Matches in SemOpenAlex for { <https://semopenalex.org/work/W2032716429> ?p ?o ?g. }
- W2032716429 endingPage "15487" @default.
- W2032716429 startingPage "15463" @default.
- W2032716429 abstract "Although slow spreading ridges characterized by a deep axial valley and fast spreading ridges characterized by an axial bathymetric high have been extensively studied, the transition between these two modes of axial morphology is not well understood. We conducted a geophysical survey of the intermediate spreading rate Southeast Indian Ridge between 88°E and 118°E, a 2300‐km‐long section of the ridge located between the Amsterdam hot spot and the Australian‐Antarctic Discordance where satellite gravity data suggest that the Southeast Indian Ridge (SEIR) undergoes a change from an axial high in the west to an axial valley in the east. A basic change in axial morphology is found near 103°30′E in the shipboard data; the axis to the west is marked by an axial high, while a valley is found to the east. Although a well‐developed axial high, characteristic of the East Pacific Rise (EPR), is occasionally present, the more common observation is a rifted high that is lower and pervasively faulted, sometimes with significant (>50 m throw) faults within a kilometer of the axis. A shallow axial valley (<700 m deep) is observed from 104°E to 114°E with a sudden change to a deep (>1200 m deep) valley across a transform at 114°E. The changes in axial morphology along the SEIR are accompanied by a 500 m increase in near‐axis ridge flank depth from 2800 m near 88°E to 3300 m near 114°E and by a 50 mGal increase in the regional level of mantle Bouguer gravity anomalies over the same distance. The regional changes in depth and mantle Bouguer anomaly (MBA) gravity can be both explained by a 1.7–2.4 km change in crustal thickness or by a mantle temperature change of 50°C–90°C. In reality, melt supply (crustal thickness) and mantle temperature are linked, so that changes in both may occur simultaneously and these estimates serve as upper bounds. The along‐axis MBA gradient is not uniform. Pronounced steps in the regional level of the MBA gravity occur at 103°30′E–104°E and at 114°E–116°E and correspond to the changes in the nature of the axial morphology and in the amplitude of abyssal hill morphology suggesting that the different forms of morphology do not grade into each other but rather represent distinctly different forms of axial structure and tectonics with a sharp transition between them. The change from an axial high to an axial valley requires a threshold effect in which the strength of the lithosphere changes quickly. The presence or absence of a quasi‐steady state magma chamber may provide such a mechanism. The different forms of axial morphology are also associated with different intrasegment MBA gravity patterns. Segments with an axial high have an MBA low located at a depth minimum near the center of the segment. At EPR‐like segments, the MBA low is about 10 mGal with along‐axis gradients of 0.15–0.25 mGal/km, similar to those observed at the EPR. Rifted highs have a shallower low and lower gradients suggesting an attenuated composite magma chamber and a reduced and perhaps episodic melt supply. Segments with a shallow axial valley have very flat along‐axis MBA profiles with little correspondence between axial depth and axial MBA gravity." @default.
- W2032716429 created "2016-06-24" @default.
- W2032716429 creator A5021771374 @default.
- W2032716429 creator A5036128363 @default.
- W2032716429 date "1997-07-10" @default.
- W2032716429 modified "2023-10-16" @default.
- W2032716429 title "The Southeast Indian Ridge between 88°E and 118°E: Gravity anomalies and crustal accretion at intermediate spreading rates" @default.
- W2032716429 cites W1966049707 @default.
- W2032716429 cites W1970259035 @default.
- W2032716429 cites W1981101269 @default.
- W2032716429 cites W1983633783 @default.
- W2032716429 cites W1988518537 @default.
- W2032716429 cites W1990125118 @default.
- W2032716429 cites W1990814837 @default.
- W2032716429 cites W1992046648 @default.
- W2032716429 cites W1993808968 @default.
- W2032716429 cites W1994175975 @default.
- W2032716429 cites W1995904733 @default.
- W2032716429 cites W1997359321 @default.
- W2032716429 cites W1998671678 @default.
- W2032716429 cites W2001514620 @default.
- W2032716429 cites W2006712012 @default.
- W2032716429 cites W2009905326 @default.
- W2032716429 cites W2010868553 @default.
- W2032716429 cites W2013539586 @default.
- W2032716429 cites W2013923435 @default.
- W2032716429 cites W2017460701 @default.
- W2032716429 cites W2017714045 @default.
- W2032716429 cites W2024137847 @default.
- W2032716429 cites W2025611134 @default.
- W2032716429 cites W2026807252 @default.
- W2032716429 cites W2037283958 @default.
- W2032716429 cites W2045638671 @default.
- W2032716429 cites W2048824368 @default.
- W2032716429 cites W2050889054 @default.
- W2032716429 cites W2057371440 @default.
- W2032716429 cites W2060195375 @default.
- W2032716429 cites W2062837188 @default.
- W2032716429 cites W2066925877 @default.
- W2032716429 cites W2068473785 @default.
- W2032716429 cites W2069172403 @default.
- W2032716429 cites W2073881300 @default.
- W2032716429 cites W2075530822 @default.
- W2032716429 cites W2075845557 @default.
- W2032716429 cites W2083882926 @default.
- W2032716429 cites W2087239287 @default.
- W2032716429 cites W2102234201 @default.
- W2032716429 cites W2107316430 @default.
- W2032716429 cites W2114003980 @default.
- W2032716429 cites W2121873899 @default.
- W2032716429 cites W2130763109 @default.
- W2032716429 cites W2135494568 @default.
- W2032716429 cites W2150226675 @default.
- W2032716429 cites W2162129176 @default.
- W2032716429 cites W2485744459 @default.
- W2032716429 cites W2486364046 @default.
- W2032716429 cites W3103104081 @default.
- W2032716429 doi "https://doi.org/10.1029/97jb00511" @default.
- W2032716429 hasPublicationYear "1997" @default.
- W2032716429 type Work @default.
- W2032716429 sameAs 2032716429 @default.
- W2032716429 citedByCount "67" @default.
- W2032716429 countsByYear W20327164292012 @default.
- W2032716429 countsByYear W20327164292013 @default.
- W2032716429 countsByYear W20327164292014 @default.
- W2032716429 countsByYear W20327164292015 @default.
- W2032716429 countsByYear W20327164292017 @default.
- W2032716429 countsByYear W20327164292018 @default.
- W2032716429 countsByYear W20327164292019 @default.
- W2032716429 countsByYear W20327164292020 @default.
- W2032716429 countsByYear W20327164292021 @default.
- W2032716429 countsByYear W20327164292022 @default.
- W2032716429 crossrefType "journal-article" @default.
- W2032716429 hasAuthorship W2032716429A5021771374 @default.
- W2032716429 hasAuthorship W2032716429A5036128363 @default.
- W2032716429 hasBestOaLocation W20327164291 @default.
- W2032716429 hasConcept C111368507 @default.
- W2032716429 hasConcept C117485682 @default.
- W2032716429 hasConcept C121332964 @default.
- W2032716429 hasConcept C127313418 @default.
- W2032716429 hasConcept C151730666 @default.
- W2032716429 hasConcept C165205528 @default.
- W2032716429 hasConcept C174943157 @default.
- W2032716429 hasConcept C194482375 @default.
- W2032716429 hasConcept C2776401274 @default.
- W2032716429 hasConcept C32277403 @default.
- W2032716429 hasConcept C44870925 @default.
- W2032716429 hasConceptScore W2032716429C111368507 @default.
- W2032716429 hasConceptScore W2032716429C117485682 @default.
- W2032716429 hasConceptScore W2032716429C121332964 @default.
- W2032716429 hasConceptScore W2032716429C127313418 @default.
- W2032716429 hasConceptScore W2032716429C151730666 @default.
- W2032716429 hasConceptScore W2032716429C165205528 @default.
- W2032716429 hasConceptScore W2032716429C174943157 @default.
- W2032716429 hasConceptScore W2032716429C194482375 @default.
- W2032716429 hasConceptScore W2032716429C2776401274 @default.
- W2032716429 hasConceptScore W2032716429C32277403 @default.
- W2032716429 hasConceptScore W2032716429C44870925 @default.