Ocean Ridges and Oceanic Lithosphere
Ocean Ridges: Structure and Characteristics
Overview of Oceanic Ridges
Oceanic ridges indicate the loci of divergent plate margins where new oceanic lithosphere is created, comprising crust plus the uppermost mantle.
Considered as the longest, continuous mountain belt on Earth, the oceanic ridges show significant variability along their lengths.
Current Statistics:
Total ridge length: ~60,000 km
Topographic footprint: 1000–4000 km wide
Crest elevation: ~2–3 km above neighboring ocean basins.
Spreading Rates of Oceanic Ridges
Global variegation in oceanic ridge full-spreading rates can be categorized as follows:
Slow: 2.0 – 5.5 cm/yr
Intermediate: 5.5 – 10.0 cm/yr
Fast: > 10 cm/yr
Ultraslow: newly defined as < 2.0 cm/yr (discussion deferred).
Topography of Ocean Ridges
Ridge morphology is influenced significantly by the spreading rate:
Fast-Spreading Ridges:
Example: East Pacific Rise (EPR) at 3° S, characterized by a relatively smooth profile, even in the crestal region.
Slow-Spreading Ridges:
Example: Mid-Atlantic Ridge (MAR) at 37° N, featuring rugged terrain with a median rift valley typically 30–50 km wide and up to 3 km deep.
Intermediate-Spreading Ridges: marked by graben-like topography that is more subdued than slow-spreading ridges.
Geological Features of Ocean Ridges
General Structures
Deep median rift valleys (graben) are normally bounded by back-tilted, inward-facing normal faults, with fault scarps presenting many hundreds of meters of relief.
An axial topographic high (~1–5 km wide) appears due to multiple small shield volcanoes aligned parallel to the rift valley.
Specific Examples of Topographic Profiles
Mid-Atlantic Ridge:
Rough topography with a median rift valley.
East Pacific Rise:
Smoother slopes, indicating differences in volcanic activity across regions.
Depth-Age Relationship of Oceanic Lithosphere
Overview
The sea floor's depth increases with distance from the central spreading ridge, showcasing a systematic relationship across the Pacific, Indian, and Atlantic Oceans irrespective of spreading rates.
Cooling Effects
Newly formed oceanic lithosphere expands and exhibits thermal buoyancy, giving rise to uplift at the central ridge. This lithosphere cools as it ages, resulting in:
Increased plate density.
Increased lithospheric thickness, where the lithosphere's base lies at the 1300°C isotherm.
Lithospheric Thickness Changes
Thickness increment from a few kilometers at the ridge crest to:
30 km at 5 million years (Ma)
100 km at 50 Ma.
Thermo-Mechanical Models:
Half-Space (HS) Cooling Model: relates age (t; Myr) to depth (d) with the formula:
d = 2500 + 350 imes t^{1/2} (applicable for oceanic lithosphere younger than 70 Ma).
Two-Layer Model (PSM):
Defines a rigid upper layer and a viscous lower layer that convects and supports heat transfer to the upper layer, applicable for lithosphere older than 70 Ma.
Coincides with the formula:
d = 6400 + 3200 e^{-t/62.8} .
Global Data Analysis
Stein and Stein (1992) proposed using a large dataset of depth and heat flow measurements:
Statistically fitted two separate depth-age equations (GDH1) with:
d = 2600 + 365 t^{1/2} for t < 20 Myr .
These equations follow a general format similar to HS and PSM but are considered more rigorously fitted.
Cooling Mechanisms in Oceanic Lithosphere
Hydrothermal Circulation
Thermal contraction generates cracking and permeability:
As oceanic crust moves away from the ridge crest, it subsides and builds up impermeable sediments.
Pores and cracks become filled with minerals deposited by circulating seawater.
Sealing Age: appears to be ~60 Myr.
Evidence of Hydrothermal Circulation
Evidence is visible in metalliferous deposits at ridge crests, generated by:
Hydrothermally mobile metals dissolved from the crust.
Precipitation upon cooling in contact with cold seawater.
Types of smokers:
Black Smokers: 350–400 °C, which precipitate metal sulfides (e.g., Au, Zn, Pb, Cu).
White Smokers: 30–330 °C, which precipitate sulfates (Ba, Ca, Si).