SlideShare a Scribd company logo
9
Most read
15
Most read
20
Most read
Seismic Refraction
Method
Overview
Prepared by
Dr. Amin Khalil
Seismic refraction method lecture 21
TYPES AND PROPERTIES OF SEISMIC
WAVES
• There are two types of elastic body wave in a solid:
– P-Waves: compression waves
– S-waves: shear waves
• P-waves are the faster and are usually the ones studied in
simple seismic methods.
• Other waves (surface waves) also exist but are much slower.
It is these waves that do the damage in earthquakes.
• We will focus our attention on P-waves from now on.
Compressional (“P”) Wave
Identical to sound wave – particle motion is parallel to propagation
direction.
Animation courtesy Larry Braile, Purdue University
Shear (“S”) Wave
Particle motion is perpendicular
to propagation direction.
Animation courtesy Larry Braile, Purdue University
Velocity of Seismic Waves
Depends on density elastic moduli


3
4


K
Vp


Vs
where K = bulk modulus,  = shear modulus, and
 = density.
Velocity of Seismic Waves
Bulk modulus = resistance to
compression = incompressibility
Shear modulus = resistance to
shear = rigidity
The less compressible a material is, the greater its p-wave
velocity, i.e., sound travels about four times faster in water
than in air. The more resistant a material is to shear, the
greater its shear wave velocity.
RIGIDITY
It a measure of how the medium resist the change in shape. Hence, rigidity in
fluids and fluid-like media is zero. This mean that no shear wave (S-waves) are
travelling in fluids.
This property help in the identification that the outer core is liquid like shell.
Surface waves in an elastic solid
Seismic refraction method lecture 21
Seismic waves at an interface
What happen when seismic waves encounters an
interface?!!!
We start by defining some important
phenomena:
1- Seismic wave propagation in a media is dependent on
elastic impedance Z. The elastic impedance Z is defined
by:
Z=  v
Where:
  density
v= seismic velocity
At an interface
Seismic waves exhibit number of actions named collectively as
energy partition at an interface. The seismic waves are reflected,
refracted and converted from P to S and from S to P. The
reflection is governed by the reflection coefficient which represent
the percentage of the energy that will be reflected.
Energy Partition
21
12
zz
zz
R



REFLECTION Coefficient is defined by:
Where Z1 and Z2 are the impedances
for the first and second layer
respectivley.
Seismic refraction method lecture 21
Seismic refraction method lecture 21
Basic laws:
Snell Law
Reciprocity law
Snell’ law
This law control the refraction of seismic energy
at an interface:
2
1
2
1
)sin(
)sin(
V
V
i
i

Where i1 and i2 are the incident and refracted
angles and V1 and V2 are velocities of the first
layer and second layer respectively.
Primarily, refraction method depends on
the hypothesis that velocity increases with
depth. This is because refracted waves to
be recorded by an array of geophones on
the surface should be critically refracted,
i.e. The refraction angle be 90o , in this
case the refracted energy propagate
parallel to interface with the speed of the
faster second layer. This type of
propagation is called head waves. Head
waves itself acts as seismic rays incident
at the interface with 90o angle and
refraction back to the surface is then taking
place
source geophone
V1
V2
ic
ic
Ic is the angle of critical refraction and is given by:
Ic =sin-1 (V1 /V2 )
Snell’s Law
If V2>V1, then as i increases, r
increases faster
Principal of Reciprocity
• The travel time of seismic energy
between two points is independent
of the direction traveled, i.e.,
interchanging the source and the
geophone will not affect the seismic
travel time between the two.
END

More Related Content

PPTX
Seismic refraction method lec22
PDF
Seismic Methods
PPTX
Introduction to Seismic Method
PPT
Fundamentals of Seismic Refraction
PDF
Seismic Refraction Surveying
PPTX
Seismic Reflection
PPT
Refraction Seismic
PPTX
Role of Geophysics in the Oil and Gas Industry
Seismic refraction method lec22
Seismic Methods
Introduction to Seismic Method
Fundamentals of Seismic Refraction
Seismic Refraction Surveying
Seismic Reflection
Refraction Seismic
Role of Geophysics in the Oil and Gas Industry

What's hot (20)

PPTX
SEISMIC METHOD
PPT
Sequence stratigraphy and its applications
PPT
Sequence Stratigraphy - Principles
PDF
Seismic Refraction Test
PPTX
Seismic stratigraphy
PPTX
Geophysical methods brief summary
PDF
Magnetic Survey
PPTX
Paired metamorphic belts
PPT
Determination of strike and dip and geological cross section
PPT
Structur Alanalysis
PPTX
Sedimentary depositional environments
 
PPTX
Gravity and magmetic method
PPT
Magnetic prospecting
PPTX
Introduction to Sedimentary Rocks
PPTX
Geophysics (definition,scope and applications)
PPTX
Geochemical methods in mineral exploration
PPTX
Southern granulite
PPTX
Gravity anomaly across reagional structures
PDF
Self Potential Method (Electrical Survey)
SEISMIC METHOD
Sequence stratigraphy and its applications
Sequence Stratigraphy - Principles
Seismic Refraction Test
Seismic stratigraphy
Geophysical methods brief summary
Magnetic Survey
Paired metamorphic belts
Determination of strike and dip and geological cross section
Structur Alanalysis
Sedimentary depositional environments
 
Gravity and magmetic method
Magnetic prospecting
Introduction to Sedimentary Rocks
Geophysics (definition,scope and applications)
Geochemical methods in mineral exploration
Southern granulite
Gravity anomaly across reagional structures
Self Potential Method (Electrical Survey)
Ad

Similar to Seismic refraction method lecture 21 (20)

PPT
Seismic waves
PPTX
seismic mentioned that going on dov.pptx
PDF
Basic seismology
PDF
Acoustic Waves for Geoscience. Good for students
PPT
propagation seismic waves w p waves .ppt
PPTX
Seismology and earthquake
PPT
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
PDF
Geophysical data analysis
PPTX
Seismic wave propagation
PPTX
SD.pptx of soil dynamics mtech presentation
PDF
Seismic Interpretation and Modelling_4 Grade_Tanta University.pdf
PPTX
Seismic waves (1).pptx
PPT
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
PPTX
EarthsInterior.pptx
PPT
seismicwaves-ppt presentation in science 10
PPT
seismicwaves-.ppt presentation for grade 10 science
PDF
Shearwaves2
PPTX
Seismic_Refraction_for_class_1.pptxhhhhh
PPT
Seismic Waves quarter 1 for Grade 10.ppt
PPT
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
Seismic waves
seismic mentioned that going on dov.pptx
Basic seismology
Acoustic Waves for Geoscience. Good for students
propagation seismic waves w p waves .ppt
Seismology and earthquake
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
Geophysical data analysis
Seismic wave propagation
SD.pptx of soil dynamics mtech presentation
Seismic Interpretation and Modelling_4 Grade_Tanta University.pdf
Seismic waves (1).pptx
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
EarthsInterior.pptx
seismicwaves-ppt presentation in science 10
seismicwaves-.ppt presentation for grade 10 science
Shearwaves2
Seismic_Refraction_for_class_1.pptxhhhhh
Seismic Waves quarter 1 for Grade 10.ppt
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
Ad

More from Amin khalil (20)

PPTX
Isostacy
PPTX
Application of integrated geophysical technique for the mapping
PPTX
Brief discussion on inverse Theory
PPTX
Staclim2016
PPTX
Importing data in Oasis Montaj
PPTX
Oasis montaj workshop session 1
PPTX
Extended seismic data processing dmo
PPTX
Extended seismic data processing lec25, fk filtering
PPTX
Extended seismic processing sequence lecture 24
PPTX
Lecture 23 april29 static correction
PPTX
Lecture 20, marine surveying 2
PPTX
Lecture 19, marine seismic surveying
PPTX
Seismic data processing 16, migration&land seismic survey
PPTX
Seismic data processing 15, kirchhof migration
PPTX
Seismic data processing 14, stacking&migration2
PPTX
Seismic data processing 13 stacking&migration
PPTX
Seismic data processing
PPTX
Import waveform files into seisan
PPTX
Earthquake ground motion simulation during 1992 cairo earthquake
PPTX
Seismic reflection at lang kawi
Isostacy
Application of integrated geophysical technique for the mapping
Brief discussion on inverse Theory
Staclim2016
Importing data in Oasis Montaj
Oasis montaj workshop session 1
Extended seismic data processing dmo
Extended seismic data processing lec25, fk filtering
Extended seismic processing sequence lecture 24
Lecture 23 april29 static correction
Lecture 20, marine surveying 2
Lecture 19, marine seismic surveying
Seismic data processing 16, migration&land seismic survey
Seismic data processing 15, kirchhof migration
Seismic data processing 14, stacking&migration2
Seismic data processing 13 stacking&migration
Seismic data processing
Import waveform files into seisan
Earthquake ground motion simulation during 1992 cairo earthquake
Seismic reflection at lang kawi

Recently uploaded (20)

PDF
TR - Agricultural Crops Production NC III.pdf
PDF
O5-L3 Freight Transport Ops (International) V1.pdf
PDF
2.FourierTransform-ShortQuestionswithAnswers.pdf
PDF
Abdominal Access Techniques with Prof. Dr. R K Mishra
PPTX
Cell Types and Its function , kingdom of life
PPTX
Cell Structure & Organelles in detailed.
PDF
Saundersa Comprehensive Review for the NCLEX-RN Examination.pdf
PPTX
school management -TNTEU- B.Ed., Semester II Unit 1.pptx
PPTX
Final Presentation General Medicine 03-08-2024.pptx
PDF
Anesthesia in Laparoscopic Surgery in India
PDF
Supply Chain Operations Speaking Notes -ICLT Program
PDF
Pre independence Education in Inndia.pdf
PPTX
Institutional Correction lecture only . . .
PDF
Module 4: Burden of Disease Tutorial Slides S2 2025
PPTX
IMMUNITY IMMUNITY refers to protection against infection, and the immune syst...
PDF
O7-L3 Supply Chain Operations - ICLT Program
PPTX
Pharmacology of Heart Failure /Pharmacotherapy of CHF
PDF
BÀI TẬP BỔ TRỢ 4 KỸ NĂNG TIẾNG ANH 9 GLOBAL SUCCESS - CẢ NĂM - BÁM SÁT FORM Đ...
PPTX
Lesson notes of climatology university.
PDF
The Lost Whites of Pakistan by Jahanzaib Mughal.pdf
TR - Agricultural Crops Production NC III.pdf
O5-L3 Freight Transport Ops (International) V1.pdf
2.FourierTransform-ShortQuestionswithAnswers.pdf
Abdominal Access Techniques with Prof. Dr. R K Mishra
Cell Types and Its function , kingdom of life
Cell Structure & Organelles in detailed.
Saundersa Comprehensive Review for the NCLEX-RN Examination.pdf
school management -TNTEU- B.Ed., Semester II Unit 1.pptx
Final Presentation General Medicine 03-08-2024.pptx
Anesthesia in Laparoscopic Surgery in India
Supply Chain Operations Speaking Notes -ICLT Program
Pre independence Education in Inndia.pdf
Institutional Correction lecture only . . .
Module 4: Burden of Disease Tutorial Slides S2 2025
IMMUNITY IMMUNITY refers to protection against infection, and the immune syst...
O7-L3 Supply Chain Operations - ICLT Program
Pharmacology of Heart Failure /Pharmacotherapy of CHF
BÀI TẬP BỔ TRỢ 4 KỸ NĂNG TIẾNG ANH 9 GLOBAL SUCCESS - CẢ NĂM - BÁM SÁT FORM Đ...
Lesson notes of climatology university.
The Lost Whites of Pakistan by Jahanzaib Mughal.pdf

Seismic refraction method lecture 21

  • 3. TYPES AND PROPERTIES OF SEISMIC WAVES • There are two types of elastic body wave in a solid: – P-Waves: compression waves – S-waves: shear waves • P-waves are the faster and are usually the ones studied in simple seismic methods. • Other waves (surface waves) also exist but are much slower. It is these waves that do the damage in earthquakes. • We will focus our attention on P-waves from now on.
  • 4. Compressional (“P”) Wave Identical to sound wave – particle motion is parallel to propagation direction. Animation courtesy Larry Braile, Purdue University
  • 5. Shear (“S”) Wave Particle motion is perpendicular to propagation direction. Animation courtesy Larry Braile, Purdue University
  • 6. Velocity of Seismic Waves Depends on density elastic moduli   3 4   K Vp   Vs where K = bulk modulus,  = shear modulus, and  = density.
  • 7. Velocity of Seismic Waves Bulk modulus = resistance to compression = incompressibility Shear modulus = resistance to shear = rigidity The less compressible a material is, the greater its p-wave velocity, i.e., sound travels about four times faster in water than in air. The more resistant a material is to shear, the greater its shear wave velocity.
  • 8. RIGIDITY It a measure of how the medium resist the change in shape. Hence, rigidity in fluids and fluid-like media is zero. This mean that no shear wave (S-waves) are travelling in fluids. This property help in the identification that the outer core is liquid like shell.
  • 9. Surface waves in an elastic solid
  • 11. Seismic waves at an interface What happen when seismic waves encounters an interface?!!!
  • 12. We start by defining some important phenomena: 1- Seismic wave propagation in a media is dependent on elastic impedance Z. The elastic impedance Z is defined by: Z=  v Where:   density v= seismic velocity
  • 13. At an interface Seismic waves exhibit number of actions named collectively as energy partition at an interface. The seismic waves are reflected, refracted and converted from P to S and from S to P. The reflection is governed by the reflection coefficient which represent the percentage of the energy that will be reflected.
  • 15. 21 12 zz zz R    REFLECTION Coefficient is defined by: Where Z1 and Z2 are the impedances for the first and second layer respectivley.
  • 19. Snell’ law This law control the refraction of seismic energy at an interface: 2 1 2 1 )sin( )sin( V V i i  Where i1 and i2 are the incident and refracted angles and V1 and V2 are velocities of the first layer and second layer respectively.
  • 20. Primarily, refraction method depends on the hypothesis that velocity increases with depth. This is because refracted waves to be recorded by an array of geophones on the surface should be critically refracted, i.e. The refraction angle be 90o , in this case the refracted energy propagate parallel to interface with the speed of the faster second layer. This type of propagation is called head waves. Head waves itself acts as seismic rays incident at the interface with 90o angle and refraction back to the surface is then taking place
  • 21. source geophone V1 V2 ic ic Ic is the angle of critical refraction and is given by: Ic =sin-1 (V1 /V2 )
  • 22. Snell’s Law If V2>V1, then as i increases, r increases faster
  • 23. Principal of Reciprocity • The travel time of seismic energy between two points is independent of the direction traveled, i.e., interchanging the source and the geophone will not affect the seismic travel time between the two.
  • 24. END

Editor's Notes

  • #8: P-WAVE IS SENSITIVE TO RESISTANCE TO CHANGE IN VOLUME, WHEREAS S-WAVES IS DEPENDENT ON THE RESISTANCE TO CHANGE IN SHAPE.