Title: Gravity
1Gravity
- (or, lies my physics class told me about physical
contants)
2Couple of things
- Problem sets are due today.
- Lectures on web.
- AWOL papers.
- February 12 (and maybe part 19) Gravity
- February 19 Magnetics (problem set)
- February 26 Examples (combined data sets).
- February 26 Maps to 2-credit people.
- April 1 Papers due, 2-credit people.
3What physics 101 says
All objects falling toward the Earth have the
same acceleration (free-fall) (neglecting air
resistance). Weight (w) mass x gravity. Physics
says g 9.81 N/kg 9.81 m/s2 (a constant).
A good approximation and O.K. for physics
problems, but NOOOOOOOO!
4What geologists say
- Gravity varies from location to location on the
Earth! - Varies inversely with the square of distance
from the center of the Earth (objects weigh
slightly less at high altitudes than at sea
level) (goes as r2) - Varies with latitude (Earth is not precisely
spherical is flattened at the poles) - Varies with subsurface geology
5How does gravity help in geology?
- Bathymetry, sidescan surface observations.
- Gravity subsurface.
- Density mass/volume.
- Look at relative density contrasts between
subsurface geological bodies .
6Density of Earth materials
Material Density (g/cm3)
Air 0
Water 1
Sediment 1.7-2.3
Sandstone 2.0-2.6
Shale 2.0-2.7
Limestone 2.5-2.8
Granite 2.7-3.1
Basalt 2.6-3.0
7Caveat Emptor
- Note that theres a lot of overlap in densities
of Earth materials. - Cannot use gravity to uniquely identify rock
formations (dont know absolute magnitudes,
either -- just relative densities). - Must use other geological information
(identification, geological context, etc.).
8Caveat Emptor
- But -- the measured gravity profile can be used
to model the shape of the subsurface density
anomaly. - Buried sphere, buried cylinder, infinitely long
sheet, infinitely long line.
9Gravimeter
Gravimeter gravity meter Two kinds Land and
air/sea Air/sea built on gyroscope to keep
instrument stable Measures SMALL, relative
variations in the Earths gravity field.
10Gravimeter
11Gravimeter measurements
Hang a mass on a spring --gt force of gravity will
stretch spring a distance x that is proportional
to the gravitational force. Gravitational
acceleration g (Gm)/r2 x (mg)/k, where h is
spring constant (describes stiffness of spring)
12Gravity units
Land gravimeter precision 1 part in 100
million 1 milligal 1 x 10-5 m/s2 Land
gravimeter precision 0.01 mgal Marine
gravimeter precision few mgal Marine seafloor
features tens to hundreds of milligals
13Correcting gravity
Terrestrial
14Correcting gravity
- Instrument drift (systematic changes in absolute
value of measurements over time). Fit straight
line. - Latitude effects (Earth is an oblate spheroid.)
Reference acceleration of gravity - go 978.03185 (1.0 0.005278895
sin2(lat) - 0.000023462 sin4(lat)),
cm/s2
15Correcting gravity
- Elevation. Correction for taking measurements at
different altitudes - gh (2hgo)/ro, where go reference
(latitude-corrected gravity), and ro Earths
radius. - Elevation correction at 1 km 3.08 mm/s2
(0.308 mgal per meter of elevation change). - Free-air correction.
- Corrected gravity free-air anomaly (gfa).
- gfa gmeasured - go - gh.
16Correcting gravity
- Bouguer correction
- Corrects for excess mass underlying
observation points that were higher than the
observation datum (or conversely). - gb 2 pi G pc h, where G
gravitational constant, pc density of
underlying rocks (2.67 g/cm3), and h
observation height. - Bouguer gravity gobserved - go - gh - gb
17Correcting gravity
- Terrain correction
- Accounts for variations in local gravitational
field caused by topography. Usually used only in
areas of steep terrain, or where defined regional
gradient exists. - Terrain correction (gtc) ad hoc function
defined by researcher - Residual gravity gobserved - go - gh - gb -
gtc
18Example from Sebago pluton, ME
19Correcting gravity
Marine
20Marine gravity
To first order, marine gravity looks like
bathymetry. Marine gravity is poor mans
bathymetry. Ship --gt marine gravity measured at
sea surface. Sea surface equipotential surface
(elevation datum everywhere equals 0). No height
corrections necessary. Gravity measured on ship
free-air gravity. Do correct for known or
calculable subsurface effects.
21AtlanticBathymetry
22Bathymetry
23Gravity
24Satellite gravity
ERS-1
Geosat
Geosat data was classified by the military until
1995, when the European ERS-1 data (of comparable
quality) was released.
25Ship vs satellite
Test accuracy of satellite-derived gravity by
comparing to shiptrack measurements. RMS
(root-mean-square, a way of quantifying error) is
about 3 mgal when shiptrack is along altimeter
profile. Away from altimeter profile, 4-7
mgal. Satellite gravity is less accurate near
shelf areas and near coasts (because of tidal
effects). Shiptrack and satellite data are
coherent down to wavelengths of 25-30 km.
26Global satellite-derived gravity
27Marine gravity corrections
Great, got free-air everywhere. What do you do
with it?
28Marine gravity corrections
Free-air (FAA) measured gravity at sea
surface. Want to know whats going on in
subsurface. Subtract from FAA the gravitational
signal of a model oceanic crust (6 km thick, with
assumed density, whose shape follows seafloor
topography). Result Mantle Bouguer anomaly
(MBA) MBA reflects subsurface density variations
due to (1) crustal thickness variations, (2)
mantle temperature variations, and (3)
lithospheric cooling. Lithospheric cooling
Plates diverge away from ridge axis, cooling as
they go. Cooling --gt lower density --gt lower
gravity. Cooling is a function of lithospheric
age. Know lithospheric age --gt can calculate
lithospheric cooling --gt can calculate
gravitational signal of lithospheric
cooling. Subtract gravitational signal of
lithospheric cooling from MBA. Result Residual
mantle Bouguer anomaly (RMBA)
29Marine gravity corrections
Example Southwest Indian Ridge (SWIR) Will mail
out PDF of Georgen et al. (gravity variations
near hotspots along the SWIR). Another reading
Turcotte and Schubert, chapter 5 (outside office
tonight).