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Application of modern geodetic<br />

measurements to the geophysics and<br />

Earth’s s environmental problem<br />

Tadahiro<br />

SATO<br />

National Astronomical Observatory of Japan


For the geosciences based on the<br />

data obtained from the modern geodetic<br />

measurements, GIA (Glacial<br />

Isostatic Adjustment)<br />

is important to study the Earth’s viscoelastic<br />

structure and dynamics, and the<br />

environmental problem of the Erath.


Following two topicst<br />

will be introduced;<br />

/ Experience at Ny-Ålesund<br />

lesund, , Svalbard in the<br />

Arctic,<br />

/ Japan–US joint observation project in<br />

Southern Alaska started in 2005**.<br />

**<br />

Abstract #053 of P41 by Freymueller et al.<br />

last day talk closely relates to the 2 nd topics.


Experience at Ny-Ålesund<br />

lesund,<br />

Svalbard in the Arctic<br />

(Sato et al., 2006, GJI, in press)


Geodetic observations at Ny-Ålesund<br />

AG: Absolute Gravimeter<br />

SG: Superconducting<br />

Gravimeter<br />

NALL & NAL1: GPS sites<br />

VLBI: VLBI site<br />

TG: Tide Gauge<br />

L&R: LaCoste & Romberg<br />

Gravimeter


Secular uplift rates at Ny-Ålesund<br />

(<strong>mm</strong>/<strong>yr</strong>)<br />

VLBI 4.8 (1.1)<br />

GPS (NYA1) 4.8 (1.5)*<br />

GPS (NALL) 5.3 (0.9)*<br />

Tide Gauge 5.2 (0.3)**<br />

----------------------------------<br />

Mean 5.2 (0.6)<br />

The GPS solutions derived by<br />

Heflin (2004).<br />

* The GPS rates shown here are corrected<br />

for a GPS scale rate error of +1.6 <strong>mm</strong>/<strong>yr</strong> to<br />

the VLBI rate, which was found from a<br />

comparison between VLBI and GPS at the 30<br />

collocation sites in the world.<br />

** Assumed 1.7 <strong>mm</strong>/<strong>yr</strong> as a rate of global<br />

secular sea level change


Absolute gravity observations<br />

• Rate: -2.5+/ 2.5+/-0.9<br />

μGal/<strong>yr</strong><br />

AG measurement in 2002 carried<br />

out by the Luxembourg group.


Predicted PGR (Post Glacial Rebound) :<br />

no more than 2-32<br />

3 <strong>mm</strong>/<strong>yr</strong><br />

Observed uplift rates:<br />

5.2+/-0.6 <strong>mm</strong>/<strong>yr</strong><br />

**Observation is two times larger than the<br />

proposed model results for the PGR effect.<br />

References: Lambeck 1995; Kaufmann & Wolf 1996;<br />

Kaufmann & Wu 1998; Scherneck et al. . 2002.


Possible origins that we studied;<br />

(1) Effect of the secular sea level (SSL(<br />

SSL)<br />

of a few 10 years in the oceans of the<br />

northern part of Europe,<br />

(2) Effect of the present-day ice melting<br />

(PDIM),<br />

(3) Effect of the ambiguity in the modeling<br />

of PGR.


Computation of the PDIM effect<br />

Method:<br />

Convolution of the changing<br />

mass with the loading Green’s<br />

function (for the PREM earth<br />

model) over the main 16 glaciers<br />

approximated their shape with<br />

elliptical cylinder.<br />

Results:<br />

Uplift: 2.04 <strong>mm</strong>/<strong>yr</strong><br />

Gravity: -0.53<br />

μGal/<strong>yr</strong><br />

SVAL model by<br />

Hagedoorn & Wolf<br />

(2003)<br />

For a mean melting rate of -45 cm/<strong>yr</strong><br />

over Svalbard that was inferred from<br />

glaciology data.


Sensitivity test of the PGR rate<br />

Large ice model<br />

● : ARC3+ANT4<br />

▼ : ICE-3G (large ice model)<br />

Small ice model:<br />

○ : ANU+ANT4<br />

Computed by Okuno


Comparison between the observation and the prediction<br />

• Displacement<br />

NS EW Vertical<br />

Gravity<br />

(<strong>mm</strong>/<strong>yr</strong>) (<strong>mm</strong>/<strong>yr</strong>) (<strong>mm</strong>/<strong>yr</strong>) (μGal(<br />

Gal/<strong>yr</strong>)<br />

Observation Mean 0.1 (0.4) -1.8 (0.4) 5.2 (0.6) -2.5 (0.9)<br />

Corrections<br />

1. RSL 0.00 -0.01 0.12 -0.04<br />

2. PDIM SVAL model 0.05 -0.83 2.04 -0.53<br />

3. PGR ANU+ANT4 0.53 -0.71 1.18 -0.33<br />

ARC3+ANT4 1.30 -2.98 1.46 -0.29<br />

ICE-3G<br />

1.16 -2.43 1.88 -0.31<br />

Sum of the corrections<br />

ANU+ANT4 0.58 -1.54 3.33 -0.88<br />

ARC3+ANT4 1.35 -3.82<br />

3.61 -0.84<br />

ICE-3G<br />

1.21 -3.26 4.03 -0.86


A geophysical interpretation<br />

Assumed melting rate vs Estimated PDIM effect


Su<strong>mm</strong>ary<br />

Both the observed uplift and gravity rates at Ny-Ålesund<br />

are larger than that expected from the PGR effects.<br />

Our study indicates;<br />

(1) Relative sea level (RSL) changes:<br />

not major origin<br />

(2) Present-day ice melting (PDIM):<br />

If the recent ice melting rate increases, it can be<br />

a strong candidate to explain the difference between the t<br />

observed ed rates and the predicted ones.<br />

(3) Ambiguity of the computation of PGR effect:<br />

Computation is sensitive to both the ice mode and Earth’s<br />

structural parameters.<br />

At Ny-Ålesund<br />

lesund, the horizontal rates are useful to<br />

constrain the discussion of the vertical rate of the PGR.


Japan–US joint observation project<br />

Period: 2005-2008<br />

2008<br />

in Southern Alaska<br />

Leaders:<br />

S. Miura (Tohoku Univ.)<br />

J. T. Freymueller (Univ. Alaska, Fairbanks)<br />

Members:<br />

T. Sato (NAOJ),<br />

H. Fujimoto (Tohoku Univ.),<br />

Y. Miyagi, M. Kasahara, , H. Takahashi (Hokkaido Univ.),<br />

T. Sugano, W. Sun, J. Okuno (ERI, Univ. Tokyo),<br />

C. F. Larsen, R. Motyka (Univ. Alaska, Fairbanks) .


Glacier Bay in Southern Alaska<br />

60N<br />

160W<br />

140W<br />

after C. Larsen (2002)


Rapid Uplift Rate Observed in Southern Alaska<br />

GPS and tide gauges give consistent uplift rates each other.<br />

after Larsen, C. F. et al., 2004 and 2005


Intensive GIA study was done in this area<br />

by University of Alaska, Fairbanks<br />

C.. F. Larsen, R. J. Motyka, , J. T. Freymueller,<br />

K. A. Echelmeyer and E. R. Ivins,<br />

Rapid uplift of southern 1118, Alaska caused by recent ice<br />

loss,<br />

Geophys. . J. Int., (2004) Vol. 158, P.<br />

C. F. Larsen, R. J. Motyka, , J. T. Freymueller,<br />

K. A. Echelmeyer, , E. R. Ivins<br />

Rapid viscoelastic uplift in southeast Alaska caused<br />

by post-Little Ice Age glacial retreat,<br />

EPSL, (2005) 237, p. 548


Su<strong>mm</strong>ary of the study by Alaskan group<br />

1. Large uplift rates: 30 <strong>mm</strong>/<strong>yr</strong> at the maximum.<br />

2. The observed rapid rates may not explain from the<br />

tectonic rate.<br />

3. The uplift pattern estimated from the GPS and TG data is<br />

consistent each other in general.<br />

4. A two-layer<br />

viscoelastic model (i.e. Elastic crust and Low<br />

viscosity half-space mantle) is not adequate to explain all<br />

three data sets of the GPS, TG and raised shore line.<br />

Three-layer<br />

viscoelastic earth model (i.e.<br />

Elastic<br />

lithosphere,<br />

low-viscosity<br />

athenosphere and<br />

high-<br />

viscosity lower mantle) is favorable to explain<br />

consistently all three data sets.<br />

5. For the observed viscous motion to the long-term forcing,<br />

there is a possibility that the effect of post-Little Ice Age<br />

contributes.


Subjects in the project<br />

1. Which global past-ice model among those now<br />

proposed is the best to explain the data obtained in<br />

Southern Alaska<br />

2. What is the best combination of the viscoelastic<br />

structural parameters for the study area<br />

3. How we can precisely separate two contributions<br />

from the past-ice and from the present-day ice<br />

These questions are closely linked each other.


GPS measurements<br />

100 km<br />

after C. F. Larsen (2003)<br />

45 Sites<br />

Red: good data<br />

Blue: need to be visited again


Collocation observation of GPS and gravity<br />

• By collocating the position and gravity measurements.<br />

we have an opportunity to discuss the elastic and<br />

viscous problems separately (Wahr(<br />

et al. . ,1995)<br />

Key numbers;<br />

+6.5 <strong>mm</strong>/μGal<br />

Gal: : a ratio of the viscous displacement<br />

to the viscous gravity change due to<br />

the mass redistribution in the mantle.<br />

-0.3<br />

μGal/<strong>mm</strong>: Free-air gravity change<br />

-0.15<br />

μGal/<strong>mm</strong><br />

(i.e. -0.3+1/6.5):<br />

viscous gravity rate


Observation and study in this project<br />

1. Observation<br />

/ GPS:<br />

Survey at some sites which are suggested to visit again<br />

from the previous observations<br />

Continuous observations<br />

/ Absolute<br />

and relative gravity measurements<br />

Gravity measurements with FG5 absolute gravimeter<br />

Continuous observation of the gravity tide<br />

2. Modeling<br />

/ Modeling of PGR & PDIM<br />

/ Improving the ocean tide model around the field<br />

/ Application of GRACE data to this area by increasing<br />

the spatial resolution of the analysis


Observation plan<br />

● AG, ○ Tidal Gravity, ●, Continuous GPS, ● GPS survey


Absolute gravityg<br />

measurement in Southern Alaska


Results of the AG measurement in 1987<br />

9.81832420 (±2.8 Gal)<br />

Sasagawa et al. (1989)<br />

Expected gravity change:<br />

δh = 18*(2006-1987)<br />

= 342 <strong>mm</strong><br />

δg = -0.2*342<br />

= 68 μGal at least


Tide Gauge Stations<br />

100 km<br />

after C. F. Larsen (2003)<br />

20 sites<br />

Black: Permanent site


Effect of the Ocean tide in Southern Alaska (SA)<br />

The ocean tide in SA is very large. Moreover, SA is a place at<br />

where the accuracy of the modern ocean tide models are low,<br />

i.e. difference among the models are large.<br />

This is a reason why we do the observation of gravity tide in<br />

SA.<br />

Ny-Ålesund<br />

1<strong>yr</strong><br />

Ocean (cm) 6.1<br />

Vertical (<strong>mm</strong>) 3.1<br />

Gravity (μGal) 1.2<br />

8 m<br />

Alaska<br />

Ocean (cm) 39<br />

Vertical (<strong>mm</strong>) 18<br />

Gravity (μGal) 6


Su<strong>mm</strong>ary<br />

/ Experiences in Svalbard and Southern Alaska<br />

introduced here also show that the modern<br />

geodetic measurements are worth very much<br />

not only the GIA problem but also a tool to<br />

consider the Earth’s s environmental problem via<br />

the present-day ice melting.<br />

/ Experiences in Ny-Ålesund<br />

suggest that the<br />

horizontal displacements are important to<br />

constrain the ice problem, especially for an area<br />

which locates at an edge of past- or present-<br />

day ice sheets.<br />

/ GRACE data may help to determine the low-<br />

order gravity changes and its results should be<br />

used by combing with the data from the ground<br />

observations.


Thanks for your attention.


Observed displacement rates<br />

• NS EW Vertical<br />

• (<strong>mm</strong>/<strong>yr</strong>) (<strong>mm</strong>/<strong>yr</strong>) (<strong>mm</strong>/<strong>yr</strong>)<br />

• VLBI 14.4 (0.5) 10.3 (0.5) 5.1 (1.1)<br />

• 13.8 11.3 4.8<br />

• GPS (NYA1) 14.6 (0.6) 10.0 (0.6) 6.6 (1.5)<br />

• 13.8 10.7 6.4<br />

• GPS (NALL) 14.2 (0.5) 10.7 (0.5) 7.0 (0.9)<br />

• 13.5 11.4 6.9<br />

• NUVEL1A-NNR NNR 13.6 13.0 -------<br />

Note:<br />

The first line for the VLBI and GPS (Heflin, 2004) indicates rates given in an<br />

ITRF2000 frame. The second line indicates rates in a NNR-NUVEL-1A frame.

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