36 research outputs found
Maakoore vertikaalliikumised Eestis tรคppisnivelleerimiste andmetel
The aim of this study was to detect vertical crustal movements in Estonia and find out possible
changes of vertical crustal movements in time. Vertical velocities of the benchmarks were
calculated from the precise levellings between 1933 and 2011 of the Estonian levelling network
using the joint weighted kinematic least squares adjustment of the levelling campaigns. Two
different mathematical models, the โheights includedโ and the โheights eliminatedโ model, were
used in the adjustment. Different options of the computer software Surfer were used for modelling
of the vertical crustal movements. Accuracy of the models was estimated by finding differences
between the velocities interpolated from the models and adjusted vertical velocities of the
benchmarks, using the cross validation technique, and by comparing models with the results from
other geodetic measurements (continuously operating GNSS stations, tide gauges, other land uplift
models).
From the variance component estimation, it appeared that levelling errors of the First levelling
campaign were ~3 times larger than estimated a priori. Final adjustment was performed with the
re-scaled weights according to the results of the variance component estimation. Models of the
vertical crustal movements EST2013LU and EST2015LU were created based on the vertical
velocities of the benchmarks. According to the models, rates of the land uplift in Estonia range
from โ0.7 mm/yr in SE Estonia to +2.8 mm/yr in the island of Hiiumaa in NW Estonia. Accuracy
of the models was estimated to be ยฑ0.4 mm/yr on average. The comparison of the models with
the velocities from the independent measurement methods revealed best fit with the velocities of
the GNSS permanent stations where residual differences remained within ยฑ0.3 mm/yr on average.
The discrepancies between the velocities of the coastal tide gauges and the velocities from the
models were ยฑ0.7โฆยฑ1.0 mm/yr on average. Obtained differences implied to the systematic biases
in tide gauge velocities. Comparison with the historical vertical crustal movement maps of Estonia
showed that differences remained within ยฑ0.7 mm/yr on average. The fit between the most recent
Fennoscandian LU map NKG2005LU and the models obtained in the present study was very
good. Differences remained within ยฑ0.3 mm/yr on average. It appeared also that vertical velocity
of the benchmarks has been significantly changed between the levelling periods. Results of the
study can be used to estimate the risks to the coastal areas coming from the global warming related
rise of the sea level.Doktoritรถรถ eesmรคrk oli leida maakoore vertikaalliikumiste kiirused Eestis nelja
kordusnivelleerimise (1933-2011) andmete pรตhjal ja vรคlja selgitada reeperite kiiruste muutumine
ajas. Reeperite vertikaalliikumise kiirused leiti nivelleerimiste รผhisest kaalutud kinemaatilisest
tasandusest vรคhimruutude meetodil. Tasandusel kasutati kahte matemaatilist mudelit: nn
โkรตrgustegaโ ja โkรตrgustetaโ mudelit. Maakoore vertikaalliikumiste modelleerimiseks kasutati
tarkvara Surfer erinevaid vรตimalusi. Mudelite tรคpsust hinnati mudelist interpoleeritud ja reeperite
tasandatud kiiruste vaheliste erinevuste leidmise, ristvalideerimise ja sรตltumatute
mรตรตtmistulemustega (GNSS-pรผsijaamad, veemรตรตdujaamad, teised mudelid) vรตrdlemise teel.
Dispersioonikomponentide hindamisest selgus, et esimese nivelleerimiskampaania vead on ~3
korda suuremad kui a priori eeldati. Lรตplik tasandus teostati dispersioonikomponentide hindamise
tulemuste pรตhjal รผmberskaleeritud kaaludega. Reeperite kiiruste pรตhjal loodi Eesti maakoore
vertikaalliikumiste mudelid EST2013LU ja EST2015LU. Mudelite pรตhjal ulatuvad maatรตusu
kiirused Eestis alates โ0.7 mm/a Kagu-Eestis kuni +2.8 mm/a Hiiumaal. Mudelite tรคpsuseks
hinnati keskmiselt ยฑ0.4 mm/a. Vรตrdluses sรตltumatutest meetoditest mรครคratud maatรตusu kiirustega
selgus, et parim oli sobivus GNSS-pรผsijaamade kiirustega, keskmiselt ยฑ0.3 mm/a. Halvim oli
sobivus ranniku veemรตรตdujaamade kiirustega: ยฑ0.7โฆ.ยฑ1.0 mm/a. Saadud erinevused viitasid
sรผstemaatilistele nihetele veemรตรตdujaamade kiirustes. Vรตrdlus Eesti varasemate maakoore
vertikaalliikumiste kaartidega nรคitas, et erinevused jรคid keskmiselt ยฑ0.7 mm/a piiridesse. Mudelite
sobivus viimase Fennoskandia maatรตusu mudeliga NKG2005LU oli aga vรคga hea, erinevused jรคid
keskmiselt ยฑ0.3 mm/a piiridesse. Samuti selgus, et nivelleerimisperioodide vahel on reeperite kiirus
statistiliselt oluliselt muutunud. Uurimistรถรถ tulemusi saab kasutada kliimasoojenemisest tulenevate
meretรตusu riskide hindamiseks rannikualadel
Hydrocode modeling of oblique impacts into terrestrial planets
The abundance of moderately siderophile elements (โiron-lovingโ; e.g., Co, Ni) in the Earthโs mantle is 10 to 100 times larger than predicted by chemical equilibrium between silicate melt and iron at low pressure, but it does match expectation for equilibrium at high pressure and temperature. Recent studies of differentiated planetesimal impacts assume that planetesimal cores survive the impact intact as concentrated masses that passively settle from a zero initial velocity and undergo turbulent entrainment in a global magma ocean; under these conditions, cores greater than 10 km in diameter do not fully mix without a sufficiently deep magma ocean. I have performed hydrocode simulations that revise this assumption and yield a clearer picture of the impact process for differentiated planetesimals possessing iron cores with radius = 100 km that impact into magma oceans. The impact process strips away the silicate mantle of the planetesimal and then stretches the iron core, dispersing the liquid iron into a much larger volume of the underlying liquid silicate mantle. Lagrangian tracer particles track the initially intact iron core as the impact stretches and disperses the core. The final displacement distance of initially closest tracer pairs gives a metric of core stretching. The statistics of stretching imply mixing that separates the iron core into sheets, ligaments, and smaller fragments, on a scale of 10 km or less. The impact dispersed core fragments undergo further mixing through turbulent entrainment as the molten iron fragments sink through the magma ocean and settle deeper into the planet. My results thus support the idea that iron in the cores of even large differentiated planetesimals can chemically equilibrate deep in a terrestrial magma ocean.
The largest known impact on the Moon formed the South Pole-Aitken (SP-A) basin and excavated material as deep as the mantle. Here I suggest that large impacts eject enough material to cover the farside of the Moon. During the impact process, ejecta leave the crater and travel well beyond the transient crater. Ejecta blankets depend on impactor size and angle. I use iSALE, an impact hydrocode, to determine the ejecta distribution, volume, and thickness. I calculate the trajectory of ejecta that leave the crater and return to the lunar surface. In these simulations, an ejecta blanket forms, with a thickness of kilometers, over the lunar farside. The ejecta blanket thicknesses are comparable to the difference between nearside and farside crustal thickness. Previous studies suggest other possible mechanisms for the lunar farside-nearside dichotomy. However, the impact that formed SP-A basin was large enough to eject material onto the farside. I also suggest a differentiated impactorโs core would disperse downrange of the impact point underneath the basin.
Doublet craters form within crater rays on terrestrial bodies. The near simultaneous impact of two projectiles results in overlapping craters. This process results in modified crater morphologies and ejecta morphologies. I modeled the impact of two identical projectiles and vary the angle, timing, and initial separation distance. In this work, I identified projectiles with a separation distance of four times their initial diameter will form distinct craters, but the ejecta from the uprange crater will overfill the downrange crater and result in a smaller crater depth. This result implies the direction of the impactor may be inferred from the crater depths. Also, I found impacts that form closer together result in elliptical or dumbbell craters depending upon the impact parameters. The ejecta curtains interact in each simulation and result in structures similar to the V-shaped ridges or โherringboneโ patterns traversing clusters of secondary craters in observations. The ejecta that lands within the ridges comes from a depth that is 100 to 125 m for a 500 m impactor traveling at 1 km/s. This is less deep than the maximum excavation depth of 125 to 150 m, depending upon the impact angle. This work represents a first step towards a more comprehensive method for not only determining how doublet craters form and how aberrant craters form, such as Messier A on the Moon, but also determining how the regolith changes and the ejecta blanket forms for such impacts
MODELLING THE EARTH: COMPRESSIBLE VISCOELASTODYNAMICS, GRAVITATIONAL SEISMOLOGY AND TRUE POLAR WANDER
This thesis reviews and sheds new light on compressible Earth models and theories for the modelling of megathrust earthquakes and rotational instabilities caused by glacial isostatic adjustments and mantle convection. The basic theory is outlined in the first chapter, where we discuss the response of a self-gravitating Earth to external forces and loads seated at its surface or interior and we focus on elastic static perturbations and the transition between the elastic and fluid behaviours of the Earth that occurs on thousand and million years time scales.
In the first part of this thesis, we derive the analytical solution of the momentum and Poisson equations for a spherically symmetric viscoelastic Earth model that accounts for compressibility both at the initial state of hydrostatic equilibrium and during the perturbations. This constitutes a step ahead with respect to all previous analytical solutions, which actually neglect compressibility in some aspects, and allows to gain deep insight into the relaxation spectrum of compressible viscoelastic Earth models.
In the second part, we discuss long-wavelength gravity anomalies caused by the 2004 Sumatra earthquake and detected by the Gravity Recovery And Climate Experiment (GRACE) space mission. We extend the classic theory in order to interpret gravity anomalies in terms of volume changes within the solid Earth, advection of the initial density field and ocean water redistribution caused by perturbations of the ocean floor and surface topographies. This physics is then exploited in order to develop a novel procedure for the inversion of the principal seismic source parameters (hypocentre and moment tensor) of large earthquakes relying solely on space gravity data. This procedure, which complements traditional seismology and which we shall name Gravitational Centroid Moment Tensor (GCMT) analysis, is applied for the first time to the 2011 Tohoku earthquake.
In the third part of the thesis, we discuss issues related to long time scale instabilities of the Earth's rotation. The slow motion of the rotation axis with respect to the mantle, called True Polar Wander (TPW), has continuously been debated after the pioneering works in the sixties by Munk, MacDonald and Gold. We thus discuss TPW due to variations of surface loading from ice ages on hundreds of thousand year time scales, its sensitivity to the elastic or viscoelastic rheologies of the lithosphere and the stabilizing role of mantle density heterogeneities. Also, we face the problem of TPW driven by mantle convection on the million years time scale. Most studies have assumed that on this long time scale the planet readjusts without delay and that the Earth's rotation axis and the maximum inertia direction of mantle convection coincide. We herein overcome this approximation and we provide a novel treatment of the Earth's rotation, which clearly explains the interaction between mantle convection and rotational bulge readjustments, and the physical laws for the characteristic times controlling the polar motion in the directions of the intermediate and minimum principal axes of the mantle convection inertia tensor. We thus clarify a fundamental issue related to mantle mass heterogeneities and TPW dynamics
์ง์งํ์ ๋ฐฉ๋ฒ์ ์ด์ฉํ ๋๋ถ์์์ ์๋ถ ๋งจํ ์๋ ๊ตฌ์กฐ ๊ท๋ช ๋ฐ ๋งจํ ๋์ญํ๊ณผ ํ๋ด ํ์ฐ ํ๋์ ๋ํ ๊ณ ์ฐฐ
ํ์๋
ผ๋ฌธ(๋ฐ์ฌ) -- ์์ธ๋ํ๊ต๋ํ์ : ์์ฐ๊ณผํ๋ํ ์ง๊ตฌํ๊ฒฝ๊ณผํ๋ถ, 2021.8. ์ด์ค๊ธฐ.Volcanism and plate subduction are manifestations of vigorous mantle convection, and are important research subjects for understanding the thermodynamic state of the Earth's interior. Seismic waves propagating through the mantle reflect the physical properties of the mantle, providing detailed information on its thermal and compositional structure. Here we use various seismic methods to investigate the detailed upper mantle structure in northeast Asia where there are active intraplate volcanoes and ongoing plate subduction. Based on our results, we discuss the evolution of the upper mantle and mechanism of intraplate volcanism. Specifically, we apply teleseismic body-wave traveltime tomography to image the volcanic structure beneath Jeju Volcanic Island (Chapter 1), lithosphere and asthenosphere structures beneath the Korean Peninsula (Chapter 2), the stagnant Pacific slab and mantle transition zone structures (Chapter 3), and shallow asthenosphere structures beneath Quaternary volcanoes (Chapter 4). We measure relative arrival time residuals of the teleseismic P and S waves in high precision based on waveform similarity, and invert the datasets for constructing three-dimensional velocity structures using an iterative nonlinear tomography inversion technique. In Chapter 1, we use a unique dataset collected from the deployment of temporary broadband stations in Jeju Island and find out magmatic structures associated with a complex volcanic system that show evidence of a strong interaction between the continental lithosphere and ascending magmas. In Chapter 2, we image the detailed upper mantle structures beneath the Archean-Proterozoic massifs in the Korean Peninsula, which suggest the possible presence of a long-lasting lithospheric root that has experienced heterogeneous modification and reactivation at a craton margin in northeast Asia. In chapter 3, we image high-resolution deeper upper mantle structures including the mantle transition zone in northeast Asia by using the datasets of dense seismic arrays in the Korean Peninsula and southwest Japan. We find segmented stagnant Pacific slabs with a pronounced gap beneath the Korean Peninsula that was not revealed by previous studies due to limited resolution in this region. We detect and model wavefield variations of teleseismic body waves caused by the deeper upper mantle heterogeneities using 3-D waveform simulation. In the last chapter, we constrain thermal and compositional properties of the upper mantle based on quantitative assessment of high-resolution upper mantle seismic velocity models using thermodynamic calculations, mineralogical modeling, and seismic attenuation. We find evidence for shallow upper mantle melting zones focused beneath major Quaternary volcanoes and suggest an important role of shallow decompressional melting in developing and sustaining localized, long-lived intraplate volcanoes. Throughout all chapters, we have general implications for the origin, evolution, and relationships between the imaged upper mantle structures in the context of geology, tectonics, and geodynamics.ํ์ฐ ํ๋๊ณผ ํ๊ตฌ์กฐ ์ด๋(์, ํ์ ์ญ์
)์ ์ง๊ตฌ ๋ด๋ถ์ ํ๋ฐํ ๋งจํ ๋๋ฅ๋ฅผ ์
์ฆํ๋ฉฐ, ์ง๊ตฌ ๋ด๋ถ ์ด์ญํ์ ์ํ๋ฅผ ์ดํดํ๋๋ฐ ์ค์ํ ์ฐ๊ตฌ ๋์์ด๋ค. ์ง์งํ๋ ์ง๊ฐ๊ณผ ๋งจํ์ ํต๊ณผํ๋ฉด์ ์ด๋ค์ ๋ฌผ๋ฆฌ์ ์ธ ์ํ๋ฅผ ๋ฐ์ํ๋ฉฐ, ์ด๋ฅผ ๋ถ์ํ์ฌ ์ง๊ตฌ ๋ด๋ถ์ ์ด์ ๋ฐ ์ฑ๋ถ์ ํน์ฑ์ ๋ํด ์ฐ๊ตฌํ ์ ์๋ค. ๋ณธ ๋
ผ๋ฌธ์์๋ ๋ค์ํ ์ง์งํ์ ๋ฐฉ๋ฒ์ ํ์ฉํ์ฌ ํ ๋ด ํ์ฐํ๋๊ณผ ํ์ ์ญ์
์ด ํ๋ฐํ ์ผ์ด๋๊ณ ์๋ ๋๋ถ ์์์ ์๋ถ ๋งจํ ๊ตฌ์กฐ๋ฅผ ์ฐ๊ตฌํ๋ค. ๊ตฌ์ฒด์ ์ผ๋ก, ์๊ฑฐ๋ฆฌ ์ง์ง ์ฃผ์ ํ ๋ชจ๊ทธ๋ํผ๋ฅผ ์ฌ์ฉํ์ฌ ํ ๋ด ํ์ฐ์ผ๋ก ์๋ ค์ง ์ ์ฃผ๋ ํ๋ถ ์์๊ถ ๋ฐ ์ฐ์ฝ๊ถ์ ๊ตฌ์กฐ(์ 1์ฅ), ํ๋ฐ๋ ํ๋ถ์ ์์๊ถ ๋ฐ ์ฐ์ฝ๊ถ ๊ตฌ์กฐ(์ 2์ฅ), ๋๋ถ์์์ ์ง์ญ์ ์๋ถ ๋งจํ ์ ์ด๋์ ์ ์ฒด๋ ์ฌ๋ฉ(์ 3์ฅ), ํ๋ฐ๋ ์ฃผ๋ณ ์ 4๊ธฐ ํ์ฐ์ฒด ํ๋ถ์ ์์ ์ฐ์ฝ๊ถ(์ 4์ฅ)์ 3์ฐจ์ ๊ตฌ์กฐ๋ฅผ ์์ํํ๊ณ ๋ถ์ํ๋ค. ์ฐ๊ตฌ ์๋ฃ๋ก ์๊ฑฐ๋ฆฌ ์ง์ง์ ์ค์ฒดํ ์ ํธ(P, Sํ)๋ฅผ ์ด์ฉํ์ฌ ์ฐ๊ตฌ ์ง์ญ์ ์กฐ๋ฐํ๊ฒ ์ค์น๋ ์ง์ง๊ณ ๊ฐ์ ํํ ์ ์ฌ์ฑ์ ๊ธฐ๋ฐํ ๋ฐฉ๋ฒ์ผ๋ก ์ ๋ฐํ๊ฒ ์ธก์ ๋ ์๋ ์ฃผ์ ์์ฐจ๋ฅผ ์ฌ์ฉํ๋ฉฐ, ํด๋น ์์ฐจ๋ฅผ ์ต์ํํ ์ ์๋ ์ต์ ์ 3์ฐจ์ ์๋ ๊ตฌ์กฐ ๋ชจ๋ธ์ ๋น์ ํ ๋ฐ๋ณต ์ญ์ฐ ๋ฐฉ๋ฒ์ ํตํด ๊ตฌํ๋ค. ์ 1์ฅ์์๋, ์์ธ๋ํ๊ต ์ง์งํ ์ฐ๊ตฌ์ค์์ ์ ์ฃผ๋์ ์ฝ 2๋
๊ฐ ์ค์นํ ์์ ์ง์ง ๊ด์ธก๋ง ์๋ฃ๋ฅผ ์ฌ์ฉํ์์ผ๋ฉฐ, ์ ์ฃผ๋ ํ๋ถ ์์นํ๋ ๋ง๊ทธ๋ง์ ๋๋ฅ ์์๊ถ ๊ฐ์ ์ํธ์์ฉ์ผ๋ก ๋ฐ๋ฌํ ๋ณต์กํ ํํ์ ๋ง๊ทธ๋ง ์์คํ
์ ์์ํ ํ์๋ค. ์ 2์ฅ์์๋ ํ๋ฐ๋์ ์์๋ ๋ฐ ์์๋ ๋๋ฅ์๊ถ ํ๋ถ์ ์๋ถ ๋งจํ์ ์์ํํ๋ฉฐ, ๊ทธ ๊ฒฐ๊ณผ ๋๋ถ ์์์ ๋๋ฅ ์ฐ๋ณ๋ถ์์ ๋ถ๊ท ์งํ ์์ ๋ฐ ์ฌํ์ฑํ๋ฅผ ๊ฒช์ ์ค๋๋๊ณ ๋๊บผ์ด ์์๊ถ ๊ตฌ์กฐ๋ฅผ ํ์ธํ์๋ค. ์ 3์ฅ์์๋ ํ๋ฐ๋์ ์ผ๋ณธ ๋จ์๋ถ์ ๊ด์ธก๋ง ์๋ฃ๋ฅผ ์ฌ์ฉํ์ฌ ํ๋ฐ๋๋ฅผ ํฌํจํ ๋๋ถ์์์ ํ๋ถ์ ๊น์ ์๋ถ ๋งจํ ๊ตฌ์กฐ๋ฅผ ์์ํ ํ์๋ค. ๊ทธ ๊ฒฐ๊ณผ ์ ๋ผ์์ํ ํ๋ถ์ ์ ์ฒด๋ ํํ์ ์ฌ๋ฉ์ ๋ถ๊ท ์งํ ๋ถํฌ๋ฅผ ํ์ธํ์๊ณ , ๊ธฐ์กด ์ฐ๊ตฌ์์ ํด์๋ ํ๊ณ๋ก ๋ณด์ด์ง ์์๋ ํ๋ฐ๋ ํ๋ถ์ ์ฌ๋ฉ ๊ฐ๊ทน์ ์กด์ฌ๋ฅผ ์๋กญ๊ฒ ๋ฐํ๋ธ๋ค. ๋ํ ํ๋ฐ๋์ ๊ธฐ๋ก๋ ์๊ฑฐ๋ฆฌ ์ง์ง์ Sํ๋ฅผ ๋ถ์ํ์ฌ ์ฌ๋ฉ ๊ฐ๊ทน์ ์ํ ํ๋ฉด ์๊ณก์ ๊ด์ธกํ์๊ณ ์ด๋ฅผ 3์ฐจ์ ํํ ์๋ฎฌ๋ ์ด์
์ ํตํด ๋ชจ์ฌํ์๋ค. ๋ง์ง๋ง์ผ๋ก ์ 4์ฅ์์๋ ๊ธฐ์กด์ ์ป์ด์ง ๊ณ ํด์๋ ์๋ ๊ตฌ์กฐ ๋ชจ๋ธ์ ๋ฐํ์ผ๋ก ๋๋ถ ์์์ ์๋ถ ๋งจํ์ ์ด์ ๋ฐ ์ฑ๋ถ์ ํน์ฑ์ ์ด์ญํ์ ๊ณ์ฐ ๋ฐ ์ง์งํ ๊ฐ์ ํน์ฑ์ ๊ณ ๋ คํ์ฌ ์ ๋์ ์ผ๋ก ์ถ์ ํ๋ค. ๊ทธ ๊ฒฐ๊ณผ ํ๋ฐ๋ ์ฃผ๋ณ ์ 4๊ธฐ ํ์ฐ ์ง์ญ(์, ์ธ๋ฆ๋, ๋
๋, ๋ฐฑ๋์ฐ, ์ ์ฃผ๋, ํํ๊ฐ ์ ์ญ)์ ๊ตญ์ง์ ์ด๊ณ ์ง์์ ์ธ ๋ง๊ทธ๋ง ๋ฐ๋ฌ์ ๊ธฐ์ฌํ์์ ๊ฒ์ผ๋ก ์๊ฐ๋๋ ์ง์ค๋ ์์ ์ฐ์ฝ๊ถ ๋งจํ์ ๋ถ๋ถ ์ฉ์ต์ ํ์ธํ์๋ค. ์ ์ฅ์ ํตํ์ด, ์๋ถ ๋งจํ ๊ตฌ์กฐ๋ค์ ๊ธฐ์, ์งํ, ๊ทธ๋ฆฌ๊ณ ์ํธ ๊ด๊ณ์ ๋ํด ์ง์งํ์ , ์ง๊ตฌ์กฐ์ , ๊ทธ๋ฆฌ๊ณ ์ง๊ตฌ๋์ญํ์ ์ธ ๊ด์ ์์ ํด์ํ๊ณ ๋
ผ์ํ๋ค.Introduction 1
Chapter 1. Imaging of Lithospheric Structure Beneath Jeju Volcanic Island by Teleseismic Traveltime Tomography 4
1.1 Introduction 4
1.2 Methods 10
1.3 Results and Discussions 38
1.4 Conclusions 64
Chapter 2. Heterogeneous Modification and Reactivation of a Craton Margin Beneath the Korean Peninsula by Teleseismic Traveltime Tomography 66
2.1 Introduction 66
2.2 Methods 73
2.3 Results and Discussions 95
2.4 Conclusions 109
Chapter 3. Segmented Stagnant Pacific Slab and Its Interaction with the Mantle Transition Zone Beneath Northeast Asia Continental Margin by Teleseismic Traveltime Tomography 111
3.1 Introduction 111
3.2 Methods 115
3.3 Results and Discussions 131
3.4 Conclusions 153
Chapter 4. Seismic Evidence of Persistent Intraplate Volcanism by Shallow Mantle Melting in Northeast Asia 154
4.1 Introduction 154
4.2 Methods 158
4.3 Results 188
4.4 Discussions 198
4.5 Conclusions 211
Summary and Conclusions 212
Bibliography 217
Abstract in Korean (๊ตญ๋ฌธ ์ด๋ก) 263๋ฐ
Geodetic monitoring of tectonic deformation: Toward a strategy
Issues of interest and importance to society and science are presented. The problems considered are of national concern; their solutions may contribute to a better understanding of tectonic deformation and earthquake hazards. The need for additional field data, the role of geodetic measurements, the importance of both ground and space techniques, and the need for advanced instrumentation development are discussed
Structure and anisotropy of the upper mantle
Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Earth, Atmospheric, and Planetary Sciences, 1995.Includes bibliographical references (p. 171-180).by James B. Gaherty.Ph.D
Mantle convection and the state of the Earth's interior
During 1983โ1986, the four year period covered by this review, emphasis in the study of mantle convection shifted away from fluid mechanical analysis of simple systems with uniform material properties and simple geometries, toward analyzing the effects of more complicated, presumably more realistic models