Items in eScholarship@BC will redirect to URBC, Boston College Libraries' new repository platform. eScholarship@BC is being retired in the summer of 2025. Any material submitted after April 15th, 2025, and all theses and dissertations from Spring semester 2025, will be added to URBC only.
The Morphology of Slow-Slipping Oceanic Transform Faults on the Mid-Atlantic Ridge
Woodford, Emma. “The Morphology of Slow-Slipping Oceanic Transform Faults on the Mid-Atlantic Ridge”, Boston College, 2024. http://hdl.handle.net/2345/bc-ir:109962.
The global mid ocean ridge system is segmented by transform faults and non-transform discontinuities. Oceanic transform faults display distinct morphology characterized by a deep valley and shallow transverse ridges on either side of the valley. Although the morphology of oceanic transform faults is known to first order, there is no consensus on the processes that form the transform valley and/or the adjacent transverse ridges. To date, most models of transform morphology attribute these features to either transform-normal extension or to shear stresses induced by slip along the fault. In this thesis, I compile bathymetric data along 16 major transform faults on the Mid-Atlantic Ridge and identify the key morphological properties of each transform. Specifically, I estimate transform valley width, depth, and total relief measured from the valley floor to the adjacent transverse ridges. The strongest correlation is between the relief and maximum depth, but there is a weaker correlation between maximum depth and valley width. These morphologic properties are then compared to key fault parameters such as slip rate, fault-normal compression/extension rate, thermal area, and the seismic coupling ratio, which is defined as the fraction of total fault slip that occurs seismically. These comparisons are used to test models that describe mechanisms of the formation of the transform valley. The strongest correlation is between the fault thermal area and valley half width. This suggests that the width of the transform valley may be controlled by the shear stress applied to the fault as it slips. By contrast, the data are not consistent with a model in which the valley is created by extension across the fault, because our data show that the maximum transform valley depth increases with compression and not extension.