Review of Paleomagnetism Resume
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Is Earth's Magnetic Field Reversing? ⁎ Catherine Constable A, , Monika Korte B
Earth and Planetary Science Letters 246 (2006) 1–16 www.elsevier.com/locate/epsl Frontiers Is Earth's magnetic field reversing? ⁎ Catherine Constable a, , Monika Korte b a Institute of Geophysics and Planetary Physics, Scripps Institution of Oceanography, University of California at San Diego, La Jolla, CA 92093-0225, USA b GeoForschungsZentrum Potsdam, Telegrafenberg, 14473 Potsdam, Germany Received 7 October 2005; received in revised form 21 March 2006; accepted 23 March 2006 Editor: A.N. Halliday Abstract Earth's dipole field has been diminishing in strength since the first systematic observations of field intensity were made in the mid nineteenth century. This has led to speculation that the geomagnetic field might now be in the early stages of a reversal. In the longer term context of paleomagnetic observations it is found that for the current reversal rate and expected statistical variability in polarity interval length an interval as long as the ongoing 0.78 Myr Brunhes polarity interval is to be expected with a probability of less than 0.15, and the preferred probability estimates range from 0.06 to 0.08. These rather low odds might be used to infer that the next reversal is overdue, but the assessment is limited by the statistical treatment of reversals as point processes. Recent paleofield observations combined with insights derived from field modeling and numerical geodynamo simulations suggest that a reversal is not imminent. The current value of the dipole moment remains high compared with the average throughout the ongoing 0.78 Myr Brunhes polarity interval; the present rate of change in Earth's dipole strength is not anomalous compared with rates of change for the past 7 kyr; furthermore there is evidence that the field has been stronger on average during the Brunhes than for the past 160 Ma, and that high average field values are associated with longer polarity chrons. -
Paleomagnetism and U-Pb Geochronology of the Late Cretaceous Chisulryoung Volcanic Formation, Korea
Jeong et al. Earth, Planets and Space (2015) 67:66 DOI 10.1186/s40623-015-0242-y FULL PAPER Open Access Paleomagnetism and U-Pb geochronology of the late Cretaceous Chisulryoung Volcanic Formation, Korea: tectonic evolution of the Korean Peninsula Doohee Jeong1, Yongjae Yu1*, Seong-Jae Doh2, Dongwoo Suk3 and Jeongmin Kim4 Abstract Late Cretaceous Chisulryoung Volcanic Formation (CVF) in southeastern Korea contains four ash-flow ignimbrite units (A1, A2, A3, and A4) and three intervening volcano-sedimentary layers (S1, S2, and S3). Reliable U-Pb ages obtained for zircons from the base and top of the CVF were 72.8 ± 1.7 Ma and 67.7 ± 2.1 Ma, respectively. Paleomagnetic analysis on pyroclastic units yielded mean magnetic directions and virtual geomagnetic poles (VGPs) as D/I = 19.1°/49.2° (α95 =4.2°,k = 76.5) and VGP = 73.1°N/232.1°E (A95 =3.7°,N =3)forA1,D/I = 24.9°/52.9° (α95 =5.9°,k =61.7)and VGP = 69.4°N/217.3°E (A95 =5.6°,N=11) for A3, and D/I = 10.9°/50.1° (α95 =5.6°,k = 38.6) and VGP = 79.8°N/ 242.4°E (A95 =5.0°,N = 18) for A4. Our best estimates of the paleopoles for A1, A3, and A4 are in remarkable agreement with the reference apparent polar wander path of China in late Cretaceous to early Paleogene, confirming that Korea has been rigidly attached to China (by implication to Eurasia) at least since the Cretaceous. The compiled paleomagnetic data of the Korean Peninsula suggest that the mode of clockwise rotations weakened since the mid-Jurassic. -
Equivalence of Current–Carrying Coils and Magnets; Magnetic Dipoles; - Law of Attraction and Repulsion, Definition of the Ampere
GEOPHYSICS (08/430/0012) THE EARTH'S MAGNETIC FIELD OUTLINE Magnetism Magnetic forces: - equivalence of current–carrying coils and magnets; magnetic dipoles; - law of attraction and repulsion, definition of the ampere. Magnetic fields: - magnetic fields from electrical currents and magnets; magnetic induction B and lines of magnetic induction. The geomagnetic field The magnetic elements: (N, E, V) vector components; declination (azimuth) and inclination (dip). The external field: diurnal variations, ionospheric currents, magnetic storms, sunspot activity. The internal field: the dipole and non–dipole fields, secular variations, the geocentric axial dipole hypothesis, geomagnetic reversals, seabed magnetic anomalies, The dynamo model Reasons against an origin in the crust or mantle and reasons suggesting an origin in the fluid outer core. Magnetohydrodynamic dynamo models: motion and eddy currents in the fluid core, mechanical analogues. Background reading: Fowler §3.1 & 7.9.2, Lowrie §5.2 & 5.4 GEOPHYSICS (08/430/0012) MAGNETIC FORCES Magnetic forces are forces associated with the motion of electric charges, either as electric currents in conductors or, in the case of magnetic materials, as the orbital and spin motions of electrons in atoms. Although the concept of a magnetic pole is sometimes useful, it is diácult to relate precisely to observation; for example, all attempts to find a magnetic monopole have failed, and the model of permanent magnets as magnetic dipoles with north and south poles is not particularly accurate. Consequently moving charges are normally regarded as fundamental in magnetism. Basic observations 1. Permanent magnets A magnet attracts iron and steel, the attraction being most marked close to its ends. -
2. Geomagnetism and Paleomagnetism
2-1 2. GEOMAGNETISM AND PALEOMAGNETISM 1 https://physicalgeology.pressbooks.com/chapter/4-3-geological-renaissance-of-the-mid-20th-century/ 2 2-2 ELECTRIC q Q FIELD q -Q 3 MAGNETIC DIPOLE Although magnetic fields have a similar form to electric fields, they differ because there are no single magnetic "charges," known as magnetic poles. Hence the fundamental entity is the magnetic dipole arising from an electric current I circulating in a conducting loop, such as a wire, with area A . The field is described as resulting from a magnetic dipole characterized by a dipole moment m Magnetic dipoles can arise from electric currents - which are moving electric charges - on scales ranging from wire loops to the hot fluid moving in the core that generates the earth’s magnetic field. They also arise at the atomic level, where they are intrinsic properties of charged particles like protons and electrons. As a result, rocks can be magnetized, much like familiar bar magnets. Although the magnetism of a bar magnet arises from the electrons within it, it can be viewed as a magnetic dipole, with north and south magnetic poles at opposite ends. 4 2-3 MAGNETIC FIELD 5 We visualize the magnetic field of a dipole in terms of magnetic field lines pointing outward from the north pole of a bar magnet and in toward the south. The lines point in the direction another bar magnet, such as a compass needle, would point. At any point, the north pole of the compass needle would point along the DIPOLE field line, toward the south pole MAGNETIC of the bar magnet. -
2. Geomagnetism and Paleomagnetism
2. GEOMAGNETISM AND PALEOMAGNETISM https://physicalgeology.pressbooks.com/chapter/4-3-geological-renaissance-of-the-mid-20th-century/ Click for audio Topic 2a 1 Topic 2a 2 q Q ELECTRIC FIELD q -Q Topic 2a 3 MAGNETIC DIPOLE Although magnetic fields have a similar form to electric fields, they differ because there are no single magnetic "charges," known as magnetic poles. Hence the fundamental entity is the magnetic dipole arising from an electric current I circulating in a conducting loop, such as a wire, with area A . The field is described as resulting from a magnetic dipole characterized by a dipole moment m Magnetic dipoles can arise from electric currents - which are moving electric charges - on scales ranging from wire loops to the hot fluid moving in the core that generates the earth’s magnetic field. They also arise at the atomic level, where they are intrinsic properties of charged particles like protons and electrons. As a result, rocks can be magnetized, much like familiar bar magnets. Although the magnetism of a bar magnet arises from the electrons within it, it can be viewed as a magnetic dipole, with north and south magnetic poles at opposite ends. Topic 2a 4 Magnetic field B Units of B Tesla (T) = kg/s 2 -A A = Ampere (unit of current) Gauss (G) = 10-4 Tesla Gamma (! )= 10-9 Tesla = 1 nanoTesla (nT) Earth’s field is about 50 "T = 50 x 10-6 Tesla Topic 2a 5 We visualize the magnetic field of a dipole in terms of magnetic field lines pointing outward from the north pole of a bar magnet and in toward the south. -
Dating Techniques.Pdf
Dating Techniques Dating techniques in the Quaternary time range fall into three broad categories: • Methods that provide age estimates. • Methods that establish age-equivalence. • Relative age methods. 1 Dating Techniques Age Estimates: Radiometric dating techniques Are methods based in the radioactive properties of certain unstable chemical elements, from which atomic particles are emitted in order to achieve a more stable atomic form. 2 Dating Techniques Age Estimates: Radiometric dating techniques Application of the principle of radioactivity to geological dating requires that certain fundamental conditions be met. If an event is associated with the incorporation of a radioactive nuclide, then providing: (a) that none of the daughter nuclides are present in the initial stages and, (b) that none of the daughter nuclides are added to or lost from the materials to be dated, then the estimates of the age of that event can be obtained if the ration between parent and daughter nuclides can be established, and if the decay rate is known. 3 Dating Techniques Age Estimates: Radiometric dating techniques - Uranium-series dating 238Uranium, 235Uranium and 232Thorium all decay to stable lead isotopes through complex decay series of intermediate nuclides with widely differing half- lives. 4 Dating Techniques Age Estimates: Radiometric dating techniques - Uranium-series dating • Bone • Speleothems • Lacustrine deposits • Peat • Coral 5 Dating Techniques Age Estimates: Radiometric dating techniques - Thermoluminescence (TL) Electrons can be freed by heating and emit a characteristic emission of light which is proportional to the number of electrons trapped within the crystal lattice. Termed thermoluminescence. 6 Dating Techniques Age Estimates: Radiometric dating techniques - Thermoluminescence (TL) Applications: • archeological sample, especially pottery. -
The Flux Line News of the Geomagnetism, Paleomagnetism and Electromagnetism Section of AGU
The Flux Line News of the Geomagnetism, Paleomagnetism and Electromagnetism Section of AGU November 2018 Fall 2018 AGU Meeting Events! The GPE Section will have primary responsibility for 10 oral, 11 poster sessions, 1 eLightning session and 1 Union session at the 2018 Fall AGU meeting, December 10-14, in addition to secondary sessions. GPE sessions cover all five conference days kicking off on Monday morning right through Friday morning (see synopsis on page 9). Many thanks go out to all our session conveners. A special thanks goes out to France Lagroix, GPE Secretary, who put together the GPE sessions for all of us. France points out that we need many OSPA judges for our student presentations. Please sign up to help us judge student presentations: (http://ospa.agu.org/ospa/judges/) Mark your calendars for these special events: • GPE Student Reception: Monday, Dec. 10, 6:00 – 7:30-8 pm, at Marriott-Marquis Hotel This is a GPE-sponsored event to help students and postdocs get to know each other and meet the GPE leadership. If you plan on attending please email Shelby Jones-Cervantes • AGU Icebreaker: Monday, Dec. 11, 6-8 pm, Convention Center, Exhibit Hall D-E • AGU Student Breakfast: Tuesday, Dec. 12 at 7 am, Marriot-Marquis Hotel First come, first served. Look for the GPE table. • Bullard Lecture: Tuesday, Dec 12 Hunting the Magnetic Field presented by Lisa Tauxe, Marquis 6. See story page 4 • GPE Business Meeting and Reception: Tuesday, Dec 11, 6:30 – 8:00 pm, Grand Hyatt Washington Hotel, Constitution Level, Room A • AGU Honors Ceremony: Wednesday, Dec. -
Paleomagnetism and Counterclockwise Tectonic Rotation of the Upper Oligocene Sooke Formation, Southern Vancouver Island, British Columbia
499 Paleomagnetism and counterclockwise tectonic rotation of the Upper Oligocene Sooke Formation, southern Vancouver Island, British Columbia Donald R. Prothero, Elizabeth Draus, Thomas C. Cockburn, and Elizabeth A. Nesbitt Abstract: The age of the Sooke Formation on the southern coast of Vancouver Island, British Columbia, Canada, has long been controversial. Prior paleomagnetic studies have produced a puzzling counterclockwise tectonic rotation on the underlying Eocene volcanic basement rocks, and no conclusive results on the Sooke Formation itself. We took 21 samples in four sites in the fossiliferous portion of the Sooke Formation west of Sooke Bay from the mouth of Muir Creek to the mouth of Sandcut Creek. After both alternating field (AF) and thermal demagnetization, the Sooke Formation produces a single-component remanence, held largely in magnetite, which is entirely reversed and rotated counterclockwise by 358 ± 128. This is consistent with earlier results and shows that the rotation is real and not due to tectonic tilting, since the Sooke Formation in this region has almost no dip. This rotational signature is also consistent with counterclockwise rota- tions obtained from the northeast tip of the Olympic Peninsula in the Port Townsend volcanics and the Eocene–Oligocene sediments of the Quimper Peninsula. The reversed magnetozone of the Sooke sections sampled is best correlated with Chron C6Cr (24.1–24.8 Ma) or latest Oligocene in age, based on the most recent work on the Liracassis apta Zone mol- luscan fauna, and also a number of unique marine mammals found in the same reversed magnetozone in Washington and Oregon. Re´sume´ : L’aˆge de la Formation de Sooke sur la coˆte sud de l’ıˆle de Vancouver, Colombie-Britannique, Canada, a long- temps e´te´ controverse´. -
5 Geomagnetism and Paleomagnetism
5 Geomagnetism and paleomagnetism It is not known when the directive power of the magnet 5.1 HISTORICAL INTRODUCTION - its ability to align consistently north-south - was first recognized. Early in the Han dynasty, between 300 and 5.1.1 The discovery of magnetism 200 BC, the Chinese fashioned a rudimentary compass Mankind's interest in magnetism began as a fascination out of lodestone. It consisted of a spoon-shaped object, with the curious attractive properties of the mineral lode whose bowl balanced and could rotate on a flat polished stone, a naturally occurring form of magnetite. Called surface. This compass may have been used in the search loadstone in early usage, the name derives from the old for gems and in the selection of sites for houses. Before English word load, meaning "way" or "course"; the load 1000 AD the Chinese had developed suspended and stone was literally a stone which showed a traveller the pivoted-needle compasses. Their directive power led to the way. use of compasses for navigation long before the origin of The earliest observations of magnetism were made the aligning forces was understood. As late as the twelfth before accurate records of discoveries were kept, so that century, it was supposed in Europe that the alignment of it is impossible to be sure of historical precedents. the compass arose from its attempt to follow the pole star. Nevertheless, Greek philosophers wrote about lodestone It was later shown that the compass alignment was pro around 800 BC and its properties were known to the duced by a property of the Earth itself. -
Arizona Geological Society Digest, Volume VII, November 1964 35 VIRTUAL GEOMAGNETIC POLE POSITIONS for NORTH AMERICA and THEIR SUGGESTED PALEOLATITUDES by R
Arizona Geological Society Digest, Volume VII, November 1964 35 VIRTUAL GEOMAGNETIC POLE POSITIONS FOR NORTH AMERICA AND THEIR SUGGESTED PALEOLATITUDES By R. L. DuBois Department of Geology, University of Arizona, Tucson, Arizona ABSTRACT A virtual geomagnetic polar wandering curve obtained from paleomag netic results from North America places the North Pole in the central United States in Precambrian time. The curve shows polar movement from there to a mid-Pacific position near the equator during late Precambrian time and then northward to Japan and Siberia during Paleozoic time and finally to its present position during Mesozoic and Tertiary time. Using virtual geomagnetic poles as a guide, paleolatitudes are constructed for various periods of geological time. The central North American continent occupies a near-equatorial posi tion for most of Paleozoic time. It was in high latitudes during Precambrian time and similar latitudes to present ones since mid-Tertiary. INTRODUCTION It is the purpose of this paper to describe the location of virtual geo magnetic poles as determined from paleomagnetic observations on rocks of various geological ages in North America. The results are presented as a curve that depicts a path of relative movement of the geomagnetic pole or con tinental mass with regard to time. It is impossible, with data from a single continent, to relate the relative movement to either individual polar shift or continental drift or to a combination of the two. If the pole is selected as a reference, the movement is continental; whereas, if the continent is chosen as a reference, the movement is polar. Axelrod (1963) has concluded that paleo botanical data opposes continental drift, but this evidence is essentially in con cord with the polar wandering data of this paper. -
Paleomagnetic Stability
Paleomagnetism: Chapter 5 81 PALEOMAGNETIC STABILITY With the background information gained to this point, you appreciate the importance of isolating the charac- teristic NRM by selective removal of the secondary NRM. Theory and application of paleomagnetic stability tests are introduced here. Partial demagnetization experiments are performed in the laboratory to isolate the ChRM. Although sometimes mistaken as “magic,” these laboratory procedures are well grounded in rock magnetism theory. Field tests of paleomagnetic stability can sometimes provide crucial information about the age of a ChRM, and this question is often at the heart of paleomagnetic investigations. Lack of background in paleomagnetic stability tests often prevents interested earth scientists from understanding paleomagnetism. The material in this chapter should largely remove this obstacle. If not a “Big Enchilada,” this chapter certainly qualifies as a “Burro Grande.” PARTIAL DEMAGNETIZATION TECHNIQUES Theory and application of alternating-field and thermal demagnetization are introduced in this section. Al- though a central part of paleomagnetic investigations for some time, analysis of partial demagnetization data has become more sophisticated because of widespread availability of microcomputer systems for data analysis. Understanding modern paleomagnetism requires some familiarity with the analytical techniques that are used to decipher potentially complex, multicomponent NRM. To put the theory and techniques into practice, this section concludes with some practical examples. Theory of alternating-field demagnetization The fundamental AF demagnetization procedure is to expose a specimen to an alternating magnetic field. The waveform of the alternating magnetic field is a sinusoid with linear decrease in magnitude with time. Maximum value of this AF demagnetizing field can be labeled HAF and the waveform is schematically represented in Figure 5.1a. -
Xuan Et Al QSR 2012
Quaternary Science Reviews 32 (2012) 48e63 Contents lists available at SciVerse ScienceDirect Quaternary Science Reviews journal homepage: www.elsevier.com/locate/quascirev Paleomagnetism of Quaternary sediments from Lomonosov Ridge and Yermak Plateau: implications for age models in the Arctic Ocean Chuang Xuan a,*, James E.T. Channell a, Leonid Polyak b, Dennis A. Darby c a Department of Geological Sciences, University of Florida, 241 Williamson Hall, P.O. Box 112120, Gainesville, FL 32611, USA b Byrd Polar Research Center, Ohio State University, Columbus, OH 43210, USA c Department of Ocean, Earth, and Atmospheric Sciences, Old Dominion University, Norfolk, VA 23529, USA article info abstract Article history: Inclination patterns of natural remanent magnetization (NRM) in Quaternary sediment cores from the Received 2 February 2011 Arctic Ocean have been widely used for stratigraphic correlation and the construction of age models, Received in revised form however, shallow and negative NRM inclinations in sediments deposited during the Brunhes Chron in 15 November 2011 the Arctic Ocean appear to have a partly diagenetic origin. Rock magnetic and mineralogical studies Accepted 17 November 2011 demonstrate the presence of titanomagnetite and titanomaghemite. Thermal demagnetization of the Available online 10 December 2011 NRM indicates that shallow and negative inclination components are largely “unblocked” below w300 C, consistent with a titanomaghemite remanence carrier. Following earlier studies on the Men- Keywords: e Lomonosov Ridge deleev Alpha Ridge, shallow and negative NRM inclination intervals in cores from the Lomonosov Ridge Yermak Plateau and Yermak Plateau are attributed to partial self-reversed chemical remanent magnetization (CRM) Magnetic excursions carried by titanomaghemite formed during seafloor oxidation of host (detrital) titanomagnetite grains.