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Improving Borehole Optical Stratigraphy (BOS)
T.J. Fudge
Ben Smith
Ed Waddington
What is BOS?
Hawley, 2008
BOS measures brightness of borehole wall with depth
Annual Layers are Visible
Allows rapid determination of past accumulation rate
Ability to observe seasonal firn compaction
Hawley, 2005
Why is getting in situ grain size and density important?
Densification of Firn
Trapping of Air in Firn
What causes the variations in brightness?
Can the physical characteristics of the firn, such as grain size and density, be inferred from the brightness variations?
Modeling the cause of brightness variations
-Photons enter the firn and move by scattering. -Keeps track of scattering events and position photon exits firn
Examine the effects of changes in grain size and density by using a Monte-Carlo model that tracks photons
the mean distance a photon travels between scattering events
Scattering Length:
snowgrain
photon track
Fir
n s
urf
ace
Scattering length
snow
icescat
rL
3
2
radius of snow grain
scatscatscat
QrrnL
2)(1
snow n(r)4
3r3ice
Density of scatters (grains)
Scattering efficiency, ~2
Scattering length
snow
icescat
rL
3
2
radius of snow grain
scatscatscat
QrrnL
2)(1
snow n(r)4
3r3ice
Density of scatters (grains)
Scattering efficiency, ~2
Brightness Variations can be causedby either grain size or density changes
Fine GrainCoarse Grain
Spreading of Light due to Scattering Length Change
Grainsize also affects albedo, but does not dominate scattering length brightness effects.
Multiple bounces are required to get large enough brightness changes
One limitation is that measurements cannot be made on cores
101 102 103 104
10-5
10-4
10-3
Sin
gle
-sca
tter
coa
lbe
do
geometric mean grain size, m
more absorptionless
absorption
New Device
Emphasis on measuring grain size
Currently designed for cores
New Device
Two light sources of different wavelengths
Measures spreading of light
Yellow (590nm)
Near Infrared (950nm)
0 10 20 30 40 50 60 70 8010-8
10-7
10-6
10-5
10-4
10-3
10-2
10-1
10-210-3
10-410-5
Inte
nsit
y (a
rbit
rary
uni
ts)
Scattering Lengths
101 102 103 104
10-5
10-4
10-3
10-2
10-1
Sin
gle
-sca
tter
coa
lbe
do
geometric mean grain size, m
6 8 10 12 14 16 18 20 22 24 260
0.2
0.4
0.6
0.8
1.0
Returned Intensity at 57.54 meters
Distance from source (mm)
Non
-dim
ensi
onal
ized
Inte
nsity
Modeling Results
590nm
950nm
Preliminary Results from Summit Greenland Firn Core
Light Sourcesare located closestto pixel 62
Preliminary Results from Summit Greenland Firn Core
Layer counting suggests annual layer thicknesses of 17-40cmat this depth, with 3-4 years per meter
Light Sourcesare located closestto pixel 62
Conclusions
BOS brightness variations can be caused by either changes in density or grains size.
The measurement are insufficient to determine physical properties of the firn.
A new device using two separate wavelengths of light and simplifying the geometry of the measurement yields promising results for inferring grain size.