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Earthquake Location
Manual Method
• To get an approximate location of an earthquake
is possible with the help of seismic waves.
• If the seismic network is dense and the
earthquake is originated inside the network, the
station with the earliest arrival can be
approximated as the epicentre.
• This is called earliest station method, and it gives
an estimate with a probable error of the same
order as the station spacing.
• Another approach is to contour the P-wave
arrival times.
• This is an extension of the earliest station
method.
• This may give fairly good estimate of the
epicentre location if the network is dense
enough.
• If the network is not dense and it consists of a
few stations only, then the method is not
effective.
• A good approximation of the epicentre can be
made by arc method or circle method with
three or more S-P times.
• Three parameters are calculated which include
epicentral distance X, hypocentral distance D
and depth of focus (H) of an earthquake.
• If Tp is arrival time of the P wave and Ts is that
of the S wave, then we can write:
• Where Vp and Vs are the velocity of the P-wave
and S-wave respectively.
• Equating both equations,
• Assuming Vp/Vs = 1.73, the hypocentre
distance can be estimated as
• where D is in kilometres, and S-P is in second.
• After determining D at three or more stations,
circles with radius D can be drawn with each
circle centred at the respective station.
• The epicentre lies in the region where the
circles overlap.
• This method was commonly used as a quick
means of locating earthquakes.
• The focal depth (H) can be obtained as:
• Adding more observations will give additional
intersections that theoretically should pass
through the epicentre.
• In practice, error is always present, both in
data and in assumptions, that the ray-paths
are straight and the Earth is homogeneous, so
scatter in the intersection usually occurs.
Origin Time of an Earthquake
• The origin time of an earthquake can be
determined with a very simple graphical
technique, called Wadati plot (Wadati, 1933).
• The time separation of the P and S phase (Ts – Tp)
is plotted against the arrival time of the Pwave.
• Since Ts – Tp = 0 at the hypocentre, a straight line
fit on the Wadati diagram gives the origin time at
the intercept with the P-arrival-time axis
Earthquake%20Location18%2006%202020.pdf

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Earthquake%20Location18%2006%202020.pdf

  • 2. Manual Method • To get an approximate location of an earthquake is possible with the help of seismic waves. • If the seismic network is dense and the earthquake is originated inside the network, the station with the earliest arrival can be approximated as the epicentre. • This is called earliest station method, and it gives an estimate with a probable error of the same order as the station spacing.
  • 3. • Another approach is to contour the P-wave arrival times. • This is an extension of the earliest station method. • This may give fairly good estimate of the epicentre location if the network is dense enough. • If the network is not dense and it consists of a few stations only, then the method is not effective.
  • 4. • A good approximation of the epicentre can be made by arc method or circle method with three or more S-P times. • Three parameters are calculated which include epicentral distance X, hypocentral distance D and depth of focus (H) of an earthquake. • If Tp is arrival time of the P wave and Ts is that of the S wave, then we can write:
  • 5. • Where Vp and Vs are the velocity of the P-wave and S-wave respectively. • Equating both equations,
  • 6. • Assuming Vp/Vs = 1.73, the hypocentre distance can be estimated as • where D is in kilometres, and S-P is in second.
  • 7.
  • 8.
  • 9. • After determining D at three or more stations, circles with radius D can be drawn with each circle centred at the respective station. • The epicentre lies in the region where the circles overlap. • This method was commonly used as a quick means of locating earthquakes.
  • 10.
  • 11. • The focal depth (H) can be obtained as: • Adding more observations will give additional intersections that theoretically should pass through the epicentre. • In practice, error is always present, both in data and in assumptions, that the ray-paths are straight and the Earth is homogeneous, so scatter in the intersection usually occurs.
  • 12. Origin Time of an Earthquake • The origin time of an earthquake can be determined with a very simple graphical technique, called Wadati plot (Wadati, 1933). • The time separation of the P and S phase (Ts – Tp) is plotted against the arrival time of the Pwave. • Since Ts – Tp = 0 at the hypocentre, a straight line fit on the Wadati diagram gives the origin time at the intercept with the P-arrival-time axis