2016
DOI: 10.1002/2015gl066479
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Poroelastic response of mid‐ocean ridge hydrothermal systems to ocean tidal loading: Implications for shallow permeability structure

Abstract: We use the time delay between tidal loading and exit‐fluid temperature response for hydrothermal vents to model the poroelastic behavior and shallow upflow zone (SUZ) effective permeability structure of three mid‐ocean ridge (MOR) sites with different spreading rates. Hydrothermal vents at Lucky Strike field exhibit relatively small phase lags corresponding to high SUZ effective permeabilities of ≥ ~10−10 m2, with variations that we interpret as resulting from differences in the extrusive layer thickness. By c… Show more

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Cited by 23 publications
(48 citation statements)
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“…The layer 2A permeability corresponding to the observed phase lag has a mean value of 1:5310 212 m 2 (contour lines in Figure 11). Note that this estimate is approximately 1 order of magnitude higher than that obtained by Barreyre and Sohn [2016] (2:5310 213 m 2 ) based on the single-layer simplification of the poroelstic formulas given in Appendices A and B. In their model, the impermeable bottom boundary is set at the layer 2A/2B interface, which is essentially comparable to our two-layer model with very small layer 2B crustal permeability (i.e., the lower ends of the contour lines in Figure 11).…”
Section: Coupled Tidal Oscillations Of Temperature and Chlorinity Frocontrasting
confidence: 40%
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“…The layer 2A permeability corresponding to the observed phase lag has a mean value of 1:5310 212 m 2 (contour lines in Figure 11). Note that this estimate is approximately 1 order of magnitude higher than that obtained by Barreyre and Sohn [2016] (2:5310 213 m 2 ) based on the single-layer simplification of the poroelstic formulas given in Appendices A and B. In their model, the impermeable bottom boundary is set at the layer 2A/2B interface, which is essentially comparable to our two-layer model with very small layer 2B crustal permeability (i.e., the lower ends of the contour lines in Figure 11).…”
Section: Coupled Tidal Oscillations Of Temperature and Chlorinity Frocontrasting
confidence: 40%
“…In the current study, the fluid compressibility is calculated using the equation of state developed by Driesner [2007] for 370 C 2.85 wt % (489 mmol/kg) NaCl solution at a reference pressure of 3:35310 4 kPa. The result: b f 55:3310 29 Pa 21 is an order of magnitude higher than the one used by Barreyre and Sohn [2016]: b f 54:8310 210 Pa 21 , which is relatively low for high-temperature pore fluids.…”
Section: Coupled Tidal Oscillations Of Temperature and Chlorinity Fromentioning
confidence: 81%
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“…However, recording time series of these quantities at the seafloor (i.e., in hydrothermal vent exit fluids) is technically challenging. By contrast, it is much simpler to measure temperature fluctuations in fluids discharging at the seafloor |ΔT1|0,t (e.g., Barreyre & Sohn, ; Barreyre et al, ; Fornari et al, ; Larson et al, ; Lilley et al, ; Scheirer et al, ; Sohn, ; Tivey et al, ). We therefore complement our previous solutions with an analytical expression for temperature fluctuations due to tidal loading |ΔTj|z,t.…”
Section: A Model For Tidal Modulation Of Hydrothermal Systems With Dementioning
confidence: 99%