Geology 5660/6660 Applied Geophysics 28 Mar 2014 © A.R. Lowry 2014 For Mon 31 Mar: Burger 429-449 (§7.4–7.6) Last Time: Earth’s Main Magnetic Field Earth’s.

Slides:



Advertisements
Similar presentations
PHYSICS UNIT 8: MAGNETISM
Advertisements

30140 Geophysics Part 2: Solid Earth Physics
Chapter 28. Magnetic Field
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Geomagnetism (I).
Paleomagnetic Records: Discovery and Correlation Jeannie Bryson.
Ch 8 Magnetism.
Today’s Concept: Torques in Magnetic Fields
Solidified iron km ,00012,000 solid mantle Mg(Fe) silicates crust Rapidly convecting, electrically conducting, fluid iron The outer core:
Magnetic Field Physics 102 Professor Lee Carkner Lecture 17.
Geomagnetic field Inclination
Chapter 21.  Magnets, as you know, can exert forces on one another.  In electricity, we talk about negative and positive dipoles or charges.  In magnetism,
Magnetic Resonance Imaging Astounding. The MRI magnet and patient table The operator’s console.
Topic 6: Generators and Motors Science 9 with Mrs M Please take off your hats and hoods.
Magnetism Physical Science. What is a magnet?  2000 years ago the Greeks discovered a mineral that attracted things made of iron.  They named this mineral.
21.1 Magnets and Magnetic Fields
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics I tom.h.wilson Department of Geology and.
Electromagnetic Force
ASEN 5335 Aerospace Environments -- Geomagnetism 1 Geomagnetism Dipole Magnetic Field Geomagnetic Coordinates B-L Coordinate system L-Shells Paleomagnetism.
Geomagnetism: Earth’s magnetic field Dipole Field.
Magnetism Chapter 22.
Magnetism Chapter 24.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics I tom.h.wilson Department of Geology and.
Geomagnetism: Lecture 1 This lecture is based largely on:
© NERC All rights reserved UK Repeat Station Report T J G Shanahan and S Macmillan June 2009 MagNetE Workshop Helsinki, Finland.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Geomagnetism: Lecture 1 This lecture is based largely on:
Last Time: Magnetic Methods (Intro) Governed by Laplace’ eqn :  2 u = f (sources) Differs from gravity in that the source is a dipole rather than a monopole.
A horizontal copper loop is due east of, at the same elevation as, a straight horizontal wire carrying a steady current due north. What is the direction.
Earth’s Magnetic Poles
The link between electricity & magnetism N S When a wire moves through a magnetic field a voltage is produced N Moving a magnet moves through a coil of.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics I tom.h.wilson Department of Geology and.
Last Time: Gravity Modeling Gravitational attraction of an arbitrary body: Gravity anomaly due to a sphere: (represents only the vertical component of.
5. Magnetic forces on current l A Example: A straight wire carrying a current is placed in a region containing a magnetic field. The current flows in the.
Fluxgates By: Riley Vollmer. What a Fluxgate is 2 Ferromagnetic bars (Cores) 2 Ferromagnetic bars (Cores) Coils wound around Each core but in opposite.
5. Magnetic forces on current
Environmental and Exploration Geophysics I tom.h.wilson Department of Geology and Geography West Virginia University Morgantown,
Magnetic Fields and Electromagnetic Induction
Pearson Prentice Hall Physical Science: Concepts in Action Chapter 21 Magnetism.
Recall that the proton precession magnetometer makes measurements of the total field, not the vector components of the field. Recall also that the total.
Ch 8 Magnetism and Its Uses: Section 1 Magnetism A. Magnetism—the properties and interactions of magnets 1. Interaction between two magnets called magnetic.
Magnetism -the attraction of a magnet for another object -two magnets will either attract or repel each other -if the domain inside a magnet are aligned.
The Earth’s Magnetic Field
Geomagnetism Part II: The Earth’s Magnetic Field
Magnetism Chapter 36. Magnetic Poles ► Magnetic Poles – one of the regions on a magnet that produces magnetic forces ► The end of a magnet that points.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics I tom.h.wilson Department of Geology and.
Magnetic Fields. Magnetic Field of a bar magnet I. Field of a bar magnet The forces of repulsion and attraction in bar magnets are due to the magnetic.
Geology 5660/6660 Applied Geophysics 1 Apr 2016 © A.R. Lowry 2016 For Mon 4 Apr: Burger (§ ) Last Time: Magnetics (Measurement, Anomalies)
Environmental and Exploration Geophysics I tom.h.wilson Department of Geology and Geography West Virginia University Morgantown, WV.
Geology 5660/6660 Applied Geophysics 30 Mar 2016
Last Time: Magnetic Methods Intensity of induced magnetization by an external field is (where k is magnetic susceptibility ) Crustal minerals can be diamagnetic.
Chapter 19: Magnetic Forces and Fields
What is the magnetic potential of a dipole?
Magnetic method Magnetic force and field strength for pole strength m’ and m.
5. Magnetic forces on current
Geol 319: Important Dates Friday, Sept 28th – class cancelled
Predicting magnetic field variations
Prepared by Dedra Demaree, Georgetown University
Chapter 21: Magnetism Section 21.1 Magnets and Magnetic Fields
Chapter 21 Magnetism.
GG 450 February 19, 2008 Magnetic Anomalies.
Magnetic Field and Magnetic Forces
Magnets, Magnetism & Electromagnetism
Earth’s Magnetic Poles
A reminder about current
Magnets and Magnetic Fields
Preview Section 1 Magnets and Magnetism
5. Magnetic forces on current
Generating Electricity
Magnets and Magnetic Fields
Presentation transcript:

Geology 5660/6660 Applied Geophysics 28 Mar 2014 © A.R. Lowry 2014 For Mon 31 Mar: Burger (§7.4–7.6) Last Time: Earth’s Main Magnetic Field Earth’s Main Field derives from “core dynamo” … convective flow of Ni-Fe outer core + coriolis forces (  + feedback )  electrical current flow  magnetic field (  + feedback ) + single-crystal Fe inner core (  + feedback ) Mostly dipolar, oriented ~ (and precesses around) rotation axis; varies nonlinearly through time… Express the vector field at a point as either intensity H E, inclination i, declination or local H x, H y, H z components:

500 yrs before reversal mid-reversal500 yrs after reversal Glatzmeier modeling: Solid inner core magnetized opposite main field; forced to rotate by applied torque  precession (~0.2°/yr for real Earth) Inner core stabilizes field dipole; long time required to diffuse outer core field to inner core controls reversal timescale

Problem : If both Earth’s main field and crustal field are determined from surface measurements, how do we separate? Core field dominates long wavelengths (small n of spherical harmonics). We describe core field only out to n = 14–15 where it dominates the total field.

Measurement: Fluxgate magnetometer : Wire coils wound in opposite directions; these cancel & produce zero current in secondary coil in absence of external magnetic field, but if aligned with a field, one core reinforces, other counteracts external field resulting in a current. Gives intensity in the orientation of the coils. (Direction?)

Proton precession magnetometer : Bottle containing a hydrogen-rich fluid (distilled water or hydrocarbon) is surrounded by a wire coil. Current through the coil produces a strong magnetic field; protons align with field… Current is shut off & as protons realign with Earth’s magnetic field they precess at a frequency determined by magnetic field strength ( Hz/nT). So, measure frequency of the induced AC current and convert to a total field strength. (Lots of other types but these two are most commonly used for terrestrial geophysics!) Measurement:

Data Reduction: Remove/avoid all metal objects when collecting data!!! Keep magnetometer high off the ground to reduce “noise” Sensitive to variations in ionosphere, magnetosphere: Perform looping and correct for drift; don’t bother measuring during solar storms Correct for elevation if > a few hundred m (~0.03 nT/m) Horizontal position correction: Use WMM if latitude change is > a few hundred m (correction here ~6 nT/km) From ComponentField ValueSecular Variation Declination degrees -8.1 arcmin/year Inclination degrees -1.6 arcmin/year Horizontal Intensity10887 nT-15.8 nT/year North Component (x) nT -5.1 nT/year East Component (y) 4392 nT nT/year Vertical Intensity (z) nT nT/year Total Intensity nT-98.7 nT/year