SlideShare a Scribd company logo
1 of 18
Solid Earth Geophysics-Geop503  Ali Oncel [email_address] Department of Earth Sciences, KFUPM Seismic Waves and Earth’s Interior Reading: Fowler Chapter 8- Section 8.1
Summary: Lecture 5 ,[object Object],[object Object],[object Object],[object Object],[object Object]
Recall: Low-Velocity Layer Guttenberg (1959) inferred its existence from changes in the amplitude of arrivals, at distances of around 15 degree, which he attributed to the defocusing effect of a low-velocity region. There are two possible scenarios that produce hidden layers:   Low velocity layers and thin layers underlain by a large velocity contrast. Layers that can not be distinguished from first arrival time information are known as hidden layers.
Antipodal Focusing ,[object Object],[object Object],Fig. 3.5- 6 of Stein 2003
Example: May 23, 1968 ,[object Object],[object Object],New Zealand Porto Malaga The waves are focused and strongly amplified up to 1 order of magnitude with respect to the normal phase recorded 2° or more away.  Source: Rial, J. A.; Cormier, V. F. (1980, JGR):
Wave Animations Allen Jones http:// bingweb.binghamton.edu /~ajones/#Seismic%20Waves Seismic Waves : A program for the visualization of wave propagation Contributor:  Alan Jones  Year: 2006
Ray paths from the Peru event for major P and S phases through the AK135 model Mw= 8.1 Depth= 33 km   Date:  Saturday, June 23 Visualizing Body Waves: Peru  Event www.rses.anu.edu.au/seismology/SHon2002/sq1sw.pdf
Peru Earthquake Despite its large size, the earthquake left a death toll of only 75 persons, including 26 who died as a result of the subsequent  tsunami ,  which also caused the disappearance of 64 people.  (Source:  Wikipedia )
Expected Arrival Times:AKI135 Model
[object Object],[object Object],3D P-wave Propagation of Peru EQ
[object Object],[object Object],3D P-wave Propagation of Peru EQ
On a seismometer located at an earthquake epicenter  PcP  and  ScS  arrives  8 minutes, 34 seconds  and  15 minutes, 36 seconds  respectively after the earthquake. If the earth’s radius at this point is 6371 km, and the core’s radius is 3471 km, find the average P and S wave velocities in the earth’s mantle. (Remember it takes time to go both up and down!). When would the phase  PcS  arrive? (Note: assume that both paths are vertically incident). Ray Tracing Exercise 5 minutes 6371 3471 T  PcP =514s T  ScS =936s
The phase  PcS  takes 724.3 s or 12 minutes and 4 seconds to arrive at the station.
tt  PcP  ( Δ =0) = 511.3 s  tt  PkikP  ( Δ =0)   = 994.6 s α oc  = 9.34 km/s Reference:  Problem 13 a of Stein and Wysession in Chapter 3 5 minutes Use the travel times for PcP and PKiKP at a vertical incidence to estimate the average P-wave velocity in the outer core? 16.6 min 8.5 min α oc  = 2 (3480-1222) 994.6 – 511.3
[object Object],Reference:  Problem 13 b of Stein and Wysession in Chapter 3
Use the travel times  in the left and previous slide for PKiKP and PKIKP at vertical incidence to estimate the average  P-wave velocity in the inner core . Reference:  Problem 13 b of Stein and Wysession in Chapter 3 5 minutes tt  PKIKP  ( Δ =0) = 1212.1 s  tt  PkikP  ( Δ =0)   = 994.6 s α ic  = 11.24 km/s 20.20 min Fig.3.5-7 of Stein and Wysession α ic  = 2 (1222) 1212.1-994.6
Body Wave Velocity Structure 1.What is  the P wave velocity  in this area (km/s)? 2. What is  the origin time  of the earthquake (using only graph 1) ? Plot your P wave arrival time data on the first graph and plot your S wave arrival time data on the second graph. 3. What is  the S wave velocity  in this area (km/s)? 4. What is  the origin time  of the earthquake (using only graph 2) ? 5. Are the two origin times equal ? Why or why not? P-wave Data S-wave Data
What is the P wave velocity in this area (km/s)?  5.51km/s What is the origin time of the earthquake (using only graph 1)?  ? 27.41/ 5.51 = 4.97, so answer is 10:33:0.4.97 What is the S wave velocity in this area (km/s)?  3.26 km/s What is the origin time of the earthquake (using only graph 2) ? 16.23/3.26 = 4.97, so answer is 10:33:0.4.97 Are the two origin times equal ? Why or why not?  The origin times are equal, but only because I did the problem mathematically. If you did the problem graphically you can expect to get slightly different answers. Y= Distance in km X= Time in sec. P-wave Data S-wave Data

More Related Content

What's hot

Fraunhoffer diffraction
Fraunhoffer diffractionFraunhoffer diffraction
Fraunhoffer diffractionPrasad Gaikwad
 
Rutherford scattering show
Rutherford scattering showRutherford scattering show
Rutherford scattering showKhemendra shukla
 
Phase retardation plates
Phase retardation platesPhase retardation plates
Phase retardation platesPriyamvada003
 
Classical Statistics and Quantum Statistics
Classical Statistics and Quantum StatisticsClassical Statistics and Quantum Statistics
Classical Statistics and Quantum StatisticsDrRamBhosale
 
interference & diffraction
 interference & diffraction interference & diffraction
interference & diffractionRutikRathod
 
Maxwell equation
Maxwell equationMaxwell equation
Maxwell equationKumar
 
Makalah Radiasi Panas dan Radiasi Benda Hitam
Makalah Radiasi Panas dan Radiasi Benda HitamMakalah Radiasi Panas dan Radiasi Benda Hitam
Makalah Radiasi Panas dan Radiasi Benda Hitamkurniawanapr
 
advanced engineering mathematics-erwin kreyszig.pdf
advanced engineering mathematics-erwin kreyszig.pdfadvanced engineering mathematics-erwin kreyszig.pdf
advanced engineering mathematics-erwin kreyszig.pdfcibeyo cibeyo
 
PM [D01] Matter Waves
PM [D01] Matter WavesPM [D01] Matter Waves
PM [D01] Matter WavesStephen Kwong
 
Nuclear physics 3 lectures
Nuclear physics 3 lecturesNuclear physics 3 lectures
Nuclear physics 3 lecturesZeeshan Khalid
 
Michelson Morley experiment
Michelson Morley experiment Michelson Morley experiment
Michelson Morley experiment BidyutSinha3
 

What's hot (20)

Fraunhoffer diffraction
Fraunhoffer diffractionFraunhoffer diffraction
Fraunhoffer diffraction
 
Kuis1 elektrodinamika-2014-2015
Kuis1 elektrodinamika-2014-2015Kuis1 elektrodinamika-2014-2015
Kuis1 elektrodinamika-2014-2015
 
Ch.13
Ch.13Ch.13
Ch.13
 
Rutherford scattering show
Rutherford scattering showRutherford scattering show
Rutherford scattering show
 
STRUCTURE OF SODIUM D LINE
STRUCTURE OF SODIUM D  LINESTRUCTURE OF SODIUM D  LINE
STRUCTURE OF SODIUM D LINE
 
Gauss’s Law
Gauss’s LawGauss’s Law
Gauss’s Law
 
Phase retardation plates
Phase retardation platesPhase retardation plates
Phase retardation plates
 
Michelson - Morley Experiment - B.Sc Physics - I Year- Mechanics
Michelson - Morley Experiment - B.Sc Physics - I Year- MechanicsMichelson - Morley Experiment - B.Sc Physics - I Year- Mechanics
Michelson - Morley Experiment - B.Sc Physics - I Year- Mechanics
 
Classical Statistics and Quantum Statistics
Classical Statistics and Quantum StatisticsClassical Statistics and Quantum Statistics
Classical Statistics and Quantum Statistics
 
interference & diffraction
 interference & diffraction interference & diffraction
interference & diffraction
 
Bunyi 1-1
Bunyi 1-1Bunyi 1-1
Bunyi 1-1
 
Maxwell equation
Maxwell equationMaxwell equation
Maxwell equation
 
Makalah Radiasi Panas dan Radiasi Benda Hitam
Makalah Radiasi Panas dan Radiasi Benda HitamMakalah Radiasi Panas dan Radiasi Benda Hitam
Makalah Radiasi Panas dan Radiasi Benda Hitam
 
advanced engineering mathematics-erwin kreyszig.pdf
advanced engineering mathematics-erwin kreyszig.pdfadvanced engineering mathematics-erwin kreyszig.pdf
advanced engineering mathematics-erwin kreyszig.pdf
 
gauss law and application Arun kumar
gauss law and application Arun kumargauss law and application Arun kumar
gauss law and application Arun kumar
 
Metode Runge Kutta .pdf
Metode Runge Kutta .pdfMetode Runge Kutta .pdf
Metode Runge Kutta .pdf
 
PM [D01] Matter Waves
PM [D01] Matter WavesPM [D01] Matter Waves
PM [D01] Matter Waves
 
Nuclear physics 3 lectures
Nuclear physics 3 lecturesNuclear physics 3 lectures
Nuclear physics 3 lectures
 
Fisika Statistik
Fisika StatistikFisika Statistik
Fisika Statistik
 
Michelson Morley experiment
Michelson Morley experiment Michelson Morley experiment
Michelson Morley experiment
 

Similar to ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS

ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSAli Osman Öncel
 
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSAli Osman Öncel
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSAli Osman Öncel
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSAli Osman Öncel
 
Evidence of a plume on Europa from Galileo magnetic and plasma wave signatures
Evidence of a plume on Europa from Galileo magnetic and plasma wave signaturesEvidence of a plume on Europa from Galileo magnetic and plasma wave signatures
Evidence of a plume on Europa from Galileo magnetic and plasma wave signaturesSérgio Sacani
 
موقعیت صفحه توران.pdf
موقعیت صفحه توران.pdfموقعیت صفحه توران.pdf
موقعیت صفحه توران.pdfmahnazsabahi
 
Estimation of Dipping Angles of Refracting Interfaces
Estimation of Dipping Angles of Refracting InterfacesEstimation of Dipping Angles of Refracting Interfaces
Estimation of Dipping Angles of Refracting Interfacesiosrjce
 
Propagation usgs
Propagation usgsPropagation usgs
Propagation usgsaburocket33
 
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSAli Osman Öncel
 
case study seminar
case study seminarcase study seminar
case study seminarCharu Kamra
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSAli Osman Öncel
 
ÖNCEL AKADEMİ: İSTANBUL DEPREMİ
ÖNCEL AKADEMİ: İSTANBUL DEPREMİÖNCEL AKADEMİ: İSTANBUL DEPREMİ
ÖNCEL AKADEMİ: İSTANBUL DEPREMİAli Osman Öncel
 
First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...
First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...
First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...Sérgio Sacani
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSAli Osman Öncel
 
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSAli Osman Öncel
 
Ambient noise correlation technique
Ambient noise correlation techniqueAmbient noise correlation technique
Ambient noise correlation techniqueVIVEKANAND GUPTA
 
The October 2004 Mw=7.1 Nicaragua earthquake: Rupture process, aftershock loc...
The October 2004 Mw=7.1 Nicaragua earthquake: Rupture process, aftershock loc...The October 2004 Mw=7.1 Nicaragua earthquake: Rupture process, aftershock loc...
The October 2004 Mw=7.1 Nicaragua earthquake: Rupture process, aftershock loc...Gus Alex Reyes
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSAli Osman Öncel
 

Similar to ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS (20)

ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
 
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
 
Brazil2
Brazil2Brazil2
Brazil2
 
Evidence of a plume on Europa from Galileo magnetic and plasma wave signatures
Evidence of a plume on Europa from Galileo magnetic and plasma wave signaturesEvidence of a plume on Europa from Galileo magnetic and plasma wave signatures
Evidence of a plume on Europa from Galileo magnetic and plasma wave signatures
 
موقعیت صفحه توران.pdf
موقعیت صفحه توران.pdfموقعیت صفحه توران.pdf
موقعیت صفحه توران.pdf
 
Estimation of Dipping Angles of Refracting Interfaces
Estimation of Dipping Angles of Refracting InterfacesEstimation of Dipping Angles of Refracting Interfaces
Estimation of Dipping Angles of Refracting Interfaces
 
Propagation usgs
Propagation usgsPropagation usgs
Propagation usgs
 
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
 
case study seminar
case study seminarcase study seminar
case study seminar
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
 
ÖNCEL AKADEMİ: İSTANBUL DEPREMİ
ÖNCEL AKADEMİ: İSTANBUL DEPREMİÖNCEL AKADEMİ: İSTANBUL DEPREMİ
ÖNCEL AKADEMİ: İSTANBUL DEPREMİ
 
First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...
First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...
First Observation of the Earth’s Permanent FreeOscillation s on Ocean Bottom ...
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
 
Caribbean3.ppt
Caribbean3.pptCaribbean3.ppt
Caribbean3.ppt
 
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICSÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS
 
Ambient noise correlation technique
Ambient noise correlation techniqueAmbient noise correlation technique
Ambient noise correlation technique
 
The October 2004 Mw=7.1 Nicaragua earthquake: Rupture process, aftershock loc...
The October 2004 Mw=7.1 Nicaragua earthquake: Rupture process, aftershock loc...The October 2004 Mw=7.1 Nicaragua earthquake: Rupture process, aftershock loc...
The October 2004 Mw=7.1 Nicaragua earthquake: Rupture process, aftershock loc...
 
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICSÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
ÖNCEL AKADEMİ: INTRODUCTION TO GEOPHYSICS
 

More from Ali Osman Öncel

Riskli Yapılar - Çevre ve Şehircilik
Riskli Yapılar - Çevre ve ŞehircilikRiskli Yapılar - Çevre ve Şehircilik
Riskli Yapılar - Çevre ve ŞehircilikAli Osman Öncel
 
Riskli Yapılar -Çevre ve Şehircilik
Riskli Yapılar -Çevre ve ŞehircilikRiskli Yapılar -Çevre ve Şehircilik
Riskli Yapılar -Çevre ve ŞehircilikAli Osman Öncel
 
Kar Kar Geothermal Field Work
Kar Kar Geothermal Field WorkKar Kar Geothermal Field Work
Kar Kar Geothermal Field WorkAli Osman Öncel
 
High Resolution Earth's Gravitational Field
High Resolution Earth's Gravitational FieldHigh Resolution Earth's Gravitational Field
High Resolution Earth's Gravitational FieldAli Osman Öncel
 
Gravity Predictions for Earthquakes
Gravity Predictions for EarthquakesGravity Predictions for Earthquakes
Gravity Predictions for EarthquakesAli Osman Öncel
 
Nakamura Technique for Soil Characterization
Nakamura Technique for Soil CharacterizationNakamura Technique for Soil Characterization
Nakamura Technique for Soil CharacterizationAli Osman Öncel
 
Geopsy: Seismic Vibration Processing
Geopsy: Seismic Vibration ProcessingGeopsy: Seismic Vibration Processing
Geopsy: Seismic Vibration ProcessingAli Osman Öncel
 

More from Ali Osman Öncel (20)

APA Yazım Kuralları
APA Yazım KurallarıAPA Yazım Kuralları
APA Yazım Kuralları
 
Gravimetri : Ders 14
Gravimetri : Ders 14Gravimetri : Ders 14
Gravimetri : Ders 14
 
Gravimetri : Ders 13
Gravimetri : Ders 13Gravimetri : Ders 13
Gravimetri : Ders 13
 
Gravimetri : Ders 12
Gravimetri : Ders 12Gravimetri : Ders 12
Gravimetri : Ders 12
 
Riskli Yapılar - Çevre ve Şehircilik
Riskli Yapılar - Çevre ve ŞehircilikRiskli Yapılar - Çevre ve Şehircilik
Riskli Yapılar - Çevre ve Şehircilik
 
Riskli Yapılar -Çevre ve Şehircilik
Riskli Yapılar -Çevre ve ŞehircilikRiskli Yapılar -Çevre ve Şehircilik
Riskli Yapılar -Çevre ve Şehircilik
 
Gravimetri : Ders 07
Gravimetri : Ders 07Gravimetri : Ders 07
Gravimetri : Ders 07
 
Gravimetri : Ders 06
Gravimetri : Ders 06Gravimetri : Ders 06
Gravimetri : Ders 06
 
Gravimetri: Ders 05
Gravimetri: Ders 05Gravimetri: Ders 05
Gravimetri: Ders 05
 
Gravimetri : Ders 04
Gravimetri : Ders 04Gravimetri : Ders 04
Gravimetri : Ders 04
 
Gravimetri : Ders 03
Gravimetri : Ders 03Gravimetri : Ders 03
Gravimetri : Ders 03
 
Gravimetri Ders 02
Gravimetri Ders 02Gravimetri Ders 02
Gravimetri Ders 02
 
Gravimetri Ders 01
Gravimetri Ders 01Gravimetri Ders 01
Gravimetri Ders 01
 
Kar Kar Geothermal Field Work
Kar Kar Geothermal Field WorkKar Kar Geothermal Field Work
Kar Kar Geothermal Field Work
 
Beppu geothermal field
Beppu geothermal fieldBeppu geothermal field
Beppu geothermal field
 
High Resolution Earth's Gravitational Field
High Resolution Earth's Gravitational FieldHigh Resolution Earth's Gravitational Field
High Resolution Earth's Gravitational Field
 
Gravity Predictions for Earthquakes
Gravity Predictions for EarthquakesGravity Predictions for Earthquakes
Gravity Predictions for Earthquakes
 
Nakamura Technique for Soil Characterization
Nakamura Technique for Soil CharacterizationNakamura Technique for Soil Characterization
Nakamura Technique for Soil Characterization
 
H/V User Guidelines
H/V User Guidelines H/V User Guidelines
H/V User Guidelines
 
Geopsy: Seismic Vibration Processing
Geopsy: Seismic Vibration ProcessingGeopsy: Seismic Vibration Processing
Geopsy: Seismic Vibration Processing
 

Recently uploaded

DATA STRUCTURE AND ALGORITHM for beginners
DATA STRUCTURE AND ALGORITHM for beginnersDATA STRUCTURE AND ALGORITHM for beginners
DATA STRUCTURE AND ALGORITHM for beginnersSabitha Banu
 
MULTIDISCIPLINRY NATURE OF THE ENVIRONMENTAL STUDIES.pptx
MULTIDISCIPLINRY NATURE OF THE ENVIRONMENTAL STUDIES.pptxMULTIDISCIPLINRY NATURE OF THE ENVIRONMENTAL STUDIES.pptx
MULTIDISCIPLINRY NATURE OF THE ENVIRONMENTAL STUDIES.pptxAnupkumar Sharma
 
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...JhezDiaz1
 
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdfAMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdfphamnguyenenglishnb
 
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdfFraming an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdfUjwalaBharambe
 
Solving Puzzles Benefits Everyone (English).pptx
Solving Puzzles Benefits Everyone (English).pptxSolving Puzzles Benefits Everyone (English).pptx
Solving Puzzles Benefits Everyone (English).pptxOH TEIK BIN
 
ACC 2024 Chronicles. Cardiology. Exam.pdf
ACC 2024 Chronicles. Cardiology. Exam.pdfACC 2024 Chronicles. Cardiology. Exam.pdf
ACC 2024 Chronicles. Cardiology. Exam.pdfSpandanaRallapalli
 
Romantic Opera MUSIC FOR GRADE NINE pptx
Romantic Opera MUSIC FOR GRADE NINE pptxRomantic Opera MUSIC FOR GRADE NINE pptx
Romantic Opera MUSIC FOR GRADE NINE pptxsqpmdrvczh
 
Earth Day Presentation wow hello nice great
Earth Day Presentation wow hello nice greatEarth Day Presentation wow hello nice great
Earth Day Presentation wow hello nice greatYousafMalik24
 
Introduction to ArtificiaI Intelligence in Higher Education
Introduction to ArtificiaI Intelligence in Higher EducationIntroduction to ArtificiaI Intelligence in Higher Education
Introduction to ArtificiaI Intelligence in Higher Educationpboyjonauth
 
Keynote by Prof. Wurzer at Nordex about IP-design
Keynote by Prof. Wurzer at Nordex about IP-designKeynote by Prof. Wurzer at Nordex about IP-design
Keynote by Prof. Wurzer at Nordex about IP-designMIPLM
 
Difference Between Search & Browse Methods in Odoo 17
Difference Between Search & Browse Methods in Odoo 17Difference Between Search & Browse Methods in Odoo 17
Difference Between Search & Browse Methods in Odoo 17Celine George
 
Proudly South Africa powerpoint Thorisha.pptx
Proudly South Africa powerpoint Thorisha.pptxProudly South Africa powerpoint Thorisha.pptx
Proudly South Africa powerpoint Thorisha.pptxthorishapillay1
 
Quarter 4 Peace-education.pptx Catch Up Friday
Quarter 4 Peace-education.pptx Catch Up FridayQuarter 4 Peace-education.pptx Catch Up Friday
Quarter 4 Peace-education.pptx Catch Up FridayMakMakNepo
 
ECONOMIC CONTEXT - PAPER 1 Q3: NEWSPAPERS.pptx
ECONOMIC CONTEXT - PAPER 1 Q3: NEWSPAPERS.pptxECONOMIC CONTEXT - PAPER 1 Q3: NEWSPAPERS.pptx
ECONOMIC CONTEXT - PAPER 1 Q3: NEWSPAPERS.pptxiammrhaywood
 
What is Model Inheritance in Odoo 17 ERP
What is Model Inheritance in Odoo 17 ERPWhat is Model Inheritance in Odoo 17 ERP
What is Model Inheritance in Odoo 17 ERPCeline George
 
Full Stack Web Development Course for Beginners
Full Stack Web Development Course  for BeginnersFull Stack Web Development Course  for Beginners
Full Stack Web Development Course for BeginnersSabitha Banu
 

Recently uploaded (20)

DATA STRUCTURE AND ALGORITHM for beginners
DATA STRUCTURE AND ALGORITHM for beginnersDATA STRUCTURE AND ALGORITHM for beginners
DATA STRUCTURE AND ALGORITHM for beginners
 
MULTIDISCIPLINRY NATURE OF THE ENVIRONMENTAL STUDIES.pptx
MULTIDISCIPLINRY NATURE OF THE ENVIRONMENTAL STUDIES.pptxMULTIDISCIPLINRY NATURE OF THE ENVIRONMENTAL STUDIES.pptx
MULTIDISCIPLINRY NATURE OF THE ENVIRONMENTAL STUDIES.pptx
 
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
ENGLISH 7_Q4_LESSON 2_ Employing a Variety of Strategies for Effective Interp...
 
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdfAMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
AMERICAN LANGUAGE HUB_Level2_Student'sBook_Answerkey.pdf
 
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdfFraming an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
Framing an Appropriate Research Question 6b9b26d93da94caf993c038d9efcdedb.pdf
 
OS-operating systems- ch04 (Threads) ...
OS-operating systems- ch04 (Threads) ...OS-operating systems- ch04 (Threads) ...
OS-operating systems- ch04 (Threads) ...
 
Solving Puzzles Benefits Everyone (English).pptx
Solving Puzzles Benefits Everyone (English).pptxSolving Puzzles Benefits Everyone (English).pptx
Solving Puzzles Benefits Everyone (English).pptx
 
ACC 2024 Chronicles. Cardiology. Exam.pdf
ACC 2024 Chronicles. Cardiology. Exam.pdfACC 2024 Chronicles. Cardiology. Exam.pdf
ACC 2024 Chronicles. Cardiology. Exam.pdf
 
Romantic Opera MUSIC FOR GRADE NINE pptx
Romantic Opera MUSIC FOR GRADE NINE pptxRomantic Opera MUSIC FOR GRADE NINE pptx
Romantic Opera MUSIC FOR GRADE NINE pptx
 
Earth Day Presentation wow hello nice great
Earth Day Presentation wow hello nice greatEarth Day Presentation wow hello nice great
Earth Day Presentation wow hello nice great
 
Introduction to ArtificiaI Intelligence in Higher Education
Introduction to ArtificiaI Intelligence in Higher EducationIntroduction to ArtificiaI Intelligence in Higher Education
Introduction to ArtificiaI Intelligence in Higher Education
 
Keynote by Prof. Wurzer at Nordex about IP-design
Keynote by Prof. Wurzer at Nordex about IP-designKeynote by Prof. Wurzer at Nordex about IP-design
Keynote by Prof. Wurzer at Nordex about IP-design
 
Difference Between Search & Browse Methods in Odoo 17
Difference Between Search & Browse Methods in Odoo 17Difference Between Search & Browse Methods in Odoo 17
Difference Between Search & Browse Methods in Odoo 17
 
Proudly South Africa powerpoint Thorisha.pptx
Proudly South Africa powerpoint Thorisha.pptxProudly South Africa powerpoint Thorisha.pptx
Proudly South Africa powerpoint Thorisha.pptx
 
Quarter 4 Peace-education.pptx Catch Up Friday
Quarter 4 Peace-education.pptx Catch Up FridayQuarter 4 Peace-education.pptx Catch Up Friday
Quarter 4 Peace-education.pptx Catch Up Friday
 
9953330565 Low Rate Call Girls In Rohini Delhi NCR
9953330565 Low Rate Call Girls In Rohini  Delhi NCR9953330565 Low Rate Call Girls In Rohini  Delhi NCR
9953330565 Low Rate Call Girls In Rohini Delhi NCR
 
TataKelola dan KamSiber Kecerdasan Buatan v022.pdf
TataKelola dan KamSiber Kecerdasan Buatan v022.pdfTataKelola dan KamSiber Kecerdasan Buatan v022.pdf
TataKelola dan KamSiber Kecerdasan Buatan v022.pdf
 
ECONOMIC CONTEXT - PAPER 1 Q3: NEWSPAPERS.pptx
ECONOMIC CONTEXT - PAPER 1 Q3: NEWSPAPERS.pptxECONOMIC CONTEXT - PAPER 1 Q3: NEWSPAPERS.pptx
ECONOMIC CONTEXT - PAPER 1 Q3: NEWSPAPERS.pptx
 
What is Model Inheritance in Odoo 17 ERP
What is Model Inheritance in Odoo 17 ERPWhat is Model Inheritance in Odoo 17 ERP
What is Model Inheritance in Odoo 17 ERP
 
Full Stack Web Development Course for Beginners
Full Stack Web Development Course  for BeginnersFull Stack Web Development Course  for Beginners
Full Stack Web Development Course for Beginners
 

ÖNCEL AKADEMİ: SOLID EARTH GEOPHYSICS

  • 1. Solid Earth Geophysics-Geop503 Ali Oncel [email_address] Department of Earth Sciences, KFUPM Seismic Waves and Earth’s Interior Reading: Fowler Chapter 8- Section 8.1
  • 2.
  • 3. Recall: Low-Velocity Layer Guttenberg (1959) inferred its existence from changes in the amplitude of arrivals, at distances of around 15 degree, which he attributed to the defocusing effect of a low-velocity region. There are two possible scenarios that produce hidden layers: Low velocity layers and thin layers underlain by a large velocity contrast. Layers that can not be distinguished from first arrival time information are known as hidden layers.
  • 4.
  • 5.
  • 6. Wave Animations Allen Jones http:// bingweb.binghamton.edu /~ajones/#Seismic%20Waves Seismic Waves : A program for the visualization of wave propagation Contributor: Alan Jones Year: 2006
  • 7. Ray paths from the Peru event for major P and S phases through the AK135 model Mw= 8.1 Depth= 33 km Date: Saturday, June 23 Visualizing Body Waves: Peru Event www.rses.anu.edu.au/seismology/SHon2002/sq1sw.pdf
  • 8. Peru Earthquake Despite its large size, the earthquake left a death toll of only 75 persons, including 26 who died as a result of the subsequent tsunami , which also caused the disappearance of 64 people. (Source: Wikipedia )
  • 10.
  • 11.
  • 12. On a seismometer located at an earthquake epicenter PcP and ScS arrives 8 minutes, 34 seconds and 15 minutes, 36 seconds respectively after the earthquake. If the earth’s radius at this point is 6371 km, and the core’s radius is 3471 km, find the average P and S wave velocities in the earth’s mantle. (Remember it takes time to go both up and down!). When would the phase PcS arrive? (Note: assume that both paths are vertically incident). Ray Tracing Exercise 5 minutes 6371 3471 T PcP =514s T ScS =936s
  • 13. The phase PcS takes 724.3 s or 12 minutes and 4 seconds to arrive at the station.
  • 14. tt PcP ( Δ =0) = 511.3 s tt PkikP ( Δ =0) = 994.6 s α oc = 9.34 km/s Reference: Problem 13 a of Stein and Wysession in Chapter 3 5 minutes Use the travel times for PcP and PKiKP at a vertical incidence to estimate the average P-wave velocity in the outer core? 16.6 min 8.5 min α oc = 2 (3480-1222) 994.6 – 511.3
  • 15.
  • 16. Use the travel times in the left and previous slide for PKiKP and PKIKP at vertical incidence to estimate the average P-wave velocity in the inner core . Reference: Problem 13 b of Stein and Wysession in Chapter 3 5 minutes tt PKIKP ( Δ =0) = 1212.1 s tt PkikP ( Δ =0) = 994.6 s α ic = 11.24 km/s 20.20 min Fig.3.5-7 of Stein and Wysession α ic = 2 (1222) 1212.1-994.6
  • 17. Body Wave Velocity Structure 1.What is the P wave velocity in this area (km/s)? 2. What is the origin time of the earthquake (using only graph 1) ? Plot your P wave arrival time data on the first graph and plot your S wave arrival time data on the second graph. 3. What is the S wave velocity in this area (km/s)? 4. What is the origin time of the earthquake (using only graph 2) ? 5. Are the two origin times equal ? Why or why not? P-wave Data S-wave Data
  • 18. What is the P wave velocity in this area (km/s)? 5.51km/s What is the origin time of the earthquake (using only graph 1)? ? 27.41/ 5.51 = 4.97, so answer is 10:33:0.4.97 What is the S wave velocity in this area (km/s)? 3.26 km/s What is the origin time of the earthquake (using only graph 2) ? 16.23/3.26 = 4.97, so answer is 10:33:0.4.97 Are the two origin times equal ? Why or why not? The origin times are equal, but only because I did the problem mathematically. If you did the problem graphically you can expect to get slightly different answers. Y= Distance in km X= Time in sec. P-wave Data S-wave Data

Editor's Notes

  1. This low An important seismic discontinuity occurs as a low-velocity zone in the Upper Mantle velocity zone is called the Asthenosphere It is not sharp but stretches from a depth of about 100km to 250 km below the surface Both P- and S-wave velocities are sharply reduced within the Asthenosphere Thought to be partly molten (1-10% liquid) which accounts for its low velocities and make it very weak Most basalt magmas have their origin in the asthenosphere
  2. Fig. 3.5- 6 of Stein 2003 Rial, 1978: Volume 55 Issue 3 Page 737-743 , December 1978 Summary. This note reports on the remarkable focusing of seismic body waves at or near the antipode (Δ = 180°) of an earthquake's epicentre. The particular seismic velocity structure and sphericity of the Earth cause body-wave phases such as P (diff), PKP, PP, PPP, PcPPKP, SKSSKS, SS , etc. to converge individually at antipodal distances after being diffracted, reflected or refracted at discontinuities. This focusing strongly amplifies each signal up to almost one order of magnitude with respect to the normal phase recorded two or more degrees away. Since the signal/noise ratio is enhanced in the same proportion, seismograms at antipodal distances provide clear and strong arrivals of otherwise weak phases. Antipodal monitoring of seismic waves is suggested as a powerful means of exploring the Earth's interior. The study of these ‘seismic images’ generated at focal points of seismic rays will yield information on the departures from lateral homogeneity and sphericity of the core, as well as stronger constraints on earth models. To interpret the observations correctly, the data must be compared with theoretically generated seismograms . Since the appropriate ray theory equations (see, e.g. Scholte; Gilbert & Helmberger; Richards) are singular at Δ =180°, a corrective measure is taken which provides a formal expression for the wave amplitude that remains finite at the antipode, and reproduces the usual expressions at other distances.
  3. Figure 3.5.11 of Stein, pp. 169: It shows that seismograms recorded at PTO (Porto, Portugal) and (Malaga, Spain) from earthquake in New Zealand . Phases like PP and PKP are focused at the antipode, because paths in any direction from the source arrive at the same time. Note the larger arrivals at PTO, only 0.7 degree from the antipode. Rial, J. A. ; Cormier, V. F. (1980, JGR): The antipodal region (178°?Δ?180°) of a seismic wave source is investigated in detail and shown to provide a new set of remarkable data to use in the exploration of the earth's interior . Body and surface waves converge individually at antipodal distances after having sampled laterally the totality of the planet. The waves are focused and strongly amplified up to 1 order of magnitude with respect to the normal phase recorded 2° or more away. The delicate interference patterns thus formed yield information on departures from lateral homogeneity and sphericity of the core and mantle, the structure of the inner core, global dissipation characteristics of the upper mantle, and provide strong constraints on earth models. Seismograms have been synthesized that closely reproduce the phases P diff , PKIKP, PKIIKP, PKP(BC), PKP, and PP observed at World-Wide Standard Seismographic Network long-period instruments located within 5° from the antipode of the New Zealand Inangahua earthquake of May 23, 1968. Preliminary results indicate that the lower mantle and upper core are laterally homogeneous as seen by 15-s waves, but the core-mantle boundary region is probably laterally inhomogeneous. The inner core-outer core boundary appears to be a sharp transition with a P wave velocity jump of the order of 0.8 km/s. The resolution of the long-period data is poor, but the potential richness of the method when better data sets are available strongly motivated the investigation. Suggested future lines of research using antipodal observations include monitoring of inner core phases
  4. Allen Jones http://bingweb.binghamton.edu/~ajones/
  5. Ring of Fire strikes Peru A magnitude-8.1 earthquake at 33 kilometers deep shook Peru on Saturday, June 23,  says the USGSs National Earthquake Information Center, upping previous estimates that put the quake's magnitude at 7.9. The focus was just off the Peruvian coast, about 120 miles west of Arequipa, Peru's second largest city. Three major aftershocks followed ranging from magnitude 5.5 to 6.3.   Debris and collapsed homes killed at least 70 people, most in Arequipa, and over 30 people are missing from Camana, a nearby coastal town deluged by a quake-induced tsunami. A landslide blocked the main road into Moquegua, 60 miles from Arequipa, keeping emergency food and medicine from a town where 17 people were killed and 80 percent of the houses seriously damaged or flattened. Stretched out against an active continental margin, Peru is no stranger to big quakes. The most memorable was the devastating magnitude-7.7 event in 1970 that killed approximately 70,000 people during an avalanche of rock and snow on Mount Huascarán, a little over 200 miles north of Lima.
  6. Expected Arrival Times: AKI135 Model
  7. P-waves half way to core
  8. Incidence: Ray path in a medium with velocity increasing smoothly with depth. The ray parameter is constant along the ray path, so the angle of incidence changes as the velocity changes. The angle of incidence is smallest at the surface, where velocity is lowest, and is 90 at the bottoming depth.
  9. Y= Distance in km X= Time in sec.