Lecture 4. Things we might want to know about the geomagnetic field. Components of the geomagnetic field. The geomagnetic reference field

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Lecture 4 Things we might want to know about the geomagnetic field Components of the geomagnetic field The geomagnetic reference field All sorts of magnetic poles observables

Things we might want to know Where does the field come from? How long has it existed? What is its average strength and how does it vary? What can it tell us about processes in the deep Earth?

How can we study the magnetic field? Direct observations (satellites, ground based observatories, other human measurements [captain s logs ]) Numerical simulation (e.g., Glatzmaier & Roberts, 1995) and laboratory dynamos (e.g., Aurnou and friends) Indirect records (archaeological and geological)

1st century CE???? Perigrinus 1269 CE Direct observations go back a long way!

Studies of a lodestone ball or terrella Gilbert (1544-1603) N Q Axis Orbis Virtutis The field of a magnetic dipole The Earth itself is a great magnet!

We may see how far from unproductive magnetick philosophy is, how agreeable, how helpful, how divine! Sailors when tossed about on the waves with continuous cloudy weather, and unable by means of the celestial luminaries to learn anything about the place or the region in which they are, with a very slight effort and with a small instrument are comforted, and learn the latitude of the place. Gilbert 1600

Uses of the bar magnet hypothesis Sailors can learn their latitudes (not very accurately) by measuring dip of the field. Geologists can learn the latitude of rocks at their birth and track the movements of the continents through time. example is: shallow dip in sea-level glacial deposits used to support snow ball earth hypothesis.

Geocentric Axial Dipole (GAD); D=0 The intensity of the field is twice as strong in the polar than in the equator The inclination varies as a function of latitude from 0- at equator to vertical at poles

Lecture 4 Things we might want to know about the geomagnetic field Components of the geomagnetic field The geomagnetic reference field All sorts of magnetic poles observables

But the field is more complicated than that Magnetic North B H I B v B Down P m Geographic North D Magnetic North B v P B N B E Down B H B I East can convert between D,I B and N,E,V with trig (see Lecture 3 and Chapter 2)

Recall from the last lecture: A magnetic field (H) is the gradient of a magnetic potential: simplest case: H = r m m = m r 4 r 3 = m cos 4 r 2 So, knowing m, we can evaluate H anywhere and vice versa H r = H = @ m @r = 1 4 1 r @ m @ 2m cos r 3 = m sin 4 r 3 H m θ r P H θ

The real field is sum of dipole plus a lot of more complicated fields: dipole octupole quadrupole

dipole potential: more general case: dipole P 1 0 octupole P 3 0 P l m P 2 0 quadrupole Colatitude (θ)

Dipolar field and potential 20 10 0-10 -20 80 60 40 20 0-20 -40-60 -80

Quadrupolar field and potential 10 5 0-5 -10-15 -20-25 80 60 40 20 0-20 -40-60 -80

Octupolar field and potential 20 10 0-10 -20 80 60 40 20 0-20 -40-60 -80

m (r,, )= a µ o 1 X Geomagnetic potential: l=1 lx m=0 a r l+1 P m l (cos )(g m l cos m + h m l sin m ) So, we need a whole list of numbers g m l and h m l (International Geomagnetic Reference Fields - IGRF) hese are best-fits from the observations for a given year. These lists allow us to predict the geomagnetic field vector at any point outside the core

Lecture 4 Things we might want to know about the geomagnetic field Components of the geomagnetic field The geomagnetic reference field All sorts of magnetic poles observables

Getting a reference field model Make a bunch of measurements of the geomagnetic field vector all over the world Find the best-fit coefficients to a special equation (the geomagnetic potential equation) These coefficients are the international geomagnetic reference field Can calculate the geomagnetic field vector ANYWHERE outside the source (the core) 21

geomagnetic observatories and satellites Observatories since 1800s; IGRFs since 1900

current version is IGRF-12 Thebault et al. (2015): dx.doi.org/10.1186/s40623-015-0228-9 online calculator: http://www.ngdc.noaa.gov/iaga/vmod/igrf.html

B Inc Still has increase in B towards the pole and change in inc with latitude, but more complicated 90% dipolar though!

Different projections of the same thing - IGRF 2005 Magnetic field lines 800 700 600 500 400 300 200 100 65 60 55 50 45 40 35 30 25 strength at the CMB strength at the surface

1900 2005 Secular variation 70 65 60 55 50 45 40 35 30 65 60 55 50 45 40 35 30 25 DIPOLE STRENGTH (nt) YEAR 8% drop over last century

Lecture 4 Things we might want to know about the geomagnetic field Components of the geomagnetic field The geomagnetic reference field All sorts of magnetic poles observables

Our first three poles (more to come) Geographic Magnetic Geomagnetic geographic: spin axis (the GAD pokes out here) magnetic: places where field is vertical geomagnetic: piercing points of best-fit dipole

Lecture 4 Things we might want to know about the geomagnetic field Components of the geomagnetic field The geomagnetic reference field All sorts of magnetic poles observables

80 60 40 20 0-20 -40-60 -80 Declination and inclination observed around the globe and plotted on equal area projection You will do something like this for problems 2.1 & 2.2 in your assignment

80 60 40 20 0-20 -40-60 -80 evaluate the field vector at these points λ

Lecture 4 Things we might want to know about the geomagnetic field Components of the geomagnetic field The geomagnetic reference field All sorts of magnetic poles: 2 more! observables

But first: a math refresher spherical trigonometry A law of sines: sin sin a = sin sin b = sin sin c B c β α a γ b C B r A c law of cosines: cos a = cos b cos c +sinb sin c cos

another pole a) N Virtual Dipole Moment (Am 2 ) Virtual Geomagnetic P Pole (λ p,φ p ) S (λ s,φ s ) b) S φ s θ s N φ D φ p θ m θ p P } } λ p λ s µt c) 55 d) 50 45 S( λ s, φ s ) 40 35 30 Virtual Axial Dipole Moment (Am 2 ) Essentials: Chapter 2

The last pole! When you average a bunch of poles together (to average out secular variation), you get one more pole a Paleomagnetic Pole. This is assumed to be equivalent to GAD: aligned with the spin axis and centered in the earth. Can you these poles to calculate paleolatitude, e.g.

Assignment Make sure you have properly installed PmagPy (now you need it!). Follow the instructions in the cookbook for moving the data_files directory to your Homework folder Do problems 2.1 and 2.2 in the online version of the textbook.