seismic exploration: fundementals-2
TRANSCRIPT
Introduction to Geophysics
Ali [email protected].
saDepartment of Earth SciencesKFUPM
Seismic Exploration: Fundamentals 2
Previous Lecture
Huygens's Principle Fermat's Principle Travel-time Graph Estimates of Seismic Velocity Reflected/Refracted waves Model Calculation for simple, horizontal, two layers Ray Paths Snell's law-Critically Refracted Arrival Seismic Refraction Behavior of refracted ray on velocity changes
12°
15°20°
35°
#1 #2 #3
medium 1
medium 2
A ray incident on surface results in 3 reflected and refracted rays. If the seismic velocities in medium 1 are α = 6.5 km/sec, β = 3.8 km/sec, what are the seismic velocities in medium 2? What type of material is medium2? Identify rays #1, #2, #3, #4
as P or S waves.
Homework Due to Wednesday
Energy Return and Critical Angle
A critically refracted wave, traveling at the top of
the lower layer with velocity V2, leaks energy back
into the upper layer at the critical angle (θ2)
c c c c c c
Lillie, Whole Earth Geophysics, Fig 3.25
Angle of For Incident P wave For Incident S waveIncidence Reflected Refracted Reflected Refracted
P-wave S-wave P-wave S-wave S-wave P-wave S-wave P-wave10 10 6 28 16 10 17 28 5111 11 7 31 18 11 19 31 5812 12 7 34 19 12 20 34 6813 13 8 37 21 13 22 37 8914 14 8 40 23 14 24 40 #NUM!15 15 9 44 24 15 26 44 #NUM!16 16 10 47 26 16 27 47 #NUM!17 17 10 51 28 17 29 51 #NUM!18 18 11 55 30 18 31 55 #NUM!19 19 11 60 31 19 33 60 #NUM!20 20 12 66 33 20 35 66 #NUM!21 21 12 73 35 21 37 73 #NUM!22 22 13 87 37 22 39 87 #NUM!23 23 14 #NUM! 39 23 41 #NUM! #NUM!24 24 14 #NUM! 41 24 43 #NUM! #NUM!25 25 15 #NUM! 43 25 45 #NUM! #NUM!26 26 15 #NUM! 45 26 47 #NUM! #NUM!27 27 16 #NUM! 47 27 49 #NUM! #NUM!28 28 16 #NUM! 49 28 51 #NUM! #NUM!29 29 17 #NUM! 51 29 54 #NUM! #NUM!30 30 17 #NUM! 53 30 56 #NUM! #NUM!
Modified Table 2.3 after Berger, pp.29.V1-P (m/s) 1500
V1-S (m/s) 900V2-P (m/s) 4000V2-S (m/s) 2400
Xc=critical distance
Xcr=crossover distance
T1= Intercept time
Travel time for Direct/Refracted Waves
12
2112 VV
VVhxcr
Xc=critical distance
Xcr=crossover distance
T1= Intercept time
Seismic Reflection
Reflection occurs when Z1 differs from Z2, where Z
Acoustic impedance which is product of density and velocityV-shaped ray paths for a compressional wave from a
source to 6 receivers, reflected from a horizontal
interface.
=Z1
=Z2
Lillie, Whole Earth Geophysics, Fig 3.28
These exercises are designed to illustrates some of the basic characteristics of wave propagation in a single layer model use ray-tracing concepts to determine the arrival times of particular events. These exercises require that you construct the time-distance plot for the given model. In addition to
constructing the time-distance plots,
Due to Next Week
INTRODUCTORY RAY TRACING EXERCISESGENERAL INSTRUCTIONS
http://www.mines.edu/fs_home/tboyd/GP311/MODULES/SEIS/NOTES/deriv1.html
Observational DataDistance Direct Refracted Reflected
Arrival Arrivalft ft/sec
0 0.00 0.17 0.20500 0.10 0.22 0.22
1000 0.20 0.27 0.281500 0.30 0.32 0.362000 0.40 0.37 0.452500 0.50 0.42 0.543000 0.60 0.47 0.633500 0.70 0.52 0.734000 0.80 0.57 0.824500 0.90 0.62 0.925000 1.00 0.67 1.02
Single-Layer Model
XV
tdirect
1
1
21
21
21
2 4
V
h
V
Xtreflection
21
22
21
1
2
21VV
VV
hX
Vtrefraction
Equations