EOSC 454 Lab #3. 3D Magnetics. Date: Feb 3, Due: Feb 10, 2009.
|
|
- Adele Gibbs
- 5 years ago
- Views:
Transcription
1 EOSC 454 Lab #3 3D Magnetics Date: Feb 3, Due: Feb 10, Introduction In this exercise you will perform both forward models and inversions of magnetic data. You will compare the response of a dipole with that of a small susceptible prism. You will be using Meshtools as well as the UBC-GIF Magnetic Dipole Applet, which is located at: First experiment with the different parameters to get a feel for how the applet is used. Use the following options when using the applet for this tutorial: magnetic moment of 100 Am 2, inclination of 0, declination of 0, data spacing of 1 and a length of 25. The applet places a at dipole a specified depth below the surface and calculates the response at an elevation of 1m above the surface. Use the B t component for comparison with Meshtools. Note: Data in the applet is calculated at an elevation of 1m above the surface of the Earth. Meshtools Setup: Using Meshtools, create a mesh with the following properties: top south-west corner (-11, -11,0), (dx,dy) of (1,1) and length of (22,22). This will create cells of dimension (1, 1, 0.5). When performing forward model, use field strength of 40,000nT, inclination and declination of (0,0) and take the survey at a constant elevation of 1.0m above the mesh surface. You will need to use a data spacing of (2,2) to ensure that you do not generate more than 200 data points. Also, use a data area of x0 = -11.5, xn = 11.5, y0 = -11.5, yn = 11.5 to compute the data in the magnetics forward modelling dialog box. This ensures that you have a data point directly above the center of the mesh. 1
2 Questions: 1. Determine the susceptibility κ that will give rise to a magnetic moment of 100 Am 2 for a 1mx1mx1m prism. 2. Using Meshtools, create a 1mx1mx1m prism with at or near the center of the mesh. Use a value of susceptibility you just calculated. Place the center of the prism at a depth below the surface such that the top is at z=-5.5m and the bottom is at z=-6.5m (the center of the prism is now at z=-6m). Calculate the response at an elevation of 1m above the surface. What are the maximum and minimum values of the data? 3. Using the applet, generate the data from a dipole with a magnetic moment of 100 Am 2 at a depth of 6m below the surface. Compare this result with the response generated from the susceptible prism. Does a dipole appear to be a good approximation for a small prism at this distance from the observation point? Make your comparison by comparing the maximum and minimum values and the shape of the anomaly by generating profiles along the surface. 4. Calculate the max/min values of the response for both the prism and the dipole. Evaluate how well the dipole does in estimating the response of a prism by calculating the forward model at a variety of heights. Use an elevation above the surface of the mesh of 1-12 meters with 1 meter increments. (Note the dipole applet is distance to dipole, not height above the surface, and measurements in the dipole are 1m above the surface). Plot the difference between the max values computed using mag3d and with the dipole applet using d prism d dipole d prism (1) where d prism and d dipole are the maximum values computed at a particular elevation using meshtools, and the dipole applet. Using the maximum response at each depth as the data. At what depth does the dipole fail to be a good approximation to the prism? Support your findings with sketches of the profiles over the targets. Printed images of the results are optional. 2 Applet Questions To determine whether a magnetic survey might detect a buried object it is important to estimate the amplitude of the expected magnetic anomaly. Instruments may be accurate to about 1nT but other factors, like inaccurate removal of the time varying fields, geologic noise, etc. may require that the magnetic amplitude from the anomalous body is significantly larger than the 1nT threshold. 2
3 We will now carry out an analysis of a dipole buried at Vancouver. The first step is to determine the strength and geometry of the inducing field at Vancouver. Using the website: Determine the parameters for the inducing field at Vancouver. Use coordinates of 49 o N, 123 o W, altitude of 200m and today s date. From the output, obtain the inclination declination and field strength at Vancouver. 1. What are the Earth s magnetic field inclination, declination and total strength for Feb 3, 2009 at Vancouver? 2. Consider a partly rusted iron sphere that has a diameter of 60 cm and an effective susceptibility κ = 3 and is buried at a local site in Vancouver. What is the magnetic moment of this sphere when buried at Vancouver? 3. Plot a graph of the maximum value of the magnetic anomaly when the sphere is buried within the range 1-30 meters beneath the surface? To evaluate the amplitudes, use the Magnetic Dipole Applet. Plot amplitude on the vertical axis and the horizontal axis should be depth below the sensor. (Remember the receiver in the Applet demo is at a height of 1 m above the earth s surface. ) 4. Assuming a 1nT noise estimate, what is the maximum depth of burial of the sphere so that it can still be detected with the magnetic survey? 5. Plot a graph of the half-width of the anomaly as a function of depth of burial. Again, make the horizontal axis the depth of the dipole below the sensor. A magnetic survey was conducted directly over the body (that s fortunate!) and along a direction of N22E. The half-width of the curve was found to be 8 meters. Use the graph you constructed to estimate how deep you need to trench before you hit the buried sphere. 6. Suppose you know that the sphere lies between 4-8 meters depth. What should your line spacing and data spacing be? How do you arrive at your answer? 7. It is not only the peak amplitude of the anomaly which is important but also the shape of the anomalous field. By the time we have finished magnetics I want you to be able to visualize magnetic fields that would result from simple buried objects and then to be able to sketch the individual components of the field in the x- or z- directions or that component in the direction of the earth s field. The latter is the total field anomaly as measured with a proton precession magnetometer. To provide practise, consider the following: When a small spherically shaped object is placed in a magnetic field it produces a magnetic field like that due to a dipole which is orientated in the direction of the inducing field. Establish a coordinate system with x positive in the north magnetic direction, y positive east, and z positive down. The relationship between inclination of the earth s field and latitude is given by tan(i) = 2/tan(θ) 3
4 Sketch B z, along a traverse in the x direction at y = 0. but with latitudes 90 o, 45 o, 0 o. Sketch B T, along a traverse in the x direction at y=0. but with latitudes 90 o, 45 o, 0 o. Of course you can simply use the Applet profile tool and so everybody should get the right answer. That is why there won t be many marks for this question. However, the learning portion of this problem arises when you try to make your sketches before you view the answer. To make your sketches it is easiest to begin with the fields from a dipole (use one of the pictures handed out in class) and draw a straight line through the fields which represents the observation plane. Then make your inferences about sign and magnitude of the field components to complete your sketch. Check to see that you agree with the profiles provided in the Applet demo. 3 Synthetic inversion of magnetic data You will now explore the 3D magnetics inversion code through a synthetic example. 1. Using MeshTools3D create a mesh for the San Nicolas region, using the following parameters: (dx,dy) = (150,150), (length x,length y) = (3450,3450), top south-west corner = (-3400,-1800,0) 2. Create a prism to approximate the sulphide deposit of San Nicolas. Use parameters of 0.01 SI susceptibility with the following geometry: x = (-1750,-1450), y = (-300,0), z = (-225,-375). 3. Forward model the magnetics response of this prism. On the dialogue window, use parameters of Date area (x0 = -2575, xn = -525, y0 = -975, yn = 825) and Data spacing (X = 140, Y = 140). Using a constant height of 1 meter. The inclination at San Nicolas is degrees, declination is degrees and field strength of 44,000 nt. 4. What are the minimum and maximum values of the computed magnetic field 5. Assign a standard deviation of 5% with a floor or 0.8. Save this data file. 6. Load the data file into the mag3d-gui. Set the wavelet compression to none and invert the synthetic magnetic data. 7. What is the size of the recovered anomaly? What is the maximum and minimum recovered susceptibilities? 4
5 4 Inversion of San Nicolas Magnetic Data The magnetics data have been provided to you in the SN mag.dat and these data have already had the regional field removed. Load the data file into the Magnetics inversion GUI. View the data. Assign a standard deviation of 5% plus a floor of 2. Click the create-mesh button. Use a cell size of 50 and an elevation of 0. Disable wavelet compression, save the.inp file, and run the inversion. View the inversion log and view the predicted data. Does the inversion converge to the desired misfit? Does the misfit map show any correlations? After viewing the inversion model, it appears that the default mesh for this model is not deep enough. Open the mesh file in note, and add 5 more 25 meter cells to the z-line of the file, note you will need to increase the number of z cells on the first line of the file. Re-invert the San Nicolas magnetics data using this new mesh. What is the maximum susceptibility in the recovered model? What are the dimensions of the anomaly? 4.1 Discrimination of massive sulphide You now have two separate models of the San Nicolas deposit: a density model and a susceptibility model. You are going to delineate the San Nicholas deposit by isolating model cells which are both density and susceptible. Since the gravity and magnetics models are on two different meshes, the first step is to interpolate the magnetics model onto the gravity. A matlab utility is provided to perform the interpolation. Run the util remesh.m Matlab file. The, select the magnetics mesh, then select the gravity inversion mesh. Then select the magnetic inversion model maginv3d.sus. Select an output file to output the magnetics model now using the gravity inversion mesh. Using Matlab s importdata command, load both the density and susceptibility models, i.e. rho = importdata( gzinv3d.den ); sus = importdata( maginv3d.sus ); 5
6 Write a matlab script that generates a model file that contains 1 for each cell that is both susceptible and dense, and 0 otherwise. You will need to view the gravity and susceptible models to estimate cutoff values. You can use the Matlab command save to output the model save( output_filename, model_variable, -ascii ); where output filename is the filename that will be output, model variable is the Matlab variable containing your San Nicolas model containing 0 or 1. View your San Nicolas deposit estimate in MeshTools. What cut-off values did you select for the density and susceptibility? What are the dimensions of your estimated San Nicolas model? How does your estimated deposit model compare to the estimated San Nicolas cross-section provided in lab 1? Contact Elliot Holtham at eholtham@eos.ubc.ca, or drop by Room 332 in the Geophysics building for help regarding the exercises. 6
Question: What are the origins of the forces of magnetism (how are they produced/ generated)?
This is an additional material to the one in the internet and may help you to develop interest with the method. You should try to integrate some of the discussions here while you are trying to answer the
More informationGeophysics 224 B2. Gravity anomalies of some simple shapes. B2.1 Buried sphere
Geophysics 4 B. Gravity anomalies of some simple shapes B.1 Buried sphere Gravity measurements are made on a surface profile across a buried sphere. The sphere has an excess mass M S and the centre is
More informationHow Deep Can My Magnetometer See?
A common question when using magnetometers or gradiometers is, How deep is my instrumentation seeing? This Magnetic Moment provides some answers to this question while emphasizing quick analysis methods
More information3D modeling of the Quest Projects Geophysical Datasets. Nigel Phillips
3D modeling of the Quest Projects Geophysical Datasets Nigel Phillips Advanced Geophysical Interpretation Centre Undercover Exploration workshop KEG-25 April 2012 Mineral Physical Properties: density sus.
More informationSite map 1 of 1. Complete 3D mag/grav workflow outline. 1. Setting up for inversion. 1. Introduction
Site map 1 of 1 Complete 3D mag/grav workflow outline 0. Introduction Goals Using the workflow Best practice 4. Relevant assumptions 5. Codes needed 6. Examples Setting up for inversion Clarify the problem
More informationGravity Methods (VII) wrap up
Environmental and Exploration Geophysics II Gravity Methods (VII) wrap up tom.h.wilson tom.wilson@mail.wvu.edu Department of Geology and Geography West Virginia University Morgantown, WV Items on the list
More informationMVI Documentation. Release 2.0 UBC-GIF
MVI Documentation Release 2.0 UBC-GIF Sep 01, 2017 Contents 1 Elements of the program MVIINV 3 1.1 Introduction............................................... 3 1.2 General files for MVI programs.....................................
More informationQUEST Project: 3D inversion modelling, integration, and visualization of airborne gravity, magnetic, and electromagnetic data, BC, Canada.
Mira Geoscience Limited 409 Granville Street, Suite 512 B Vancouver, BC Canada V6C 1T2 Tel: (778) 329-0430 Fax: (778) 329-0668 info@mirageoscience.com www.mirageoscience.com QUEST Project: 3D inversion
More informationGRAPRISM. Version Markku Pirttijärvi
GRAPRISM Version 1.1 2003 Markku Pirttijärvi Introduction: Gravity, the attraction force between masses, is one of the basic forces of the physical world. The objective of geophysical gravity method is
More informationMagnetics. Introduction to Filtering using the Fourier Transform. Chuck Connor, Laura Connor. Potential Fields. Magnetics.
Introduction to using the Chuck Connor, Laura Connor Potential Fields for this week Nm Sm Schematic Earth dipolar magnetic field. The field lines placed in the page plane are drawn as thick lines, those
More informationThree-dimensional inversion of borehole, time-domain, electromagnetic data for highly conductive ore-bodies.
Three-dimensional inversion of borehole, time-domain, electromagnetic data for highly conductive ore-bodies. Nigel Phillips, Doug Oldenburg, Eldad Haber, Roman Shekhtman. UBC-Geophysical Inversion Facility
More informationMAGPRISM. Version Markku Pirttijärvi
MAGPRISM Version 1.1 2003 Markku Pirttijärvi Introduction: The objective of geophysical magnetic field method is to obtain indirect information about the subsurface structures from the measurements made
More informationAdaptive and Iterative Processing Techniques for Overlapping Signatures
VA-118-001-06-TR Adaptive and Iterative Processing Techniques for Overlapping Signatures Technical Summary Report March 2006 PERFORMING ORGANIZATION AETC Incorporated 1225 South Clark Street, Suite 800
More informationOasis montaj Best Practice Guide. VOXI Earth Modelling - Building Geologic Models with NODDY
Oasis montaj Best Practice Guide VOXI Earth Modelling - The software described in this manual is furnished under license and may only be used or copied in accordance with the terms of the license. Manual
More informationAdding Magnetic Data to a GM-SYS Profile Model
Adding Magnetic Data to a GM-SYS Profile Model In GM-SYS Profile, a "Station" is a location at which an anomaly component is calculated and, optionally, was measured. In order for GM-SYS Profile to calculate
More informationH3DTD MUMPS. A Program Library for Forward Modelling of Multi-Transmitter, Time-Domain Electromagnetic Data over 3D structures.
H3DTD MUMPS A Program Library for Forward Modelling of Multi-Transmitter, Time-Domain Electromagnetic Data over 3D structures. Version 1.6 Developed under the MITEM consortium Research Project Multi-Source
More informationIntroduction to Geophysical Inversion
Introduction to Geophysical Inversion Goals Understand the non-uniqueness in geophysical interpretations Understand the concepts of inversion. Basic workflow for solving inversion problems. Some important
More information2D Inversions of 3D Marine CSEM Data Hung-Wen Tseng*, Lucy MacGregor, and Rolf V. Ackermann, Rock Solid Images, Inc.
2D Inversions of 3D Marine CSEM Data Hung-Wen Tseng*, Lucy MacGregor, and Rolf V. Ackermann, Rock Solid Images, Inc. Summary A combination of 3D forward simulations and 2D and 3D inversions have been used
More information26257 Nonlinear Inverse Modeling of Magnetic Anomalies due to Thin Sheets and Cylinders Using Occam s Method
26257 Nonlinear Inverse Modeling of Anomalies due to Thin Sheets and Cylinders Using Occam s Method R. Ghanati* (University of Tehran, Insitute of Geophysics), H.A. Ghari (University of Tehran, Insitute
More informationElectromagnetic migration of marine CSEM data in areas with rough bathymetry Michael S. Zhdanov and Martin Čuma*, University of Utah
Electromagnetic migration of marine CSEM data in areas with rough bathymetry Michael S. Zhdanov and Martin Čuma*, University of Utah Summary In this paper we present a new approach to the interpretation
More informationLab 21.1 The Tangent Galvanometer
Name School Date Lab 21.1 The Tangent Galvanometer Purpose To investigate the magnetic field at the center of a current-carrying loop of wire. To verify the right-hand rule for the field inside a current
More informationCOMBINING MULTIPLE GEOPHYSICAL DATA SETS INTO A SINGLE 3D IMAGE. Abstract
COMBINING MULTIPLE GEOPHYSICAL DATA SETS INTO A SINGLE 3D IMAGE Jeffrey J. Daniels*, Mark Vendl+, Jennifer Holt*, and Erich Guy* *OSU, Columbus, OH +USEPA, Chicago, IL Abstract Traditional geophysical
More informationApplication of wavelet theory to the analysis of gravity data. P. Hornby, F. Boschetti* and F. Horowitz, Division of Exploration and Mining, CSIRO,
Application of wavelet theory to the analysis of gravity data. P. Hornby, F. Boschetti* and F. Horowitz, Division of Exploration and Mining, CSIRO, Australia. Summary. The fundamental equations of potential
More informationThree-Dimensional Laser Scanner. Field Evaluation Specifications
Stanford University June 27, 2004 Stanford Linear Accelerator Center P.O. Box 20450 Stanford, California 94309, USA Three-Dimensional Laser Scanner Field Evaluation Specifications Metrology Department
More informationThe interpolation of a 3-D data set by a pair of 2-D filters
Stanford Exploration Project, Report 84, May 9, 2001, pages 1 275 The interpolation of a 3-D data set by a pair of 2-D filters Matthias Schwab and Jon F. Claerbout 1 ABSTRACT Seismic 3-D field data is
More informationThe simulation requires several input parameters that may be categorized as following:
User Manual Author and Developer: Pavlos Paschalis National and Kapodistrian University of Athens Physics Department Cosmic Ray Station Principal Investigator Prof. Helen Mavromichalaki 2016 1. Versioning
More informationREPORT ON A 3D INDUCED POLARISATION SURVEY OVER THE HOMEEP AND SHIRLEY TRENDS, CONCORDIA DISTRICT, NORTHERN CAPE
GEOSPEC INSTRUMENTS (PTY) LTD REPORT ON A 3D INDUCED POLARISATION SURVEY OVER THE HOMEEP AND SHIRLEY TRENDS, CONCORDIA DISTRICT, NORTHERN CAPE PREPARED FOR MINXCOM (Pty) Ltd and Galileo Resources PLC BY
More informationOasis montaj How-To Guide. VOXI Earth Modelling - Running an Inversion Using Gradient Weighting
Oasis montaj How-To Guide VOXI Earth Modelling - Running an Inversion Using Gradient Weighting The software described in this manual is furnished under license and may only be used or copied in accordance
More informationRegional 3D inversion modelling of airborne gravity, magnetic, and electromagnetic data, Central BC, Canada.
Mira Geoscience Limited 409 Granville Street, Suite 512 B Vancouver, BC Canada V6C 1T2 Tel: (778) 329-0430 Fax: (778) 329-0668 info@mirageoscience.com www.mirageoscience.com Regional 3D inversion modelling
More informationQualitative Depth Estimation by Differencing Upward Continuations
Qualitative Depth Estimation by Differencing Upward Continuations Jacobsen (1987) made a strong case for using upward continuation filtering as a method for separating causative sources from various depths.
More informationEfficient 3D Gravity and Magnetic Modeling
Efficient 3D Gravity and Magnetic Modeling X. Li Fugro Gravity & Magnetic Services Inc., Houston, Texas, USA Summary There are many different spatial-domain algorithms for 3D gravity and magnetic forward
More informationInversion concepts: Introducing geophysical inversion
Inversion concepts: Introducing geophysical inversion This chapter deals with basic concepts underlying geophysical inversion. Four sections provide an overview of essential ideas without mentioning mathematical
More informationThis presentation focuses on 2D tactile roughness measurements. Three key points of the presentation are: 1. Profiles are simply a collection of
1 This presentation focuses on 2D tactile roughness measurements. Three key points of the presentation are: 1. Profiles are simply a collection of relative heights. 2. Parameters are statistics, not dimensions.
More informationExploring IX1D The Terrain Conductivity/Resistivity Modeling Software
Exploring IX1D The Terrain Conductivity/Resistivity Modeling Software You can bring a shortcut to the modeling program IX1D onto your desktop by right-clicking the program in your start > all programs
More informationIntroduction to Geophysical Modelling and Inversion
Introduction to Geophysical Modelling and Inversion James Reid GEOPHYSICAL INVERSION FOR MINERAL EXPLORERS ASEG-WA, SEPTEMBER 2014 @ 2014 Mira Geoscience Ltd. Forward modelling vs. inversion Forward Modelling:
More informationOasis montaj How-To Guide. VOXI Earth Modelling - Running an AGG Unconstrained Inversion
Oasis montaj How-To Guide VOXI Earth Modelling - Running an AGG Unconstrained Inversion The software described in this manual is furnished under license and may only be used or copied in accordance with
More informationUXO DISCRIMINATION USING TIME DOMAIN ELECTROMAGNETIC INDUCTION
UXO DISCRIMINATION USING TIME DOMAIN ELECTROMAGNETIC INDUCTION Introduction Leonard R. Pasion, Stephen D. Billings, and Douglas W. Oldenburg UBC - Geophysical Inversion Facility Department of Earth and
More informationDCIP3D OCTREE. Version 1.0
DCIP3D OCTREE A Program Library for Forward Modelling and Inversion of DC/IP data over 3D Structures using Octree meshes Version 10 Developed under the consortium research project: COOPERATIVE INVERSION
More informationUNIVERSITI MALAYSIA SARAWAK FACULTY OF ENGINEERING CIVIL ENGINEERING DEPARTMENT
UNIVERSITI MALAYSIA SARAWAK FACULTY OF ENGINEERING CIVIL ENGINEERING DEPARTMENT KNS 1461 CIVIL ENGINEERING LABORATORY 2 LABORATORY MANUAL (Edited : December 2008) CIVIL ENGINEERING LABORATORY 2 KNS 1461
More informationExercise 16: Magnetostatics
Exercise 16: Magnetostatics Magnetostatics is part of the huge field of electrodynamics, founding on the well-known Maxwell-equations. Time-dependent terms are completely neglected in the computation of
More informationGRAV3D Version 3.0. A Program Library for Forward Modelling and Inversion of Gravity Data over 3D Structures.
GRAV3D Version 3.0 A Program Library for Forward Modelling and Inversion of Gravity Data over 3D Structures. UBC-Geophysical Inversion Facility Department of Earth and Ocean Sciences University of British
More informationGEOPHYS 242: Near Surface Geophysical Imaging. Class 8: Joint Geophysical Inversions Wed, April 20, 2011
GEOPHYS 4: Near Surface Geophysical Imaging Class 8: Joint Geophysical Inversions Wed, April, 11 Invert multiple types of data residuals simultaneously Apply soft mutual constraints: empirical, physical,
More information(x, y, z) m 2. (x, y, z) ...] T. m 2. m = [m 1. m 3. Φ = r T V 1 r + λ 1. m T Wm. m T L T Lm + λ 2. m T Hm + λ 3. t(x, y, z) = m 1
Class 1: Joint Geophysical Inversions Wed, December 1, 29 Invert multiple types of data residuals simultaneously Apply soft mutual constraints: empirical, physical, statistical Deal with data in the same
More informationGeology and Calculus
GEOL 452 - Mathematical Tools in Geology Lab Assignment # 6 - Feb 25, 2010 (Due March 9, 2010) Name: Geology and Calculus A. Volume of San Nicolas Island San Nicolas Island is one of the remote and smaller
More informationPotent can model multi-component data, such as down-hole Fx, Fy, Fz magnetic data, or tensor gravity data.
Getting Started What is Potent? Main concepts A simple tutorial What is Potent? Potent is a program for modelling the magnetic and gravitational effects of subsurface structures. It provides a highly interactive
More informationOasis montaj How-To Guide. VOXI Earth Modelling - Running an Inversion
Oasis montaj How-To Guide VOXI Earth Modelling - Running an Inversion The software described in this manual is furnished under license and may only be used or copied in accordance with the terms of the
More informationWorkhorse ADCP Multi- Directional Wave Gauge Primer
Acoustic Doppler Solutions Workhorse ADCP Multi- Directional Wave Gauge Primer Brandon Strong October, 2000 Principles of ADCP Wave Measurement The basic principle behind wave the measurement, is that
More informationEMIGMA V9.x Premium Series
EMIGMA V9.x Premium Series EMIGMA BASIC January 2014 Firstly, EMIGMA Basic describes the tools that are available in every EMIGMA license. Secondly, EMIGMA Basic is the name we use for our free viewing
More informationDOWN PLUNGE CROSS SECTIONS
GG303 Lab 7 10/6/10 1 DOWN PLUNGE CROSS SECTIONS I Main Topics A Cylindrical folds B Downplunge cross-section views C Apparent dip II Cylindrical folds A Surface of a cylindrical fold is parallel to a
More informationSection Graphs of the Sine and Cosine Functions
Section 5. - Graphs of the Sine and Cosine Functions In this section, we will graph the basic sine function and the basic cosine function and then graph other sine and cosine functions using transformations.
More informationnewfasant US User Guide
newfasant US User Guide Software Version: 6.2.10 Date: April 15, 2018 Index 1. FILE MENU 2. EDIT MENU 3. VIEW MENU 4. GEOMETRY MENU 5. MATERIALS MENU 6. SIMULATION MENU 6.1. PARAMETERS 6.2. DOPPLER 7.
More informationGravity Gradients in PreStack Depth Migration
Index Table of contents Gravity Gradients in PreStack Depth Migration Ed. K. Biegert Shell International Exploration and Production Summary Subsurface de-risking is presently almost exclusively done by
More informationHomework Set 3 Due Thursday, 07/14
Homework Set 3 Due Thursday, 07/14 Problem 1 A room contains two parallel wall mirrors, on opposite walls 5 meters apart. The mirrors are 8 meters long. Suppose that one person stands in a doorway, in
More informationChapter 14 Mensuration Surface Area and Volume Conversion of one solid into another solid Some time we have to melt one solid and convert it to another shap. For example we have to convert a metallic sphere
More information3D Inversion of Time-Domain Electromagnetic Data for Ground Water Aquifers
3D Inversion of Time-Domain Electromagnetic Data for Ground Water Aquifers Elliot M. Holtham 1, Mike McMillan 1 and Eldad Haber 2 (1) Computational Geosciences Inc. (2) University of British Columbia Summary
More informationAdding a roof space over several zones.
Adding a roof space over several zones. Adding a roof space zone connecting to several rooms requires a sequence of actions from the user. There is no wizard for this. And it is possible to do this and
More informationActivity The Coordinate System and Descriptive Geometry
Activity 1.5.1 The Coordinate System and Descriptive Geometry Introduction North, east, south, and west. Go down the street about six blocks, take a left, and then go north for about 2 miles; you will
More informationPrentice Hall Pre-Algebra 2004 Correlated to: Hawaii Mathematics Content and Performance Standards (HCPS) II (Grades 9-12)
Hawaii Mathematics Content and Performance Standards (HCPS) II (Grades 9-12) NUMBER AND OPERATIONS STANDARD 1: Students understand numbers, ways of representing numbers, relationships among numbers, and
More informationRay Optics I. Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex
Phys 531 Lecture 8 20 September 2005 Ray Optics I Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex Today shift gears, start applying
More informationINDUCTIVE AND CAPACITIVE ARRAY IMAGING OF BURIED OBJECTS
INDUCTIVE AND CAPACITIVE ARRAY IMAGING OF BURIED OBJECTS D. Schlicker, A. Washabaugh, I. Shay, N. Goldfine JENTEK Sensors, Inc., Waltham, MA, USA Abstract: Despite ongoing research and development efforts,
More informationChapter 5. 3D data examples REALISTICALLY COMPLEX SYNTHETIC INVERSION. Modeling generation and survey design
Chapter 5 3D data examples In this chapter I will demonstrate the e ectiveness of the methodologies developed in the previous chapters using 3D data examples. I will first show inversion results of a realistically
More informationA Avenue, Bus: (604) Delta BC V4C 3W2 CANADA Memorandum
11966 95A Avenue, Bus: (604) 582-1100 Delta BC V4C 3W2 CANADA E-mail: trent@sjgeophysics.com www.sjgeophysics.com To: Triple Nine Resources Ltd. Four Corners Mining Corp. Memorandum Attn: Victor French
More informationExcerpt from the Proceedings of the COMSOL Conference 2010 Paris
Excerpt from the Proceedings of the COMSOL Conference 2010 Paris Simulation of Flaw Signals in a Magnetic Flux Leakage Inspection Procedure O. Nemitz * and T. Schmitte Salzgitter Mannesmann Forschung GmbH
More informationExercise in Biology and Geometry Part 2
Exercise in Biology and Geometry Part 2 Background Information Imagine you are a scientist that is sent two specimens that have a 3-D configuration. The two specimens have the same size, volume, shape,
More informationReview Sheet for Second Midterm Mathematics 1300, Calculus 1
Review Sheet for Second Midterm Mathematics 300, Calculus. For what values of is the graph of y = 5 5 both increasing and concave up? 2. Where does the tangent line to y = 2 through (0, ) intersect the
More informationSimulation and Validation of Turbulent Pipe Flows
Simulation and Validation of Turbulent Pipe Flows ENGR:2510 Mechanics of Fluids and Transport Processes CFD LAB 1 (ANSYS 17.1; Last Updated: Oct. 10, 2016) By Timur Dogan, Michael Conger, Dong-Hwan Kim,
More informationClasswork. Opening Exercise. Example 1. Which prism will hold more 1 in. 1 in. 1 in. cubes? 12 in. 6 in. 4 in. 5 in. 10 in. 8 in.
Classwork Opening Exercise Which prism will hold more 1 in. 1 in. 1 in. cubes? 6 in. 12 in. 10 in. 4 in. 8 in. 5 in. How many more cubes will the prism hold? Example 1 A box with the same dimensions as
More informationPressure Wave and CO 2 Seismic Events Profile Viewer Java Applet
Pressure Wave and CO 2 Seismic Events Profile Viewer Java Applet by John R. Victorine Introduction This applet is a profile viewer in time that will display the pressure wave data and the selected CO 2
More information= 3 + (5*4) + (1/2)*(4/2)^2.
Physics 100 Lab 1: Use of a Spreadsheet to Analyze Data by Kenneth Hahn and Michael Goggin In this lab you will learn how to enter data into a spreadsheet and to manipulate the data in meaningful ways.
More informationEMIGMA V9.x Premium Series April 8, 2015
EMIGMA V9.x Premium Series April 8, 2015 EMIGMA for Gravity EMIGMA for Gravity license is a comprehensive package that offers a wide array of processing, visualization and interpretation tools. The package
More informationTorsional-lateral buckling large displacement analysis with a simple beam using Abaqus 6.10
Torsional-lateral buckling large displacement analysis with a simple beam using Abaqus 6.10 This document contains an Abaqus tutorial for performing a buckling analysis using the finite element program
More informationUnstructured grid modelling to create 3-D Earth models that unify geological and geophysical information
Unstructured grid modelling to create 3-D Earth models that unify geological and geophysical information Peter Lelièvre, Angela Carter-McAuslan, Cassandra Tycholiz, Colin Farquharson and Charles Hurich
More informationLight, Photons, and MRI
Light, Photons, and MRI When light hits an object, some of it will be reflected. The reflected light can form an image. We usually want to be able to characterize the image given what we know about the
More informationLithological and surface geometry joint inversions using multi-objective global optimization methods
Lithological and surface geometry joint inversions using multi-objective global optimization methods Peter G. Lelièvre 1, Rodrigo Bijani and Colin G. Farquharson 1 plelievre@mun.ca http://www.esd.mun.ca/~peter/home.html
More information4.5 Conservative Forces
4 CONSERVATION LAWS 4.5 Conservative Forces Name: 4.5 Conservative Forces In the last activity, you looked at the case of a block sliding down a curved plane, and determined the work done by gravity as
More informationNX Tutorial - Centroids and Area Moments of Inertia ENAE 324 Aerospace Structures Spring 2015
NX will automatically calculate area and mass information about any beam cross section you can think of. This tutorial will show you how to display a section s centroid, principal axes, 2 nd moments of
More informationPhys102 Lecture 21/22 Light: Reflection and Refraction
Phys102 Lecture 21/22 Light: Reflection and Refraction Key Points The Ray Model of Light Reflection and Mirrors Refraction, Snell s Law Total internal Reflection References 23-1,2,3,4,5,6. The Ray Model
More informationCSEM data uncertainty analysis for 3D inversion Jan Petter Morten, EMGS, Astrid Kornberg Bjørke, EMGS, and Trude Støren, EMGS
CSEM data uncertainty analysis for 3D inversion Jan Petter Morten, EMGS, Astrid Kornberg Bjørke, EMGS, and Trude Støren, EMGS SUMMARY Inaccurate navigation can be an important source of measurement errors
More informationA MATLAB-Based Numerical and GUI Implementation of Cross-Gradients Joint Inversion of Gravity and Magnetic Data
Journal of Software Engineering and Applications, 2015, 8, 93-101 Published Online February 2015 in SciRes. http://www.scirp.org/journal/jsea http://dx.doi.org/10.4236/jsea.2015.82010 A MATLAB-Based Numerical
More informationWe 2MIN 02 Data Density and Resolution Power in 3D DC Resistivity Surveys
We 2MIN 02 Data Density and Resolution Power in 3D DC Resistivity Surveys M. Gharibi 1 *, R. Sharpe 1 1 Quantec Geoscience Ltd Summary Resolution power of a field 3D DC dataset is examined by gradually
More information3.9 LINEAR APPROXIMATION AND THE DERIVATIVE
158 Chapter Three SHORT-CUTS TO DIFFERENTIATION 39 LINEAR APPROXIMATION AND THE DERIVATIVE The Tangent Line Approximation When we zoom in on the graph of a differentiable function, it looks like a straight
More informationCombined Electrical and Magnetic Resistivity Tomography (ERT/MMR)
Combined Electrical and Magnetic Resistivity Tomography (ERT/MMR) Gail Heath 1, John M. Svoboda 1, Birsen Canan 2, Shannon Ansley 1, David Alumbaugh 3, Douglas LaBrecque 4, Roger Sharpe 4,Roelof Versteeg
More informationSection 1.2: Points and Lines
Section 1.2: Points and Lines Objective: Graph points and lines using x and y coordinates. Often, to get an idea of the behavior of an equation we will make a picture that represents the solutions to the
More informationBasic Exercises Maxwell Link with ANSYS Mechanical. Link between ANSYS Maxwell 3D and ANSYS Mechanical
Link between ANSYS Maxwell 3D and ANSYS Mechanical This exercise describes how to set up a Maxwell 3D Eddy Current project and then link the losses to ANSYS Mechanical for a thermal calculation 3D Geometry:
More informationForward and Inverse Modeling of Gravity Data: Locating buried glacial channels and evaluating the results of published analysis
GRAVITY COMPUTER LAB Forward and Inverse Modeling of Gravity Data: Locating buried glacial channels and evaluating the results of published analysis During this lab your task will be to evaluate the accuracy
More informationGEOG 4110/5100 Advanced Remote Sensing Lecture 4
GEOG 4110/5100 Advanced Remote Sensing Lecture 4 Geometric Distortion Relevant Reading: Richards, Sections 2.11-2.17 Geometric Distortion Geometric Distortion: Errors in image geometry, (location, dimensions,
More informationRadiography and Tomography Lab 2: Computing Radiographs
Radiography and Tomography Lab 2: Computing Radiographs An Abbreviated View of Radiography Transmission Radiography is the process of measuring and recording changes in a high-energy particle beam (X-rays,
More informationFAULT SLIP. GG303 Lab 13 11/29/16 1
GG303 Lab 13 11/29/16 1 FAULT SLIP Lab 13 The purpose of this lab is to develop your ability to evaluate the slip along faults. The lab has three parts. The first requires you to evaluate the slip at a
More informationMo 21P1 08 Comparison of Different Acquisition Patterns for 2D Tomographic Resistivity Surveys
Mo 21P1 08 Comparison of Different Acquisition Patterns for 2D Tomographic Resistivity Surveys R. Martorana* (University of Palermo), P. Capizzi (University of Palermo), A. D'Alessandro (INGV - Roma) &
More informationSPRINGBOARD UNIT 5 GEOMETRY
SPRINGBOARD UNIT 5 GEOMETRY 5.1 Area and Perimeter Perimeter the distance around an object. To find perimeter, add all sides. Area the amount of space inside a 2 dimensional object. Measurements for area
More informationGenerate Digital Elevation Models Using Laser Altimetry (LIDAR) Data
Generate Digital Elevation Models Using Laser Altimetry (LIDAR) Data Literature Survey Christopher Weed October 2000 Abstract Laser altimetry (LIDAR) data must be processed to generate a digital elevation
More informationLocal Magnetic Distortion Effects on 3-Axis Compassing
PNI White Paper Local Magnetic Distortion Effects on 3-Axis Compassing SUMMARY Digital 3-axis compasses from three different manufacturers were tested for heading error when a battery (having magnetic
More informationCharacter Modeling IAT 343 Lab 6. Lanz Singbeil
Character Modeling IAT 343 Lab 6 Modeling Using Reference Sketches Start by creating a character sketch in a T-Pose (arms outstretched) Separate the sketch into 2 images with the same pixel height. Make
More informationChapter 7: Geometrical Optics. The branch of physics which studies the properties of light using the ray model of light.
Chapter 7: Geometrical Optics The branch of physics which studies the properties of light using the ray model of light. Overview Geometrical Optics Spherical Mirror Refraction Thin Lens f u v r and f 2
More informationAirborne IP for Kimberlite
The University of British Columbia Geophysical Inversion Facility Airborne IP for Kimberlite Douglas W. Oldenburg and Seogi Kang IP workshop 2016 June 7 th 2016 gif.eos.ubc.ca slide 1 Acknowledgements
More informationPlotting Graphs. Error Bars
E Plotting Graphs Construct your graphs in Excel using the method outlined in the Graphing and Error Analysis lab (in the Phys 124/144/130 laboratory manual). Always choose the x-y scatter plot. Number
More informationAstromechanics. 12. Satellite Look Angle
Astromechanics 12. Satellite Look Angle The satellite look angle refers to the angle that one would look for a satellite at a given time from a specified position on the Earth. For example, if you had
More informationMARINE HARBOR SURVEY USING THE G-882 TRANSVERSE GRADIOMETER WITH ANALYTIC SIGNAL PROCESSING
M-TR138 MARINE HARBOR SURVEY USING THE G-882 TRANSVERSE GRADIOMETER WITH ANALYTIC SIGNAL PROCESSING Mikhail Tchernychev and George Tait Geometrics September 2007 Data courtesy of the US Navy MFS Hawaii
More informationGmax Terrain Tutorial
Gmax Terrain Tutorial by Kobbe Farwick http://realscenes.proboards81.com You will need the following - Global Mapper Mesh data (GeoTIFF) Aerial/Satellite Imagery (GeoTIFF) FSX/FS2004 Gmax Gamepack Image
More informationCOGO-50 v1.81 User Manual By Jacob Wall
COGO-50 v1.81 User Manual By Jacob Wall COGO-50 is a (mostly) UserRPL program written for the HP 49g+/50g using ROM Version 2.09 (also tested with ROM Version 2.15). It is a land surveying program capable
More information