http://www.redorbit.com/images/pic/29380/earths-magnetic-field/ The magnetic field and magnetic measurements Einar Ragnar Sigurðsson 27th November 2013 Slide no: Outline of presentation 1. The magnetic field of Earth: ▫ The dipole moment ▫ Reversals 2. The rock magnetization: Induced and remanent 3. The remanent magnetization such as TRM, DRM, VRM 4. Different methods for measuring the rock magnetization 5. The master’s thesis: Rock magnetization in Icelandic volcanic zone Einar Ragnar Sigurðsson - 27.11.2013 The Earth’s magnetic field during reversal. Ref: Glatzmaier, G.A. & Coe, R.S. (2007) Paleo-magnetism and magnetic measurements Slide no: 2 The magnetic field of Earth • Generated be an electric current in the liquid outer core. Magnetic dipole generated from current in a loop • The dipole magnetic moment can describe 80-90% of the magnetic field of Earth. • Now, there is a magnetic south pole in northern hemisphere and magnetic north pole in the south hemisphere. • Simplification since 10-20% is left and how the current actually is, is not well known (Kristjansson L., 1985) Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 3 The rotation axis of Earth and the magnetic dipole don’t fit -> Declination • Since the dipole doesn’t correspond to the geographical poles we get the declination and from the nature of the dipole moment we get inclination angle. ▫ B: The total magnetic field ▫ H: The horizontal component of the field ▫ Z: The vertical component of the field ▫ I: Inclination angle, the dip of the magnetic field ▫ D: Declination. The angle between the (true) geographical north and the magnetic north • (Kearey et al, 2002) Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 4 The IGRF11 model (NOAA – National Geophysical Data Center, 2013) Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 5 The unstable magnetic field • Diurnal variations • Source of change is solarwind and thunderstorms close to equator • Can disturb magnetic measurements but is also the key to some electromagnetic resistance measurements (MT measurements) • Secular variations • Slow changes with time, both in intensity and location of the poles • Source of change is assumed to be changes in the current generating the Earth magnetic field • Measurable through paleomagnetic measurements Einar Ragnar Sigurðsson - 27.11.2013 • Can led to reversals of the magnetic poles • Major time periods with the same direction of the magnetic field: - Brunhes: 0-0.78 Ma (normal) - Matuyama: 0.78-2.6 Ma (reversed) - Gauss: 2.6-3.6 Ma (normal) - Gilbert: 3.6-6.0 Ma (reversed) • Measurable through paleo-magnetic measurements Paleo-magnetism and magnetic measurements Slide no: 6 The geomagnetic reversal • During the geomagnetic reversals the dipole field wanders down to lower latitudes. • In same time it weakens a lot • Then it strengthens again when going to higher latitudes again finishing the reversal, if there is a reversal. • Based on number of lavas the dipole field is most often close to the true north and south. (Kristjánson, L) Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 7 The rock it self can be magnetized : Induced and remanent • The induced magnetization, Ji is induced by the present external magnetic force ▫ Is in same direction as the external field ▫ Ji depends on the material property called susceptibility (k) 𝐽𝑖 = 𝑘𝐻 ▫ Will disappear when external field is “turned off” • The remanent magnetization, Ji is not dependent on the present external magnetic field. It depends on: ▫ Properties of the material - the minerals ▫ The paleo-magnetic field from the time of formation and the rock and later as well ▫ It is permanent in the rock and the present external field doesn’t have any measurable effect on it. Einar Ragnar Sigurðsson - 27.11.2013 Vector diagram showing how an external magnetizing force H (that could be from the Earth magnetic field) induces a magnetic field Ji that is added to the remanent magnetic field Jr and hence giving the total magnetic field J. (Kearey et al, 2002) Paleo-magnetism and magnetic measurements Slide no: 8 The remanent magnetization Primary Secondary • Thermo Remanent Magnetization, TRM • Chemical Remanent Magnetization, CRM • In igneous rock that solidifies and cools through the Curie temperature • Magnetic minerals: • Magnetite (Fe3O4) • Ulvöspinel (Fe2TiO4) • Depositional Remanent Magnetization, DRM • magnetic particles are deposited by sedimentation and they align with the current magnetic field Einar Ragnar Sigurðsson - 27.11.2013 • Magnetic minerals recrystallize or grow during metamorphism • Viscous Remanent Magnetization, VRM • Remanent magnetism is acquired over time if a rock is subjected to an external field different from the original field • Isothermal Remanent Magnetization, IRM • The magnetization can changes in extremely high magnetic field such as from a lightning Paleo-magnetism and magnetic measurements Slide no: 9 Different kinds of magnetic measurements: Ground magnetic survey • Detailed survey of limited area • Measurement of magnetic field to find out residual magnetic field • Residual magnetic field anomalies are caused by different magnitude and/or direction of magnetization (remanent + induced) of objects. • The purpose is to locate and find out magnetic properties of hidden objects underground (Photo: Einar Ragnar Sigurðsson) Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements (Kearey et al, 2002) Slide no: 10 Different kinds of magnetic measurements: Aeromagnetic survey – Marine magnetic survey • Survey covering large area • Magnetic anomalies caused by different magnitude and/or direction of magnetization (remanent + induced) of objects. • The purpose is among other things mapping of magnetic anomaly pattern related to plate movements and magnetic reversals. Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 11 Different kinds of magnetic measurements: Susceptibility measurement of a sediment core • The method is convenient and nondestructive. • The core is put into a magnetic field and the induced magnetization in the core is measured. • The outcome of the measurement is the susceptibility of the material in the sediment core. • High susceptibility value as a material property may indicate: ▫ ▫ ▫ ▫ Particulate pollution Ancient forest fires Floods Bands of volcanic tephra • See graph from a 12m core piece of sediment in a lake in Washington State, U.S. Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 12 Measurements of remanent rock magnetization copyright of figure: Leó Kristjánsson • • • • • Sample (lava) from the field Preparation of the sample: Demagnetization of VRM Measurement in a laboratory Calclation of paleo-declination and inclination Paleo virtual dipole Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 13 Drilling: Taking the core • Originally a chain saw. • Made in USA • An exchangeable front end with industrial diamond crown • Can last for 100 lavas • Diameter 25mm • Approximately 1 minute to drill one core • Common to take have 4 samples for each lava • Unsuccessful drilling requires on average drilling 6 cores • Use of cooling water -> difficulties when temperature is below 0°C • 1 liter for one lava • Centrifugal coupling Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Photo: Einar Ragnar Sigurðsson Slide no: 14 The orientation of the core • Richard Doell method, 50 years old! • 1” tube and Brunton compass • The direction to the sun or other known place is taken with the compass ̵ Use of GPS if no such place • For orientation of the specimen: The upper top end of the core is marked with a wire. • Finally: Break the core from the lava Photos: Leó Kristjánsson and Einar Ragnar Sigurðsson Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 15 The core • Diameter 24.5 mm • Length originally ca 50 mm • Sawed to appropriate length to have the cylinder as symmetric as possible, that is a spear like cylinder with 𝐿 = 0.5𝐷 3 ≈ 21 𝑚𝑚 • Orientation of the specimen is very important: ̵ The z axis as the axis of the cylinder ̵ The y axis is perpendicular to the z axis and was horizontal in the original rock ̵ The x axis is perpendicular to the two other axis and sloping upwards 90° from the slope of the core Photos: Einar Ragnar Sigurðsson Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 16 The magnetic measurement • Measured in all possible directions and al orientations: ̵ In x, y, z direction ̵ Positive and negative direction ̵ For all four orientations ̵ Total: 3 x 2 x 4 = 24 measurements • The equipment is perpendicular to Earth magnetic field and as well surrounded with a coil to minimize the effect of external magnetic field. • Very old equipment from institute dr Förster in Germany ̵ Tube amplifier from 1978 and design from 1968! Photos: Einar Ragnar Sigurðsson and Leó Kristjánsson Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 17 The data processing • The output from the magnetometer is mV for all 24 measurements goes to a computer program, see figures. • Average for each of x, y and z • Inclination and declination of the specimen • 𝐴𝑚𝑝𝑙 = √(𝑥 2 + 𝑦 2 + 𝑧 2 ) • Calibrated with known coil (see the small figure) to change the measured amplitude in mV to the magnetization of the specimen in A/m (J0 in the figure) Photos: Einar Ragnar Sigurðsson Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 18 Demagnetization: “Washing” the specimen • The specimen is put in to a “magnetic washing machine” where the specimen is rotated for a short time in a strong magnetic field. • Rotated to get effect on the VRM in all possible directions Photos: Einar Ragnar Sigurðsson Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 19 The theory behind the magnetic field demagnetization Ref: Kristjansson, L., 1985 • The VRM is softer than TRM so it will disappear first in a strong external alternating magnetic field • Magnetic field goes up to strengths such as: 10-15-20-25-30-35 mT and down again • Note: 10 mT is approximately 200 times larger than magnetic field of the Earth • The washing is repeated until the change in declination and/or inclination goes down to 1 or 2° • Stop washing before all TRM has been washed out so there will be some magnetic field left for the final measurement Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 20 Some interesting points regarding the magnetic field demagnetization Ref: Kristjansson, L., 1985 • The first steps of washing can increase the dipole moment as for the GL lavas. • The washing will not have so much effects on lavas younger than 700 thousand years. • In that case both TRM and VRM are normal or positive magnetized • The washing will have very large effect on a 800 thousand years old lava. • That lava should have reversed TRM but most of the VRM is normal magnetized. Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 21 The master’s thesis • Measurements of rock magnetization inside the volcanic zones • Previous measurements mostly outside the volcanic zones ̵ Difficulties with hyaloclastite ̵ Difficulties with more complicated geology than flat lavas ̵ Recognizing the magnetic reversal important • Rock magnetization measurements in Icelandic table mountains • Find out changes in declination from the eruptions: ̵ In the pillow lava ̵ In the lavashield on top of the mountain ̵ For how long time was the eruption lasting? Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements (Náttúrufræðistofnun ísladns) Slide no: 22 History of magnetic field in Reykjavik 0 52500 -5 Declination [degrees] -15 51500 -20 51000 -25 Total magnetic field [nT] 52000 -10 -30 50500 Declination -35 Total Field -40 1900 50000 1910 1920 1930 1940 1950 1960 1970 1980 1990 2000 2010 Year Declination and total magnetic field in Reykjavik (# Latitude: 64.14 degrees North, Longitude: 21.9 degrees East) from 1900 in IGRF 11. Calculations from NOAA – National Geophysical Data Center web page. Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 23 Rock-magnetic measurements in table mountains Change of declination in China • Some disadvantages: ̵ Sometimes the declination can stay stable ̵ The declination goes up and down ̵ Not very precise – we need very long eruptions to see any change in declination (Merrill & McElhinny, 1983) • Has been done at least once in Iceland ̵ Hlöðufell south of Langjökull ̵ Did not show difference in declination Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 24 References • Glatzmaier, G.A. & Coe, R.S., 2007. Magnetic polarity reversals in the core. Treatise on Geophysics, Volume 8, Core Dynamics, Chp. 9, eds. P. Olson and G. Schubert (Elsevier), pp. 283-297. • Kearey, P., Brooks P.,Hill, I (2002). An Introduction to Geophisycal Exploration. Malden: Blackwell publishing. • Kristjansson L., 1985. Bergsegulmælingar – nytsöm tækni við jarðfræðikortlagningu. Náttúrufræðingurinn, 54 (3-4), p. 119-130 • Merrill, R.T. & McElhinny, M.W., 1983. Earth's Magnetic Field: Its History, Origin and Planetary Perspective (International Geophysics Series). Academic Press Inc • NOAA – National Geophysical Data Center, 2013. Magnetic Field Calculators, retrieved from http://www.ngdc.noaa.gov/geomag on 15.11.2013. Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 25 Alternative method for demagnetization • Heating the specimen to successively higher temperatures in zero field • Measure remanent magnetic field at room temperature after cooling in zero field • Disadvantages: ̵ The magnetic minerals are often altered during the heating. ̵ Time consuming • Advantages ̵ Works better on specimens from sedimentary rocks than demagnetization employing alternating field Einar Ragnar Sigurðsson - 27.11.2013 Photo: www.kochi-core.jp/en/facilities_and_equipment/magnetism.html Paleo-magnetism and magnetic measurements Slide no: 26 Other methods • The spinner magnetometer ̵ The specimen is rotated at constant rate by a motor, close to a pick-up coil or fluxgate probe. ̵ Electronic circuits are used to amplify only a signal of the same frequency as that of the rotation ̵ More time consuming method ̵ better result with weaker magnetization Photo showing a spinner • uperconducting quantum interference device (SQUID, cryogenic) magneto- meters ̵ Can be used for very weakly magnetic rocks, even limestones Photo showing SQUID equipment (ref www.kochi-core.jp/en/facilities_and_equipment/magnetism.html) Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 27 SQUID Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 28 Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 29 History of magnetic field in USA – Washington DC 0 Declination [degrees] -2 -4 -6 -8 -10 -12 1750 1800 1850 1900 1950 2000 Year Declination in Washington DC (# Latitude: 38.89 degrees North, Longitude: 76.59 degrees West) from 1900 in IGRF 11. Calculations from NOAA – National Geophysical Data Center web page. Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 30 History of magnetic field in China (Merril & McElhinny, 1983) Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 31 History of magnetic field in London Einar Ragnar Sigurðsson - 27.11.2013 Paleo-magnetism and magnetic measurements Slide no: 32
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