Flows through the Mid-Atlantic Ridge in the Northern Channels. Charlie Gibbs Fracture Zone and Other Fracture Zones

Author(s):  
Eugene G. Morozov ◽  
Alexander N. Demidov ◽  
Roman Y. Tarakanov ◽  
Walter Zenk
1977 ◽  
Vol 14 (4) ◽  
pp. 664-673 ◽  
Author(s):  
D. I. Ross ◽  
R. K. H. Falconer

Geophysical data collected as part of Leg 37 are compiled with more recent data collected for new IPOD drilling site surveys. Bathymetric and magnetic maps covering the area of sites 332–335 are presented. On the basis of magnetic anomaly correlations it is suggested that site 334 is on normal crust between fracture zones A and B and not closer than 15 km to either fracture zone. Magnetic anomaly inversion is applied to a composite profile, extending from the ridge crest out to beyond anomaly 5. It shows a definite change in spreading rate at 4.7 ± 0.5 Ma. Average rates for the periods 0–4.7 Ma and 4.7–10 Ma are 10.2 ± 0.9 mm/yr and 14.0 ± 1.9 mm/yr respectively. The inversion results are consistent with a simple magnetic source layer 2 km thick.


1970 ◽  
Vol 7 (5) ◽  
pp. 1352-1355 ◽  
Author(s):  
M. J. Keen

A seismic reflection profile across the fracture zones on the Mid-Atlantic Ridge between 43° N and 44° N shows that the thickness of sediment increases markedly south of the fracture zone at 43° 05′ N on the eastern flank of the ridge. The thickness there is in accord with observations made west of the ridge in the region of the survey at 45° N. This suggests that the effects of rates of sea-floor spreading and sedimentation have been similar on this eastern part of the ridge to those west of the ridge farther north.


Geophysics ◽  
1995 ◽  
Vol 60 (1) ◽  
pp. 66-75 ◽  
Author(s):  
Christopher Juhlin

In 1987 the Swedish Nuclear Fuel and Waste Management Co. (SKB) funded the shooting of a 1.7-km long, high‐resolution seismic profile over the Finnsjön study site using a 60‐channel acquisition system with a shotpoint and geophone spacing of 10 m. The site is located about 140 km north of Stockholm and the host rocks are mainly granodioritic. The main objective of the profile was to image a known fracture zone with high hydraulic conductivity dipping gently to the west at depths of 100 to 400 m. The initial processing of the data failed to image this fracture zone. However, a steeply dipping reflector was imaged indicating the field data were of adequate quality and that the problem lay in the processing. These data have now been reprocessed and a clear image of the gently dipping zone has been obtained. In addition, several other reflectors were imaged in the reprocessed section, both gently and steeply dipping ones. Correlations with borehole data indicate that the origin of these reflections are also fracture zones. The improvement over the previous processing is caused mainly by (1) refraction statics, (2) choice of frequency band, (3) F-K filtering, and (4) velocity analyses. In addition to reprocessing the data, some further analyses were done including simulation of acquisition using only the near‐offset channels (channels 1–30) and the far‐offset channels (channels 31–60), and determining the damping factor Q in the upper few hundred meters based upon the amplitude decay of the first arrivals. The data acquisition simulation shows the far‐offset contribution to be significant even for shallow reflectors in this area, contrary to what may be expected. A Q value of 10, determined from observed amplitude decay rates, agrees well with theoretical ones assuming plane wave propagation in an attenuating medium.


1975 ◽  
Vol 86 (10) ◽  
pp. 1348 ◽  
Author(s):  
J. D. PHILLIPS ◽  
H. S. FLEMING ◽  
R. H. FEDEN ◽  
W. E. KING ◽  
R. K. PERRY

2019 ◽  
Vol 145 ◽  
pp. 1-12 ◽  
Author(s):  
Claudia H.S. Alt ◽  
Antonina Kremenetskaia (Rogacheva) ◽  
Andrey V. Gebruk ◽  
Andrew J. Gooday ◽  
Daniel O.B. Jones

2015 ◽  
pp. 427-436
Author(s):  
J. D. Phillips ◽  
H. S. Fleming ◽  
R. H. Feden ◽  
W. E. King ◽  
R. K. Perry

2007 ◽  
Vol 416 (1) ◽  
pp. 1120-1124 ◽  
Author(s):  
A. N. Demidov ◽  
S. A. Dobrolyubov ◽  
E. G. Morozov ◽  
R. Yu. Tarakanov

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