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Introduction to Geophysics Ali Oncel [email_address] Department of Earth Sciences KFUPM Earthquake Seismology: Fundamentals 1
Fairly   thick layers   result in distinct events on travel time graph Seismic Waves:  As Probes of Earth’s Interior Travel Time Models for FLAT EARTH
Travel Time Models of earthquakes for FLAT EARTH Series of thin layers results in rays that emerge at steeper  angles with   increasing depth .   Slopes of first arrivals change with distance, indicating the changing velocities with depth.
Numerous layers   so thin   that the changing velocity  with depth is modeled   as a function V(Z).   Deep-penetrating rays, having encountered   faster velocities ,  emerge at   steeper angles   than the shallower rays.  The   changing wave front   angles result in   changing apparent velocity , evident as changing slope on the travel-time graph. Travel Time Models of Earthquakes for FLAT EARTH
Summary: Travel Time Models
Earth with   constant   seismic velocity (V).  Ray paths are   linear   because   no refraction   occurs.  The convex-upward   form of the graph is simply because   measurements are along   Earth’s curved surface. Travel Time Models of Earthquakes for Curved EARTH
Rays bend away from the vertical, leading to   steeper emergence angles   (hence, higher apparent velocities) than for the constant velocity case in (a).  Likewise, more curvature on the travel-time graph indicates higher apparent velocity than in (a).  Earth model with a gradual increase in velocity with depth, V(z).
Selected ray paths and travel-time curves for body (P,S) and surface waves.  As in (b), seismic velocities increase with depth.
Travel Time Models of Earthquakes for Curved EARTH
Questions?
Next Lecture Field Measured Refraction Velocity

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ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS

  • 1. Introduction to Geophysics Ali Oncel [email_address] Department of Earth Sciences KFUPM Earthquake Seismology: Fundamentals 1
  • 2. Fairly thick layers result in distinct events on travel time graph Seismic Waves: As Probes of Earth’s Interior Travel Time Models for FLAT EARTH
  • 3. Travel Time Models of earthquakes for FLAT EARTH Series of thin layers results in rays that emerge at steeper angles with increasing depth . Slopes of first arrivals change with distance, indicating the changing velocities with depth.
  • 4. Numerous layers so thin that the changing velocity with depth is modeled as a function V(Z). Deep-penetrating rays, having encountered faster velocities , emerge at steeper angles than the shallower rays. The changing wave front angles result in changing apparent velocity , evident as changing slope on the travel-time graph. Travel Time Models of Earthquakes for FLAT EARTH
  • 6. Earth with constant seismic velocity (V). Ray paths are linear because no refraction occurs. The convex-upward form of the graph is simply because measurements are along Earth’s curved surface. Travel Time Models of Earthquakes for Curved EARTH
  • 7. Rays bend away from the vertical, leading to steeper emergence angles (hence, higher apparent velocities) than for the constant velocity case in (a). Likewise, more curvature on the travel-time graph indicates higher apparent velocity than in (a). Earth model with a gradual increase in velocity with depth, V(z).
  • 8. Selected ray paths and travel-time curves for body (P,S) and surface waves. As in (b), seismic velocities increase with depth.
  • 9. Travel Time Models of Earthquakes for Curved EARTH
  • 11. Next Lecture Field Measured Refraction Velocity