Introduction to Potential Fields: Magnetics
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CERI 7022/8022 Global Geophysics Spring 2016
FerrimagnetismI I Recall three types of magnetic properties of materials I Diamagnetism I Paramagnetism I Ferromagnetism I Anti-ferromagnetism I Parasitic ferromagnetism I Ferrimagnetism I Ferrimagnetism I Spinel structure is one of the common crystal structure of rock-forming minerals. I Tetrahedral and octahedral sites form two sublattices. 2+ 3+ I Fe in 1/8 of tetrahedral sites, Fe in 1/2 of octahedral sites. FerrimagnetismII I xmujpkc.xmu.edu.cn/jghx/source/chapter9.pdf Ferrimagnetism III I www.tf.uni-kiel.de/matwis/amat/def_en/kap_2/basics/b2_1_6.html I Anti-spinel structure of the most common iron oxides 3+ 3+ 2+ I Fe in 1/8 tetrahedral sites, (Fe , Fe ) in 1/2 of octahedral sites. FerrimagnetismIV I Indirect exchange involves antiparallel and unequal magnetization of the sublattices, a net spontaneous magnetization appears. This phenomenon is called ferrimagnetism. I Ferrimagnetic materials are called ferrites. I Ferrites exhibit magnetic hysteresis and retain remanent magnetization (i.e. behaves like ferromagnets.) I Above the Curie temperature, becomes paramagnetic. I Magnetite (Fe3O4), maghemite, pyrrhotite and goethite (' rust). Magnetic properties of rocksI I Matrix minerals are mainly silicates or carbonates, which are diamagnetic. I Secondary minerals (e.g., clays) have paramagnetic properties. I So, the bulk of constituent minerals have a magnetic susceptibility but not remanent magnetic properties. I Variable concentrations of ferrimagnetic and matrix minerals result in a wide range of susceptibilities in rocks. Magnetic properties of rocksII I I The weak and variable concentration of ferrimagnetic minerals plays a key role in determining the magnetic properties of the rock. Magnetic properties of rocks III I Important factors influencing rock magnetism: I The type of ferrimagnetic mineral. -
Magnetic Surveying for Buried Metallic Objects
Reprinted from the Summer 1990 Issue of Ground Water Monitoring Review Magnetic Surveying for Buried Metallic Objects by Larry Barrows and Judith E. Rocchio Abstract Field tests were conducted to determine representative total-intensity magnetic anomalies due to the presence of underground storage tanks and 55-gallon steel drums. Three different drums were suspended from a non-magnetic tripod and the underlying field surveyed with each drum in an upright and a flipped plus rotated orientation. At drum-to-sensor separations of 11 feet, the anomalies had peak values of around 50 gammas and half-widths about equal to the drum-to-sensor separation. Remanent and induced magnetizations were comparable; crushing one of the drums significantly reduced both. A profile over a single underground storage tank had a 1000-gamma anomaly, which was similar to the modeled anomaly due to an infinitely long cylinder horizontally magnetized perpendicular to its axis. A profile over two adjacent tanks had a. smooth 350-gamma single-peak anomaly even though models of two tanks produced dual-peaked anomalies. Demagnetization could explain why crushing a drum reduced its induced magnetization and why two adjacent tanks produced a single-peak anomaly. A 40-acre abandoned landfill was surveyed on a 50- by 100-foot rectangular grid and along several detailed profiles; The observed field had broad positive and negative anomalies that were similar to modeled anomalies due to thickness variations in a layer of uniformly magnetized material. It was not comparable to the anomalies due to induced magnetization in multiple, randomly located, randomly sized, independent spheres, suggesting that demagne- tization may have limited the effective susceptibility of the landfill material. -
Rock and Paleomagnetic Investigations Technical Detailed
NWM-USGS-GPP-06 RO Rock and Paleomagnetic Investigations Technical Detailed Procedure GPP-O NNWSI Project Quality Assurance Program U.S. Geological Survey Effective Date: pepared by: Joseph Rosenbaum Technical Reviewer: Richard Reynolds 'Branch Chief: Adel Zohdy NNWI Project Coordinator: W. Dudley Quality Assurance: P. L. Bussolini 8502210165 841130 PDR WASTE PDR Wm-II NWM-USGS-GPP- 06, RO NWM-USGS-GPP- o RO Page 2 of 13 Rock and Paleomagnetic Investigations 1.0 PURPOSE 1.1 This procedure provides a means of assuring the accuracy, validity, and applicability of the methods used to determine paleomagnetic and rock magnetic properties. 1.2 The procedure documents the USGS responsibilities for quality assurance training and enforcement, the processes and authority for procedure modification and revision, the requirements for procedure and personnel interfacing, and to whom the procedure applies. 1.3 The procedure describes the system components, the principles of the methods used, and the limits of their use. 1.4 The procedure describes the detailed methods to be used, where applicable, for system checkout and maintenance, calibration, operation and performance verification. 1.5 The procedure defines the requirements for data acceptance, documentation and control; and provides a means of data traceability. 1.6 The procedure provides a guide for USGS personnel and their contractors engaged to determining paleomagnetic and rock mag- netic properties and a means by which the Department of Energy (DOE) and the Nuclear Regulatory Commission (NRC) can evaluate these activities in meeting requirements for the NNWSI repository. 2.0 SCOPE OF COMPLIANCE 2.1 This procedure applies to all USGS personnel, and persons assigned by the USGS, who perform work on the procedure as described by the work activity given in Section 1.1, or use data from such activities, if the activities or data are deemed by the USGS Project Coordinator to potentially affect public health and safety as related to a nuclear waste repository. -
Magnetic Signature of the Leucogranite in Örsviken
UNIVERSITY OF GOTHENBURG Department of Earth Sciences Geovetarcentrum/Earth Science Centre Magnetic signature of the leucogranite in Örsviken Hannah Berg Johanna Engelbrektsson ISSN 1400-3821 B774 Bachelor of Science thesis Göteborg 2014 Mailing address Address Telephone Telefax Geovetarcentrum Geovetarcentrum Geovetarcentrum 031-786 19 56 031-786 19 86 Göteborg University S 405 30 Göteborg Guldhedsgatan 5A S-405 30 Göteborg SWEDEN Abstract A proton magnetometer is a useful tool in detecting magnetic anomalies that originate from sources at varying depths within the Earth’s crust. This makes magnetic investigations a good way to gather 3D geological information. A field investigation of a part of a cape that consists of a leucogranite in Örsviken, 20 kilometres south of Gothenburg, was of interest after high susceptibility values had been discovered in the area. The investigation was carried out with a proton magnetometer and a hand-held susceptibility meter in order to obtain the magnetic anomalies and susceptibility values. High magnetic anomalies were observed on the southern part of the cape and further south and west below the water surface. The data collected were then processed in Surfer11® and in Encom ModelVision 11.00 in order to make 2D and 3D magnetometric models of the total magnetic field in the study area as well as visualizing the geometry and extent of the rock body of interest. The results from the investigation and modelling indicate that the leucogranite extends south and west of the cape below the water surface. Magnetite is interpreted to be the cause of the high susceptibility values. The leucogranite is a possible A-type alkali granite with an anorogenic or a post-orogenic petrogenesis. -
Preliminary Aeromagnetic Anomaly Map of California
PRELIMINARY AEROMAGNETIC ANOMALY MAP OF CALIFORNIA By Carter W. Roberts and Robert C. Jachens Open-File Report 99-440 1999 This report is preliminary and has not been reviewed for conformity with U.S. Geological Survey editorial standards or with the North American Stratigraphic Code. Any use of trade, firm, or product names is for descriptive purposes only and does not imply endorsement by the U.S. Government. U.S. DEPARTMENT OF THE INTERIOR U.S. GEOLOGICAL SURVEY 1 INTRODUCTION The magnetization in crustal rocks is the vector sum of induced in minerals by the Earth’s present main field and the remanent magnetization of minerals susceptible to magnetization (chiefly magnetite) (Blakely, 1995). The direction of remanent magnetization acquired during the rock’s history can be highly variable. Crystalline rocks generally contain sufficient magnetic minerals to cause variations in the Earth’s magnetic field that can be mapped by aeromagnetic surveys. Sedimentary rocks are generally weakly magnetized and consequently have a small effect on the magnetic field: thus a magnetic anomaly map can be used to “see through” the sedimentary rock cover and can convey information on lithologic contrasts and structural trends related to the underlying crystalline basement (see Nettleton,1971; Blakely, 1995). The magnetic anomaly map (fig. 2) provides a synoptic view of major anomalies and contributes to our understanding of the tectonic development of California. Reference fields, that approximate the Earth’s main (core) field, have been subtracted from the recorded magnetic data. The resulting map of the total magnetic anomalies exhibits anomaly patterns related to the distribution of magnetized crustal rocks at depths shallower than the Curie point isotherm (the surface within the Earth beneath which temperatures are so high that rocks lose their magnetic properties). -
Design of a Curie Point Meter
BULLETIN 69 DESIGN OF A CURIE POINT METER A. Larochelle Price, 50 cents 1961 DESIGN OF A CURIE POINT METER 3,000-1960-1818 91594-2-1 11 026: General view of Curie point meter GEOLOGICAL SURVEY OF CANADA BULLETIN 69 DESIGN OF A CURIE POINT METER By A. Larochelle DEPARTMENT OF MINES AND TECHNICAL SURVEYS CANADA 91594-2-2 ROGER DUHAMEL. F.R.S.C. QUEEN'S PRINTER AND CONTROLLER OF STATIONERY OTTAWA, 1961 Price 50 cents Cat. No. M42-69 Preface Magnetic properties are rarely used to identify minerals because they are generally difficult to detect or to determine accurately. Ferromagnetic minerals are, however, an exception. Not only can a family of ferromagnetic minerals be identified from its magnetic properties, but individual members of the family can be recognized. The Curie point is one of the most reliable magnetic properties for identifying such minerals. The apparatus described in this bulletin was designed to permit the rapid, accurate measurement of the Curie point of the ferromagnetic minerals in rock specimens, and by this means to identify them. J. M. HARRISON, Director, Geological Survey of Canada OTTAWA, April 28, 1960 v CONTENTS PAGE Introduction 1 General description 1 The torsion balance 2 The recording system 6 The heating element ........ ..... 8 The electromagnet 9 Operation and calibration of the apparatus 12 Practical application . 15 Bibliography 18 Table I. Curie points of specimens of basic intrusive rocks . 16 Plate I. General view of Curie point meter Frontispiece Figure 1. Schematic view of the Curie point meter . 2 2. Longitudinal section of torsion balance 3 3. -
Rock Magnetism of Remagnetized Carbonate Rocks: Another Look
Downloaded from http://sp.lyellcollection.org/ at University of California Berkeley on July 30, 2013 Rock magnetism of remagnetized carbonate rocks: another look MIKE JACKSON* & NICHOLAS L. SWANSON-HYSELL Institute for Rock Magnetism, Winchell School of Earth Sciences, University of Minnesota, Minnesota, US *Corresponding author (e-mail: [email protected]) Abstract: Authigenic formation of fine-grained magnetite is responsible for widespread chemical remagnetization of many carbonate rocks. Authigenic magnetite grains, dominantly in the super- paramagnetic and stable single-domain size range, also give rise to distinctive rock-magnetic prop- erties, now commonly used as a ‘fingerprint’ of remagnetization. We re-examine the basis of this association in terms of magnetic mineralogy and particle-size distribution in remagnetized carbon- ates having these characteristic rock-magnetic properties, including ‘wasp-waisted’ hysteresis loops, high ratios of anhysteretic remanence to saturation remanence and frequency-dependent susceptibility. New measurements on samples from the Helderberg Group allow us to quantify the proportions of superparamagnetic, stable single-domain and larger grains, and to evaluate the mineralogical composition of the remanence carriers. The dominant magnetic phase is magnetite-like, with sufficient impurity to completely suppress the Verwey transition. Particle sizes are extremely fine: approximately 75% of the total magnetite content is superparamagnetic at room temperature and almost all of the rest is stable single-domain. Although it has been pro- posed that the single-domain magnetite in these remagnetized carbonates lacks shape anisotropy (and is therefore controlled by cubic magnetocrystalline anisotropy), we have found strong exper- imental evidence that cubic anisotropy is not an important underlying factor in the rock-magnetic signature of chemical remagnetization. -
GEOPHYSICAL STUDY of the SALTON TROUGH of Soutllern CALIFORNIA
GEOPHYSICAL STUDY OF THE SALTON TROUGH OF SOUTllERN CALIFORNIA Thesis by Shawn Biehler In Partial Fulfillment of the Requirements For the Degree of Doctor of Philosophy California Institute of Technology Pasadena. California 1964 (Su bm i t t ed Ma Y 7, l 964) PLEASE NOTE: Figures are not original copy. 11 These pages tend to "curl • Very small print on several. Filmed in the best possible way. UNIVERSITY MICROFILMS, INC. i i ACKNOWLEDGMENTS The author gratefully acknowledges Frank Press and Clarence R. Allen for their advice and suggestions through out this entire study. Robert L. Kovach kindly made avail able all of this Qravity and seismic data in the Colorado Delta region. G. P. Woo11ard supplied regional gravity maps of southern California and Arizona. Martin F. Kane made available his terrain correction program. c. w. Jenn ings released prel imlnary field maps of the San Bernardino ct11u Ni::eule::> quad1-angles. c. E. Co1-bato supplied information on the gravimeter calibration loop. The oil companies of California supplied helpful infor mation on thelr wells and released somA QAnphysical data. The Standard Oil Company of California supplied a grant-In- a l d for the s e i sm i c f i e l d work • I am i ndebt e d to Drs Luc i en La Coste of La Coste and Romberg for supplying the underwater gravimeter, and to Aerial Control, Inc. and Paclf ic Air Industries for the use of their Tellurometers. A.Ibrahim and L. Teng assisted with the seismic field program. am especially indebted to Elaine E. -
Magnetic Properties of the Magnetite-Spinel Solid Solution: Curie Temperatures, Magnetic Susceptibilities, and Cation Ordering
American Mineralogist, Volume 81, pages 375-384, 1996 Magnetic properties of the magnetite-spinel solid solution: Curie temperatures, magnetic susceptibilities, and cation ordering RICHARD J. HARRISON ANDANDREW PurNIS * Department of Earth Sciences, University of Cambridge, Downing Street, Cambridge CB2 3EQ, U.K. ABSTRACT Curie temperatures (Td of the (Fe304)x(MgA1204)1-xsolid solution have been deter- mined from measurements of magnetic susceptibility (x) vs. temperature. The trend in Te vs. composition extrapolates to 0 K at x = 0.27. This behavior is rationalized in terms of the trend in cation distribution vs. composition suggested by Nell and Wood (1989), with Fe occurring predominantly on tetrahedral sites for x < 0.27. High-temperature x-T curves are nonreversible because of the processes of cation or- dering and exsolution, which occur in the temperature range 400-650 0c. The Curie tem- perature of single-phase material is shown to be sensitive to the state of nonconvergent cation order, with a difference in Te of more than 70°C being observed between a sample quenched from 1400 °C and the same sample after heating to 650°C. This interaction between magnetic and chemical ordering leads to thermal hysteresis behavior such that Te measured during heating experiments is approximately 10°Chigherthan that measured during cooling. The hysteresis is due to a reversible difference in the state of cation order during heating and cooling caused by a kinetic lag in the cation-ordering behavior. Samples with compositions in the range 0.55 < x < 0.7 undergo exsolution to a mixture of ferrimagnetic and paramagnetic phases after heating to 650°C. -
Magnetic Properties of Dredged Oceanic Gabbros and the Source of Marine Magnetic Anomalies
Geophys. J. R. astr. SOC.(1978) 55,513-537 Magnetic properties of dredged oceanic gabbros and the source of marine magnetic anomalies D. v. Kent Lamont-Doherty Geological Observatory, Columbia University,-* Palisades, New York 10964, USA B. M. Honnorez Rosenstiel School of Marine and Atmospheric Science, University Miami, Miami, Florida 33149, USA of '', ~ N. D. 0pdyke' Department of Geological Sciences, Columbia University, New York, New York 10027, USA Sr P. J . FOX Department of Geological Sciences, State University, Albany, New York 12222, USA 7 Received 1978 May 1O;in original form 1978 January 16 Summary. Magnetic property studies (natural remanent magnetization, initial susceptibility, progressive alternating field demagnetization and magnetic mineralogy of selected samples) were completed on 45 samples of gabbro and metagabbro recovered from 14 North Atlantic ocean-floor localities. The samples are medium to coarse-grained gabbro and metagabbro which exhibit subophitic intergranular to hypidiomorphic granular igneous textures. The igneous mineralogy is characterized by abundant plagioclase, varying amounts of clinopyroxene and hornblende, and lesser amounts of magnetite, ilmenite and sphene. Metamorphic minerals (actinolite, chlorite, epidote and fine-grained alteration products) occur in varying amounts as replacement products or vein material. The opaque mineralogy is dominated by magnetite and ilmenite. The magnetite typically exhibits a trellis of exsolution-oxidation ilmenite lamellae that appears to have formed during deuteric alteration. The NRM intensities of the gabbros range over three orders of magnitude and give a geometric mean of 2.8 x 10-4gau~~and an arithmetic mean of 8.8 x 10-4gauss. The Konigsberger ratio, a measure of the relative importance of remanent to induce magnetization, is greater than unity for the majority of the samples and indicates that remanent magnetization on average dominates the total magnetization of oceanic gabbros in the Earth's magnetic field. -
8. Data Report: Paleomagnetic and Rock Magnetic Characterization of Rocks Recovered from Leg 173 Sites1
Beslier, M.-O., Whitmarsh, R.B., Wallace, P.J., and Girardeau, J. (Eds.) Proceedings of the Ocean Drilling Program, Scientific Results Volume 173 8. DATA REPORT: PALEOMAGNETIC AND ROCK MAGNETIC CHARACTERIZATION OF ROCKS RECOVERED FROM LEG 173 SITES1 Xixi Zhao,2 Brent D. Turrin,3 Mike Jackson,4 and Peter Solheid4 ABSTRACT We present detailed paleomagnetic and rock magnetic results of rock samples recovered during Leg 173. The Leg 173 cores display a multi- component magnetization nature. Variations in magnetic properties correlate with changes in lithology that result from differences in the 1Zhao, X., Turrin, B.D., Jackson, M., abundance and size of magnetic minerals. The combined investigation and Solheid, P., 2001. Data report: suggests that the magnetic properties of the “fresher” peridotite sam- Paleomagnetic and rock magnetic ples from Site 1070 are controlled mainly by titanomagnetite, with a characterization of rocks recovered from Leg 173 sites. In Beslier, M.-O., strong Verwey transition in the vicinity of 110 K, and with field- and Whitmarsh, R.B., Wallace, P.J., and frequency-dependent susceptibility curves that resemble those of tita- Girardeau, J. (Eds.), Proc. ODP, Sci. nomagnetites. These results are in excellent agreement with thermo- Results, 173, 1–34 [Online]. Available magnetic characteristics where titanomagnetites with Curie tempera- from World Wide Web: <http:// ture ~580°C were identified from the “fresher” peridotites. In contrast www-odp.tamu.edu/publications/ 173_SR/VOLUME/CHAPTERS/ to the magnetic properties observed from the “fresher” peridotites, the SR173_08.PDF>. [Cited YYYY-MM-DD] low-temperature curves for the “altered” peridotites did not show any 2Institute of Tectonics, University of Verwey transition. -
And Palaeo-Magnetism
Opening Remarks for Symposium on Rock- and Palaeo-Magnetism (IUGG Kyoto Symposium on Rock- and Palaeo-Magnetism) By Takesi NAGATA Organizer of the Symposium, GeophysicalInstitute, University of Tokyo In connexion with the International Conference on Magnetism and Crystallography, which is held on 25th-30th September 1961 at Kyoto under auspices of the International Union of Pare and Applied Physics (IUPAP) and the International Union of Crystal- lography (IUCr), an international symposium on rock-and ppalaeo-magnetism is now held at Kyoto. This symposium is organized according to request by a number of active workers in this branch of science and by many members of the Committee on Secular Variation and Palaeomagnetism of the Association of Geomagnetism and Aeronomy (IAGA) of the International Union of Geodesy and Geophysics (IUGG). This symposium is, therefore, formally sponsored by IUGG, and may be called the "IUGG Kyoto Symposium on Rock - and Palaeo-Magnetism in 1961." We had a scientific session on "Physical Problems of Rock Magnetism" as a part of the Conference on Magnetism and Crystallography. In the session several basic problems of physical characteristics of fine grains of rock-forming metallic oxides are mainly discussed in view of solid state physics. Two main topics in that session were self-reversal of remanent magnetization and superparamagnetism and super- antiferromagnetism of very fine grains of metallic oxides. (The full papers presented to this session will be published as a part of the proceedings of the whole conference, a special volume of the Journal of Physical Society of Japan). In the present rock- and palaeo-magnetism symposium, various important topics in rock-magnetism and palaeomagnetism will be discussed more generally in connexion with geophysics and geology as well as solid state physics of materials.