km)
Montenegro (M=6.9,rhyp=29km)
Mexico (M=8.0,rhyp=399km)
Romania (M=7.5,rhyp=183km)
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Period (sec)
5%-D
ampe
d,P
seud
o-A
bsol
ute
Acc
eler
atio
n(g
)
Peru (M=6.6,rhyp=118km)
Montenegro (M=6.9,rhyp=29km)
Mexico (M=8.0,rhyp=399km)
Romania (M=7.5,rhyp=183km)
But the response spectra (and consequences for structures) are quite different (lin-lin and log-log plots to emphasize different periods of motion):
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Period (sec)
5%-D
ampe
d,P
seud
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Acc
eler
atio
n(c
m/s
ec2)
M=7.5, NEHRP classes B, C, DM=5.5, NEHRP classes B, C, D
Boore, Joyner, and Fumal (1997); rjb = 10 km
BC
D
0.1 0.2 0.3 1 2
10
20
100
200
1000
2000
Period (sec)
M=7.5, NEHRP classes B, C, DM=5.5, NEHRP classes B, C, D
Perception of results depends on type of plot (linear, log)
Ground Motion Prediction• Intended to predict PGA, PGV, or spectral response at
periods of engineering interest• logY=a1+a2(M-Mr1)+a3(M-Mr2)+a4R+a5LogR+site+a6F• Coefficients ai are determined by regression fits to ground
motion data sets.• Ground motion generally increases with M and decreases
with R• Site term mostly depends on near-surface shear-wave
speed, usually expressed as Vs30• Site effects sometimes dominate • Response spectra much more useful than PGA for
predicting structural damage