Geology 5660/6660 Applied Geophysics 26 Feb 2014 © A.R. Lowry 2014 For Fri 28 Feb: Burger 524-548 (§8.4–8.5) Last Time: Industry Seismic Interpretation.

Slides:



Advertisements
Similar presentations
Electromagnetic Waves in Conducting medium
Advertisements

The Asymptotic Ray Theory
Prof. Ji Chen Notes 15 Plane Waves ECE Spring 2014 z x E ocean.
Lecture 8: Reflection and Transmission of Waves
PH0101 UNIT 2 LECTURE 31 PH0101 Unit 2 Lecture 3  Maxwell’s equations in free space  Plane electromagnetic wave equation  Characteristic impedance 
EEE 498/598 Overview of Electrical Engineering
Ground Penetrating Radar (GPR) GPR technology can be used to determine depth to bedrock and or water table, locate buried ordinance at gunnery ranges,
Millimeter Wave Sensor: An Overview
electromagnetic method
I. Basic Techniques in Structural Geology
Naval Weapons Systems Energy Fundamentals Learning Objectives  Comprehend basic communication theory, electromagnetic (EM) wave theory  Comprehend.
Electromagnetic Wave Theory
Reflection and Refraction of Plane Waves
1 Optical Properties of Materials … reflection … refraction (Snell’s law) … index of refraction Index of refraction Absorption.
Ultrasound Physics Sound is a mechanical, longitudinal wave that travels in a straight line Sound requires a medium through which to travel Ultrasound.
Basic Geologic and Hydrogeologic Investigations
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
GEOL 3000 With Assistance from Nigel Wattrus.  Seismic Reflection  Seismic Reflection – subhorizontal geologic structures  Siesmic Refraction  Siesmic.
Time variation Combining electrostatics and magnetostatics: (1) .E =  /  o where  =  f +  b (2) .B = 0“no magnetic monopoles” (3)  x E = 0 “conservative”
Geology 5660/6660 Applied Geophysics 17 Jan 2014 © A.R. Lowry 2014 Read for Wed 22 Jan: Burger (Ch 2.2–2.6) Last time: The Wave Equation; The Seismometer.
Seismic reflection Ali K. Abdel-Fattah Geology Dept.,
Geology 5660/6660 Applied Geophysics This Week: No new lab assignment… But we’ll go over the previous labs 06 Feb 2014 © A.R. Lowry 2014 For Fri 07 Feb:
ECEN5341/4341Bioelectromagnetics Spring 2015 Frank S. Barnes Contact Info: (303) ECOT 250
Geology 5660/6660 Applied Geophysics 24 Feb 2014 © A.R. Lowry 2014 For Wed 26 Feb: Burger (§8.4) Last Time: Industry Seismic Interpretation Well.
Geology 5660/6660 Applied Geophysics 18 Feb 2014 © A.R. Lowry 2014 For Wed 20 Feb: Burger (§ ) Last Time: Reflection Data Processing Step.
Last Time: Ground Penetrating Radar Radar reflections image variations in Dielectric constant  r ( = relative permittivity )  3-40 for most Earth materials;
SOES6002: Modelling in Environmental and Earth System Science CSEM Lecture 1 Martin Sinha School of Ocean & Earth Science University of Southampton.
Geology 5660/6660 Applied Geophysics 19 Feb 2014 © A.R. Lowry 2014 For Fri 21 Feb: Burger (§ ) Last Time: Reflection Data Processing Step.
Prof. D. R. Wilton Notes 18 Reflection and Transmission of Plane Waves Reflection and Transmission of Plane Waves ECE 3317 [Chapter 4]
ECE 3317 Prof. David R. Jackson Notes 15 Plane Waves [Chapter 3]
Electromagnetic Waves and Their Propagation Through the Atmosphere
Physical Properties of Permafrost: The Impact of Ice in the Ground to Geophysical Surveys Brian Moorman Department of Geology and Geophysics and.
Geology 5660/6660 Applied Geophysics 28 Feb 2014 © A.R. Lowry 2014 Last Time: Ground Penetrating Radar (GPR) Radar = electromagnetic radiation (light)
So far, we have considered plane waves in an infinite homogeneous medium. A natural question would arise: what happens if a plane wave hits some object?
Lale T. Ergene Fields and Waves Lesson 5.5 Wave Reflection and Transmission.
Introduction to Seismology
Designing a Ground Penetrating Radar Experiment You need to determine: 1.Amount of time to record the signal 2.Antenna frequency 3.Line spacing While thinking.
Geology 5660/6660 Applied Geophysics Last time: Overview of Applied Geophysics Important syllabus points: Labs, projects, 5-vs-6660, text Geophysics: What.
Geology 5660/6660 Applied Geophysics 27 Jan 2016 © A.R. Lowry 2016 Read for Fri 29 Jan: Burger (Ch 3-3.2) Last time: Seismic Amplitude depends on.
Geology 5660/6660 Applied Geophysics 20 Jan 2016
Geology 5660/6660 Applied Geophysics 22 Jan 2016 © A.R. Lowry 2016 For Mon 25 Jan: Burger (Ch 2.2.2–2.6) Last time: The Seismometer A seismometer.
Shot-profile migration of GPR data Jeff Shragge, James Irving, and Brad Artman Geophysics Department Stanford University.
Geology 5660/6660 Applied Geophysics Last time: The Refraction Method Cont’d Multiple Horizontal Layers: Using Snell’s law, generalizes simply to: Dipping.
Geology 5660/6660 Applied Geophysics 29 Feb 2016 © A.R. Lowry 2016 Last Time: Ground Penetrating Radar (GPR) Radar = electromagnetic radiation (light)
Geology 5660/6660 Applied Geophysics 20 Apr 2016
GROUND PENETRATING RADAR
1 Introduction to Applied Geophysics & Geophysical Exploration Prof Jeannot Trampert (coordinator) Dr Fred Beekman
Geology 5660/6660 Applied Geophysics 23 Feb 2016 Lab 3 © A.R. Lowry 2016 Seismic Reflections Next assignment due one week from now Due noon Mar 1.
5. Electromagnetic Optics. 5.1 ELECTROMAGNETIC THEORY OF LIGHT for the 6 components Maxwell Eq. onde Maxwell.
Geology 5660/6660 Applied Geophysics 12 Feb 2016
Geology 5660/6660 Applied Geophysics 24 Feb 2016 © A.R. Lowry 2016 For Fri 26 Feb: Burger (§8.4) Last Time: Industry Seismic Interpretation Well.
Geology 5660/6660 Applied Geophysics 26 Feb 2016 © A.R. Lowry 2016 For Mon 29 Feb: Burger (§8.4) Last Time: Industry Seismic Interpretation Seismic.
Geology 5660/6660 Applied Geophysics 18 Apr 2016 © A.R. Lowry 2016 Last Time: Magnetotellurics (MT) Some (minor but growing) applications in oil & mining;
Geology 5660/6660 Applied Geophysics 10 Feb 2016 © A.R. Lowry 2016 Last Time: Seismic Reflection Travel-Time Cont’d Dix Equations for multiple layers:
Geology 5660/6660 Applied Geophysics 04 Apr 2016
Geology 5660/6660 Applied Geophysics 5 Feb 2016
UPB / ETTI O.DROSU Electrical Engineering 2
GPR Simulations for pipeline oil drainage
Ground-Penetrating Radar
ECEN5341/4341 Spring 2017 Lecture 2 January 20,2017.
Geology 5660/6660 Applied Geophysics 15 Mar 2016 Lab 5 GPR
Ground Penetrating Radar using Electromagnetic Models
Technologies to model Ground water
PLANE WAVE PROPAGATION
ENE 325 Electromagnetic Fields and Waves
The radar band is loosely taken to extend from approximately 0
Wireless Communications Chapter 4
ECEN5341/4341 Spring 2019 Lecture 2 January 16,2019.
Ground-Penetrating Radar
Antenna Theory Chapter.4.7.4~4.8.1 Antennas
Presentation transcript:

Geology 5660/6660 Applied Geophysics 26 Feb 2014 © A.R. Lowry 2014 For Fri 28 Feb: Burger (§8.4–8.5) Last Time: Industry Seismic Interpretation 4D seismic: Multiple 3D reflection images over time aid in optimization of reservoir production Salt structures are especially challenging but have been a focus of innovation EM imaging is a tool of growing importance; electrical resistivity is sensitive to fluids and clay content Knowledge of geological processes key to interpretation!!!! BUT, it’s critically important to also recognize artefacts/processing limitations of the seismic reflection data.

Note: If you see something like this: … Your ppt font interpreter is missing something that’s in my equation editor. (Feel free to ask Xiaofei or I about it.)

Ground Penetrating Radar: Radar  electromagnetic waves (light) at radio frequencies (50 to 1000 MHz). Governed by physics of the wave equation (so in some respects it is very similar to seismic methods: V = f !) Requires a source and receiver ( dipole antennae for both) Source transmits a single pulse: but can transmit and receive millions of pulses per second! 0 5x10 -9 s Amplitude time Power frequency 10 Mhz

Display is very much like seismic: Amplitude (voltage) versus time on a “trace”. Source-receiver is usually near zero-offset (but can use NMO profiling, CMP gathers) High frequency  requires high sampling rate, very precise electronics. Lots more source/receiver obs  denser spatial sampling Higher frequency  higher resolution High attenuation  very shallow (< a few 10s of m)

Like seismic, waves are reflected & transmitted at interfaces with differing impedance properties: layer 1 layer 2 E0E0 E1E1 E2E2 Snell’s law applies. Amplitude dependence is somewhat different because there is only one type of wave. Reflection R & Transmission T coefficients are identical to seismic (for 90° angle of incidence): where Z i is the electromagnetic impedance in layer i.

Recall for seismic: Acoustic Impedance Z i =  i V i For Electromagnetic Impedance, where:  = frequency  = dielectric permittivity  = relative magnetic permeability  = electrical resistivity  = 1/  = electrical conductivity  r is called the dielectric constant (or “relative permittivity”): a complex variable. All of these parameters (except frequency  ) are physical properties of the medium, so like impedance & velocity in seismic studies, these contain information about the targeted volume!

Most modern radar sections are converted from two-way travel-time to depth using an assumed value for velocity… Important to note that

Soil and Rock Properties: Relative Magnetic Permeability  ~ 1 for most rocks; 1.05 for hematite 5 for magnetite Dielectric Constant  r (= relative permittivity) (real part): (dry) (wet) (defined as: ) magnetic flux density magnetic field intensity 430 soil 330 sand 512sandstone 740 clay water8088 (fresh) (brine) 48limestone 515shale

For most applications (i.e., near-surface)  1 ≈  2 ≈ 1 ;  (10 -4 –10 -1 ) «  (10 6 –10 10 !), and hence (i.e., we are imaging velocity variations corresponding to changes in dielectric constant!) For the water table, R ~ 0.1 Recall seismic waves attenuate as where Q is quality factor; Radar waves attenuate similarly as ; where Attenuation is extremely high for shale, silt, clay, and briny water (which is why GPR rarely penetrates > 10 m!). 