the earth's magnetic field the earth's magnetic field

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1 EPS 122: Lecture 5 – Earth’s magnetic field The Earth’s magnetic field Reading: Fowler Ch 3, p43-51 (and Appendix 1) EPS 122: Lecture 5 – Earth’s magnetic field The Earth’s magnetic field …almost a dipole Field would be vertical at the poles horizontal at the equator But is oriented 11.5° from the rotation axis (which is geographical north)

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Page 1: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

The Earth’s magnetic field Reading: Fowler Ch 3, p43-51 (and Appendix 1)

EPS 122: Lecture 5 – Earth’s magnetic field

The Earth’s magnetic field …almost a dipole

Field would be • vertical at the poles • horizontal at the

equator

But is oriented 11.5° from the rotation axis (which is geographical

north)

Page 2: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

Describing the field

Declination (D) Inclination (I) Horizontal Intensity (H)

Vertical Intensity (Z) North-South Intensity (X) East-West Intensity (Y) Total Intensity (F)

EPS 122: Lecture 5 – Earth’s magnetic field

The Earth’s magnetic field

Page 3: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

The Earth’s magnetic field

EPS 122: Lecture 5 – Earth’s magnetic field

Describing the Earth’s field the best fit dipole

Magnetic potential

The Earth’s best fit dipole moment, m = 7.94x1022 Am2

Magnetic field is the derivative of the potential

given the magnetic permeability of free space, μ0 = 4 x10-7 kg m A-2 s-2

dot or scalar product

This first order simple model/description of the field allows use of paleomagnetic observations to determine past plate motions

Page 4: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

Spherical polar coordinates north pole R radius

colatitude, 0 to pi

(degrees from north pole)

longitude, 0 to 2pi

Conversion from/to Cartesian coordinates

Gradient operator

EPS 122: Lecture 5 – Earth’s magnetic field

Describing the Earth’s field the best fit dipole

Magnetic field in spherical polar coordinates

the radial, southerly, easterly components

If the Earth’s magnetic dipole moment is aligned along the z-axis:

we can calculate the magnetic field at any point….

Page 5: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

Describing the Earth’s field the best fit dipole

Total field

Three components

At the north pole At the equator Magnitude of the total field at the pole is twice as

strong as at the equator

EPS 122: Lecture 5 – Earth’s magnetic field

Describing the Earth’s field

3 x 10-5 T or 3000 nT at the equator

T is the teslas

6 x 10-5 T or 6000 nT at the poles

Page 6: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

The Earth’s magnetic field

…non-dipole field

EPS 122: Lecture 5 – Earth’s magnetic field

The Earth’s magnetic field

Best-fit dipole currently 11.5° from geographic north pole

But this has varied with time

Page 7: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

A few definitions

Declination (D) Inclination (I)

Horizontal Intensity (H) Vertical Intensity (Z)

North-South Intensity (X) East-West Intensity (Y)

Total Intensity (F)

for surface measurements

where is the magnetic latitude ( = 90 – )

magnetic inclination

EPS 122: Lecture 5 – Earth’s magnetic field

Secular variation …migration of magnetic north

Page 8: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

Secular variation …in observed declination

Declination in London

1500 2000

Declination at USGS Magnetic

Observatories 2000 1900

EPS 122: Lecture 5 – Earth’s magnetic field

Secular variation

Download: http://geomag.usgs.gov/movies/

Page 9: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

Secular variation

Download: http://geomag.usgs.gov/movies/

EPS 122: Lecture 5 – Earth’s magnetic field

Solar wind …and the Earth’s magnetic field

Bow sh

ock

Magnetopause Magnetosheath

Solar wind

The solar wind confines the Earth’s magnetic field to the magnetosphere

Page 10: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

The sunspot cycle

NASA - February 2001

• 11 year sunspot cycle

• Sunspots are intense magnetic loops which poke out of the photosphere

• Sun’s dipole flips at peak in sunspot

activity

• Last peak/flip: February 2001

• The magnetic south pole is now at the geographical north pole

and flips in the Sun’s magnetic field

• On Earth the field flips at intervals of ~200,000 years (5,000 to 50 mill)

• The last reversal on Earth happened 740,000 years ago

sunsp

ot

counts

X-ray image of the Sun

EPS 122: Lecture 5 – Earth’s magnetic field

The sunspot cycle and flips in the Sun’s magnetic field

• Meridional flows carry magnetic fields from mid-latitude sunspots to the Sun's poles

• The poles flip because south-pointing magnetic flux is transported to the north magnetic pole, and north-pointing flux to the south magnetic pole

NASA - February 2001

• Do we see evidence for this migration on Earth?

Page 11: The Earth's magnetic field The Earth's magnetic field

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EPS 122: Lecture 5 – Earth’s magnetic field

Space weather solar storms

Horizontal intensity at USGS Magnetic Observatories

120 0 Hours (12-16 March 1989

Earth for scale