Spelling suggestions: "subject:"earthcrust"" "subject:"earth’scrust""
1 |
Crustal structure of the Baja Peninsula between latitudes 22 ̊N and 25 ̊NHuehn, Bruce 28 April 1977 (has links)
Geophysical data collected in 1975 and 1976 reveal major
crustal and tectonic elements of the continental margin of southern
Baja California. Gravity, magnetic, seismic reflection and bathymetric data show seaward extension of the islands enclosing Magdalena
and Almejas Bays. A seismic reflection profile, oriented
approximately normal to the trend of the Baja peninsula, indicates
normal faulting of the near surface sediment layers along the outer
continental shelf. The reflection record also shows that sediment
layers immediately above the acoustic basement dip toward the east
at the base of the continental slope. A crustal and subcrustal cross
section, oriented approximately parallel to the reflection profile and
constrained by gravity, magnetic, bathymetric and seismic refraction
data, indicates a maximum crustal thickness of approximately 21 km
for Baja California, making it intermediate in thickness between
normal continental and normal oceanic crusts. The section also indicates a low density zone in the mantle below the Gulf of California.
Magnetic anomalies along the cross section require oceanic crust of
the Pacific Plate to extend at least 50 km landward of the edge of the
western continental shelf of Baja California. This suggests either
a past period of oblique subduction of the Pacific Plate beneath Baja
California or emplacement of Pacific Plate oceanic crust beneath the
peninsula by descending spreading centers of the East Pacific Rise. / Graduation date: 1977
|
2 |
Seismic ray trace techniques applied to the determination of crustal structures across the Peru continental margin and Nazca plate at 9 ̊S. latitudeJones, Paul Roy III 09 August 1978 (has links)
Seismic refraction, reflection and gravity data obtained
across the Peru continental margin and Nazca Plate
at 9° S. permit a detailed determination of crustal structure.
Complex structures normal to the profile require the
development of a ray trace technique to analyze first and
later arrivals for eleven overlapping refraction lines.
Other data integrated into the seismic model include velocities and depths from well data, near surf ac sediment structures
from reflection profiles and velocities obtained from
nearby common depth point reflection lines. Crustal and
subcrustal densities and structures were further constrained
by gravity modeling to produce a detailed physical model of
a convergent margin.
The western portion of the continental shelf basement
consists of a faulted outer continental shelf high of
Paleozoic or older rocks. It is divided into a deeper
western section of velocity 5.0 km/sec and a shallower,
denser eastern section of velocity 5.65 to 5.9 km/sec. The
combined structure forms a basin of depth 2.5 to 3.0 km
which contains Tertiary sediments of velocity 1.6 to 3.0
km/sec. In this area, near-surface sedimentary structure
suggests truncated sinusoidal features caused by exposure
to onshore-offshore bottom currents.
The 3 km thick, 4.55 to 5.15 km/sec basement of the
eastern shelf shoals shoreward. Together, this basement
and the eastern section of the outer continental shelf high
form a synclinal basin overlain by Tertiary sediments which
have a maximum thickness of 1.8 km and a velocity range of
1.7 to 2.55 km/sec. The gravity model shows a large block
of 3.0 g/cm³ lower crustal material emplaced within the
upper crustal region beneath the eastern portion of the continental
shelf.
Refraction data indicates a continental slope basement
of velocity 5.0 km/sec overlying a slope core material with
n interface velocity of 5.6 km/sec. The sedimentary
layers of the slope consist of an uppermost layer of
slumped sediment with an assumed velocity of 1.7 to 2 km/
sec which overlies an acoustic basement of 2.25 to 3.6 km/
sec.
The high velocities (and densities) of the slope basement
suggest the presence of oceanic crustal material over
lain by indurated oceanic and continental sediments. This
slope melange may have formed during the initiation of subduction
from imbricate thrusting of upper layers of
oceanic crust. Once created, the melange forms a trap and
forces the subduction of most of the sediments that enter
the trench.
A ridge-like structure within the trench advances
the seismic arrival times of deeper refractions and supports
the suggestion that it is thrust-faulted oceanic
crust which has been uplifted relative to the trench floor.
The model of the descending Nazca Plate consists of a 4 km
thick upper layer of velocity 5.55 km/sec and a thinner
(2.5 km) but faster 7.5 km/sec lower layer which overlies
a Moho of velocity 8.2 km/sec. The gravity model indicates
that the plate has a dip of 5° beneath the continental
slope and shelf. West of the trench, the lower crustal
layers shallow, which may represent upward flexure of the
oceanic plate due to compressive forces resulting from the
subduction process.
The upper crustal layers of the 120 km long oceanic
plate portion consist of a thin 1.7 km/sec sedimentary layer
overlying a 5.0 to 5.2 km/sec upper layer. An underlying
5.6 to 5.7 km/sec lower layer becomes more shallow to the
east within 60 km of the trench while a deeper 6.0 to 6.3
km/sec layer thickens to the east. The lower crustal model
consists of a 7.4 to 7.5 km/sec high velocity layer which
varies in thickness from 2.5 km to 4.0 km. The 8.2 km/sec
Moho interface varies not more than ±0.5 km from a modeled
depth of 10.5 km. / Graduation date: 1979 / Best scan available for figures.
|
3 |
Numerical analysis of electrical fluid and rock resistivity in hydrothermal systemsMoskowitz, Bruce Matthew, 1952- January 1977 (has links)
No description available.
|
4 |
A study of the crustal structure of North Central Georgia and South Carolina by analysis of synthetic seismogramsLee, Chang Kong 08 1900 (has links)
No description available.
|
5 |
Geophysical studies of southern Appalachian crustal structureHinton, Douglas Marshall 08 1900 (has links)
No description available.
|
6 |
Modeling of crustal structures in southwest Georgia from magnetic dataHerbert, James Charles 08 1900 (has links)
No description available.
|
7 |
Determination of crustal velocity structures from teleseismic p wavesJiang, Wei Ping 05 1900 (has links)
No description available.
|
8 |
Crustal structures and tectonism in southeastern Alaska and western British Columbia from seismic refraction, seismic reflection, gravity, magnetic, and microearthquake measurementsJohnson, Stephen Hans 13 October 1971 (has links)
Seismic refraction measurements along two unreversed lines
indicate that the earth's crust is 26 km thick in southeastern Alaska
and 30 km thick along the Inside Passage of British Columbia. The
crust in southeastern Alaska, north of Dixon Entrance, consists of
a layer 9 km thick with a seismic velocity of 5.90 km/sec, a layer
7 km thick with a seismic velocity of 6.30 km/sec. and a layer 10 km
thick with a seismic velocity of 6.96 km/sec. The crust along the
Inside Passage of British Columbia, south of Dixon Entrance, consists
of a layer 13 km thick with a seismic velocity of 6.03 km/sec, a layer
5 km thick with a seismic velocity of 6.41 km/sec, and a layer 12 km
thick with a seismic velocity of 6.70 km/sec. The velocity of the
mantle below the M discontinuity is 7.86 km/sec in southeastern
Alaska and 8.11 km/sec in British Columbia.
A compilation of Bouguer gravity data along the Inside Passage
from northern Vancouver Island to northern southeastern Alaska
indicates near-zero anomalies between steep gradients offshore and
near the western margin of the Coast Mountains. A two-dimensional
gravity model, constrained by seismic refraction measurements,
suggests that the thickness of the crust is constant beneath the region
of near-zero gravity anomalies and indicates a step-like transition
between oceanic and continental structure.
Seismic reflection, gravity, and magnetic measurements,
obtained during a 1970 cruise of the R/V Yaquina, help to determine
upper crustal structures in Dixon Entrance. Gravity models, constructed to agree with these data and the measurements of previous
investigators, indicate sediment thicknesses of nearly 3 km east
of Learmonth Bank and west of Celestial Reef. Magnetic models
suggest large lateral changes in basement susceptibility. Either
highly metamorphosed rock or basaltic intrusions can account for
these changes in susceptibility. Folded sediments suggest post depositional
distortion due either to regional compression or to
major local intrusions. Several linear gravity features, observed
in northern Dixon Entrance, disappear north of Graham Island.
Either the structures responsible for the gravity features end or
thick layers of basalt, extending northward from Graham Island,
obscure the effect of the structures.
A single-station survey detected microearthquakes at nine
locations in western British Columbia and southeastern Alaska. The
majority of the observed distant microearthquakes probably originated
in the Queen Charlotte Islands fault zone. However, observed
nearby microearthquakes indicate a microearthquake seismicity of
several events per day along the mainland coast of British Columbia.
Temporary seismic arrays located at a site along the central
portion of Chatham Strait near the Chatham Strait fault and at a site
in Glacier Bay recorded few nearby microearthquakes. Arrivals at
the arrays permitted the location of distant microearthquakes, however,
with epicenters in the vicinity of northern Lynn Canal and along
the Fairweather fault. / Graduation date: 1972
|
9 |
Sonobuoy refraction study of the crust in the Gorda BasinCook, Jeffrey A. 05 December 1980 (has links)
The Gorda Basin is a young oceanic plate which comes in direct
contact with the convergent margin of western North America. Two long
sonobuoy refraction profiles crossing the basin provide nearly continuous
data for computing the velocity structure of the crust and adjacent
continental slope. Time-term analysis utilizing multiple receivers
and overlapping profiles revealed a thick transition layer which averages
2.3 km but displays considerable lateral variation. The seismic
compressional velocity of this layer is 5.3 km/sec. Th average thickness
of Layer 3 is 3.4 km with a velocity of 6.9 km/sec. The base of
the crust is marked by the seismic Moho, the velocity below which is
8.1 km/sec. Refraction and reflection studies of sediment cover indicate
a thickening of turbidite deposits to the southeast from less than
100 meters to over 2.5 km along the continental margin.
Ophiolite studies indicate that the top of Layer 3 marks the upper
extent of amphibolite facies metamorphism of basaltic sheeted dikes.
Lateral depth variations of this seismic boundary in the Gorda Basin
may suggest the occurrence of isograd relief along the spreading center.
The Moho marks the boundary between mafic and ultramafic rocks near the
ridge but may represent the maximum depth of serpentinization in the
crust after it moves away from the spreading axis.
Thin crust (4-5 km) and deep bathymetry in the central portion of
the basin have resulted from crustal formation processes occurring at
ridge crest offsets and are coincident with recent seismicity in the
area. The Gorda ridge offsets and asymmetrical fan spreading of
magnetic anomalies are features observed in response to a regional
change in spreading directions and encroachment of the Pacific and North
American plates. The Gorda plate as a whole does not respond rigidly
to the resulting north-south compression.
Complex structures of the continental slope, revealed by seismic
reflection, limited the reduction of refraction data using plane layer
methods. A simplified seismic section was computed consisting of three
probable sediment layers with velocities of 1.8, 2.5 and 4.0 km/sec
overlying oceanic crust. The crust is observed to dip about two degrees
towards the continent at the base of the slope.
A model of subduction unique to the northern California margin is
one whereby young crust is subducted slowly and quickly reheated so
that no brittle portion remains at normal Benioff depths. Rapid sedimentation
rates balance the subduction of the crust at the margin, preventing
the formation of a deep trench. / Graduation date: 1981
|
10 |
A comparison of seismic properties of young and mature oceanic crustBee, Michel 30 March 1984 (has links)
Seismic properties (P, S velocities and Poisson's ratio) of
young (0.75 m.y.) and mature (110 m.y.) oceanic crust are obtained
by studying explosive refraction data collected in the Pacific Ocean
using ocean bottom and downhole seismometers. A comparison of the
results for the two regions indicates that the upper crustal velocities
increase with age due to the cementation of cracks and fractures,
the upper mantle velocities increase with age due to cooling,
and the crust (mainly the lower crust) thickens with age. The Poisson's
ratios obtained in this study are too small to be consistent
with the presence of any serpentinization of the lower crust or
upper mantle which therefore precludes upper mantle serpentinization
as the cause for the thickening of the crust with age. When comparing
seismic structures of young and mature oceanic crust with
ophiolite models, we find close similarities between the Samail
ophiolite and young oceanic crust, and between the Bay of Islands
ophiolite and old oceanic crust. The 110 m.y. old crust of the
northwest Pacific Basin is characterized by high velocity gradients
in the upper crust, low velocity gradients in the lower crust, a
smooth 1 km-thick crust-mantle transition zone and the presence of a
minimum 14% anisotropy in the upper mantle compressional wave
velocities. Velocities are highest in an east-west direction. The
0.75 m.y. old crust at the intersection of the East Pacific Rise and
the Orozco fracture zone is characterized by a steady increase in
velocity with depth. A delay time analysis shows a trend to large
Layer 3 delay times in the Orozco fracture zone indicating a thicker
Layer 2 and/or low Layer 2 velocities.
An investigation of different model parameterizations for the
tau-zeta travel time inversion using a synthetic data set indicates
that the best velocity gradient solutions, based on the least deviation
of the solution from the true model, are obtained from models
in which the velocities of the layer bounds take on the values of
the observed velocities of the refracted waves. A trade-off curve
obtained from varying the number of layers in the model shows that a
model with as many layers as observed data points represents a satisfactory
compromise between model resolution and solution variance. / Graduation date: 1984
|
Page generated in 0.0354 seconds