Earl E Davis’s research while affiliated with Natural Resources Canada and other places

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Publications (737)


Global distribution of Ocean Drilling Program/International Ocean Discovery Program (ODP/IODP) Circulation Obviation Retrofit Kit borehole observatories within and seaward of subduction zone accretionary prisms (a), and expanded views shown for sites at the Cascadia (b), Nankai (c), and Costa Rica (Middle America Trench) (d) subduction zones. Base maps generated using GeoMapApp (www.geomapapp.org; Ryan et al. 2009) with the default map projection.
Generalized schematic diagrams of Circulation Obviation Retrofit Kit (CORK) versions developed and used for subduction zones studies, including the original CORK configuration (with perforated casing used in open-hole sedimentary sections below the main casing) (a), the Advanced CORK for multi-level monitoring (b), the CORK II and Long-Term Borehole Monitoring System (LTBMS) in which secondary casing extends below the primary casing for monitoring and other instrumentation (c), and the SmartPlug for temporary installations (d).
Schematic seismotectonic/geodynamic context of subduction zone studies, representative of those being carried out at three of the locations discussed in this paper. CORK = Circulation Obviation Retrofit Kit; ACORK = Advanced CORK; LTBMS = Long-Term Borehole Monitoring System; GNSS=Global Navigation Satellite System; OBS=Ocean Bottom Seismometer; VLFE = very low frequency earthquake; LFT = low frequency tremor; ETS = episodic tremor and slip.
Schematic illustration of seismic and geodynamic phenomena observed in Circulation Obviation Retrofit Kit data (a), spanning a broad range of frequencies (b). (after Sun and Davis 2022).
Steady-state temperatures measured with Circulation Obviation Retrofit Kit (CORK) thermistor cables at Cascadia Holes 892B and U1364A that targeted the limiting depths of gas hydrate stability (a), and with CORK thermistor cables and bottom-hole probes at Barbados Holes 948D, 949C that targeted the subduction decollement bounding the accretionary prism and subducting sediments (b). BSR, bottom simulating reflector; WSTP = water sampler temperature probe.

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Deep-sea borehole fluid pressure and temperature observations at subduction zones and their geodynamic implications
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December 2024

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17 Reads

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3 Citations

Earl E. Davis

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Tianhaozhe Sun

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Keir Becker

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[...]

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Kelin Wang

Seafloor and subseafloor temperature and pressure monitoring has been carried out with CORK (“Circulation Obviation Retrofit Kit”) sealed deep-ocean borehole observatories since their original design and deployments in 1991 in hydrologically and tectonically active settings. In this paper, we review results from 20 installations at six subduction zones that have provided novel insights into the thermal and hydrologic state, time-dependent deformation, and elastic properties of the subseafloor. Monitoring depths reached the levels of the megathrust faults beneath the outer subduction prisms at Nankai, Costa Rica, and Barbados, but only at the last were substantially elevated average pressures observed (excess fluid-pressure ratios of ∼0.3 and 0.5). Otherwise, all records are characterized by fluid pressures only slightly super-hydrostatic. Transient pressure anomalies are observed to be common within both the subduction prisms and the incoming subducting plates. These reflect deformation (volumetric strain changes) caused by distant seismogenic fault slip at the time of large earthquakes, and by more local slow slip that is seen to propagate to the outermost reaches of the prisms from greater depths at rates of several kilometers per day. No such activity is seen at the Cascadia prism site, however, suggesting that its subduction fault is more completely locked. Where CORK observatories are co-located with or near seismometers and other seafloor monitoring instruments and are connected to cable systems for power, real-time high-rate data acquisition, and precise timing, the observations allow relationships among seismic ground motion, seafloor pressure, and formation pressure to be defined. These, in turn, constrain formation elastic properties, and confirm the efficiency and fidelity with which strain is converted to formation pressure.

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Monitoring subseafloor temperature and fluid pressure in sealed ODP/IODP boreholes to constrain in situ hydrological state and processes in igneous oceanic crust

December 2024

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36 Reads

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2 Citations

We review the contributions to our understanding of the hydrogeology of the oceanic crust as gained by monitoring subseafloor temperatures and pressures in CORK (“Circulation Obviation Retrofit Kit”) sealed hole observatories that penetrate through marine sediments into igneous basement. CORKs were installed during 1991–2012 in 17 holes drilled by the Ocean Drilling Program and Integrated Ocean Drilling Programs in igneous oceanic crust (aged 0.4–24 Ma) in the thickly sedimented eastern Pacific Ocean and in the thinly sedimented north Atlantic Ocean. Results indicate that the igneous crust in all these settings is highly transmissive and supports vigorous lateral fluid flow and (or) convection beneath the sediment cover driven by very small horizontal pressure gradients. Inter-CORK experiments suggest that the horizontal permeability of the young oceanic basement at these sites may be anisotropic, with higher values in the direction parallel to the axis of spreading and tectonic fabric and lower values in a ridge-normal cross-strike direction. Tracer experiments applied to ridge-parallel flow suggest that only a small fraction of the crust is well connected. CORKs also record the response of subseafloor formation fluid pressures to seafloor tidal loading, and, once the tidal responses are filtered out, response to tectonic strain events. Interpretations based on these responses and original two-dimensional modelling of ridge-normal fluid circulation in the crust suggest a scale dependence of permeability of igneous oceanic crust (higher values at larger scales up to tens of km), although recent three-dimensional models suggest a more limited scale effect. CORKs have also provided important geochemical and microbiological results from the igneous oceanic crust, although they are not reviewed in this paper.


Long‐Term Offshore Borehole Fluid‐Pressure Monitoring at the Northern Cascadia Subduction Zone and Inferences Regarding the State of Megathrust Locking

June 2023

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132 Reads

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2 Citations

The Cascadia subduction megathrust off the Pacific Northwest follows an “end member” seismogenic behavior, producing large (up to moment magnitude 9) but infrequent (every several hundred years) earthquakes and tsunamis. Crustal deformation associated with the ongoing plate convergence has been characterized by land‐based geodetic observations, but the state of locking across the full breadth of the seismogenic fault is poorly constrained. We report results of offshore monitoring of borehole fluid pressure, as a proxy for formation volumetric strain, at a site ∼20 km landward of the Cascadia subduction deformation front since 2010. The multi‐depth pressure records were plagued by hydrologic noise, but noise at the deepest monitoring level (303 m sub‐seafloor) abated in 2015. Subsequently, including at the times of regional large earthquakes that caused significant dynamic stressing, no persistent pressure transients are present above a threshold of 0.08 kPa imposed by unremovable oceanographic signals, corresponding to a strain detection limit of ∼16 nanostrain. Simple dislocation models using local megathrust geometry suggest a resolvable slip of <1 cm along a trench‐normal corridor beneath the borehole for a range of slip‐patch dimensions. A large slip patch can be well resolved even at considerable along‐strike distances from the borehole; for instance, ∼10 cm slip is detectable over a 200‐km strike range for a slip‐patch radius of ∼50 km. This high sensitivity for detecting slip, along with the lack of observed events, stands in stark contrast to observations at other subduction zones, and suggests that the Northern Cascadia megathrust is most likely fully locked.


Monitoring the 2021 M w 8.2 Alaska Earthquake by an Offshore Seismic and Fluid Pressure Observation Network and Implications for Ocean‐Crust Dynamic Coupling

September 2022

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62 Reads

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2 Citations

Ground shaking caused by earthquakes is accompanied by seafloor and sub-seafloor formation fluid pressure variations in offshore areas, but there have been few collocated observations of these signals. In this work, we report seismic and high-sampling-rate fluid pressure records of the 2021 Mw 8.2 Alaska earthquake by the Ocean Networks Canada (ONC) NEPTUNE observatory at an epicentral distance of ∼2,200 km in the northeast Pacific Ocean. The system comprises observatory nodes in various tectonic environments, with each node including buried broadband seismometers, seafloor pressure sensors, and, at two nodes, borehole pressure sensors. Seismic and tsunami waveforms of the Mw 8.2 earthquake were documented in detail. Seismic seafloor pressure variations (Psf) were dominated by Rayleigh waves of periods between 5 and 50 s, with peak amplitudes of 3–4 kPa at most sites. Waveform similarity and the linear scaling between Psf and vertical ground acceleration indicate forced acceleration of the water column being dominant in governing Psf during long-period surface-wave arrivals, with an additional component of elastic oscillation occurring at higher frequencies (>0.1 Hz) causing extra pressure signals. Analysis of formation pressure variations due to various types of ocean loading of distinctly different frequencies (e.g., tides, tsunami, and infragravity waves) shows stable one-dimensional vertical loading efficiencies that depend on lithology at each borehole site, with loading response being strongly influenced by the presence of free gas at shallow depths within the Cascadia accretionary prism. Inter-site comparisons of seismic and seafloor pressure waveforms demonstrate a key role of sediment thickness in the amplification of surface wave amplitudes.


Location of North Pond in the North Atlantic Ocean and positions of CORKs and CTD casts
Asterisks denote locations of the CORKs; + denotes the position of the two 2014 CTD casts. At the scale of the figure, Holes U1383B and U1383C occupy essentially the same position, labeled U1383B+C. Dashed line denotes pathway for cold dense deep waters inferred to be diluted AABW to reach North Pond from deeper water to the west, passing over the deepest sill on southwest side of North Pond. Base map made with GeoMapApp (www.geomapapp.org)⁵⁶.
Six-year records of temporal variability of bottom-water temperatures at Holes U1382A and U1383C
Hole U1382A temperatures are shown in red, Hole U1383C temperatures In blue. As noted in the Methods section, there is an absolute calibration offset between sensors, but relative variations track remarkably well.
CTD and seafloor pressure–temperature data spanning the small cooling event of April 2014
This event was clearly registered at both Holes U1382A and U1383C (Fig. 2). a Plots of Conservative Temperature, Absolute Salinity, neutral density, and oxygen saturation of bottom waters over North Pond for two CTD casts in 2014 that bracketed the cooling event. Properties from the 29 March CTD cast are shown in red, properties from the 14 April CTD cast in blue. The dark centers of the Absolute Salinity profiles show results of smoothing using a ∼0.5 m box filter. b Expanded record of seafloor pressures recorded at Hole U1382A (cyan) and bottom water in-situ temperatures recorded at Holes U1382A (red) and U1383C (blue) during the first six months of 2014, illustrating the fortnightly (∼biweekly) cycles in tidal amplitudes in North Pond and the times of the two 2014 CTD casts relative to these cycles.
Correlation function and example time lags between bottom-water temperatures at Holes U1382A and U1383C
a The correlation function between temperatures at the two holes as a function of time lag. b One month record of in-situ bottom water temperatures at Holes U1382A and U1383C from late March to late April, 2014, spanning the early April cooling event and two CTD casts. DG = data gap on data download, with brief spike on resumption of data logging. c, d Expanded three-month views of the major decreases in bottom-water temperatures in 2013 and 2017, respectively, illustrating typical 2- to 3.5-day lags of events at Hole U1383C. In b–d, the U1382A temperature record is shown in red, the U1383C record is shown in blue, and vertical arrows indicate example events seen at both locations.
Cartoon representing four stages of our conceptual model for renewal of North Pond bottom waters
The model involves slow heating of bottom waters by the geothermal flux and diapycnal mixing, setting the stage for cold water intrusions inferred to be from the leading edge of diluted AABW flowing over the deepest sill on the southwest side of North Pond. Plots labeled Θ and ρ represent idealized profiles of Conservative Temperature and density at each stage. Their scales and structures are schematic and intended only to illustrate relative changes in properties with depth. As shown in the bottom key, horizontal two-sided arrows represent relative horizontal tidal velocity variations, red upward arrows represent geothermal heating, red squiggly arrows represent heat input by diapyncal mixing, and dashed blue lines represent inferred low-temperature advective flow within permeable basement. a Heating of bottom waters below sill depth by the geothermal flux through the seafloor and by diapycnal mixing in the water column. The curvatures in the profiles in the deepest geothermally heated boundary layer are drawn to be consistent with comparable bottom boundary layers documented in Cascadia Basin⁴. b Preconditioned stage reached when the vertical extent of the heated bottom waters reaches sill depth, or slightly shallower. c Gravity current inflow stage, when the horizontal tidal velocities over the sill are weak, and colder, denser diluted AABW replaces the deepest bottom water in the basin. d Reset stage after the intrusion of diluted AABW and vertical mixing have reestablished near uniform water temperature to sill depth.
Geothermal heating and episodic cold-seawater intrusions into an isolated ridge-flank basin near the Mid-Atlantic Ridge

October 2021

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205 Reads

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4 Citations

Six-year records of ocean bottom water temperatures at two locations in an isolated, sedimented deep-water (∼4500 m) basin on the western flank of the mid-Atlantic Ridge reveal long periods (months to >1 year) of slow temperature rises punctuated by more rapid (∼1 month) cooling events. The temperature rises are consistent with a combination of gradual heating by the geothermal flux through the basin and by diapycnal mixing, while the sharper cooling events indicate displacement of heated bottom waters by incursions of cold, dense bottom water over the deepest part of the sill bounding the basin. Profiles of bottom water temperature, salinity, and oxygen content collected just before and after a cooling event show a distinct change in the water mass suggestive of an incursion of diluted Antarctic Bottom Water from the west. Our results reveal details of a mechanism for the transfer of geothermal heat and bottom water renewal that may be common on mid-ocean ridge flanks.


Maps and schematics. (a) Distribution of earthquakes. Red circles show events used for analyzing data from offshore boreholes and yellow for onshore Plate Boundary Observatory sites. Complete lists of earthquakes are given in Tables S2 and S3 in Supporting Information S1. (b) Distribution of observation sites. Barbed black and blue lines show convergent and other types of plate boundaries, respectively. Gray line shows Ocean Networks Canada offshore cables. The pair of open arrows show directions of current plate spreading; fossil plate‐spreading direction at 1026B/1027C is very similar (Wilson, 1993) and therefore not shown. (c) Diagram of CORK (Circulation Obviation Retrofit Kit) observatories. Slightly different designs are used for oceanic crust holes (1026B and 1027C) and accretionary prim hole (U1364A). (d) Cartoon illustration of the physics of formation fluid pressure variations driven by Rayleigh waves from distant earthquakes. Dynamic volumetric strain causes instantaneous changes in interstitial fluid pressure.
Seismic and formation fluid pressure observations of two earthquakes. (a, d) Comparison of radial‐component ground velocity VR (in red) and formation fluid pressure Pf (in blue) for the 2021 Mw = 8.1 Kermadec and the 2018 Mw = 7.1 Alaska earthquakes. Waveforms are bandpass filtered between 10 and 40 s. Vertical gray bars and T0 show estimated arrival time window of Rayleigh waves assuming group velocities between 2.75 and 4.1 km s⁻¹. Red and blue numbers show peak amplitudes of VR and Pf, respectively. (b, e) Ground velocity and its relation to formation fluid pressure during passing Rayleigh waves. Orange line and numbers show the linear regression fit for obtaining the characteristic pressurization ratio k. For offshore sites, effect of seafloor pressure is removed from the original formation fluid pressure (in light blue) before determining k. (c, f) Amplitudes of VR and Pf in the frequency domain. (g) Map showing seismic raypaths of the two earthquakes. Insets show specific locations of offshore instruments and boreholes.
Characteristic pressurization ratio k as a function of earthquake back azimuth for all sites. Error bars show 95% confidence interval. Dashed curves show the optimal cosine‐function fit for observations at the two oceanic‐crust sites. Complete lists of observed k values are given in Tables S4–S7 in Supporting Information S1. Results with a R² < 0.5 for the regression fit are not shown. Large azimuthal variation of k is observed at the oceanic‐crust sites (1026B and 1027C) only.
Shallow crust mechanical anisotropy inferred from in situ measurements and its relation to other seismic and hydrological observations. (a) Observed characteristic pressurization ratio k values allow determining formation‐matrix compressibility βm and its direction dependence (Text S2 in Supporting Information S1). For 1027C, observed direction‐dependent k values, marked by two green arrows, follow the amplitude range of the cosine curve in Figure 3. For U1364A, the mean (blue arrow) and standard deviation (blue dashed lines) of k measurements (with R² ≥ 0.5) are used for an estimation with uncertainty shown as the blue shade. Substantial azimuthal variation in βm is observed at the oceanic crust but not the prism. Inference based on vertical tidal loading is from Davis et al. (2000, 2012). n = porosity. (b) Comparison of seismic measurements of oceanic‐crust Vp anisotropy and the inferred Vp‐equivalent anisotropy of this study (Text S6 and Figure S6 in Supporting Information S1). Categories of the mid‐ocean ridges, in terms of spreading rate, are color coded. JdF, Juan de Fuca. Seismic studies referred to are listed in Table S8 in Supporting Information S1. (c) Schematic illustration of the interrelated mechanical and hydrological anisotropy, subseafloor flow pattern, and hydration state of the abundantly fractured shallow oceanic crust. Estimated values of permeability are from Fisher et al. (2008) and Davis, LaBonte, et al. (2010).
Seismic Formation Fluid Pressure Observations Reveal High Anisotropy of Oceanic Crust

October 2021

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105 Reads

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4 Citations

Plain Language Summary Hydrothermal circulation in the oceanic crust plays fundamental roles in the exchange of water, heat, and chemical constituents between the oceanic hydrosphere and lithosphere, in the hydration of the crust and upper mantle, and in the support of the subseafloor microbial biosphere. Water is carried primarily in faults and fractures created at the time of seafloor spreading, and thus constraints on their distribution and orientation are important. Such information has been provided by active‐source seismic surveys, and results have shown that compressional wave speeds in the directions of spreading—thus across local faults and fractures—are typically <20% lower than those along the structural fabric. Here, we report more direct determinations of the anisotropy at the 3.6‐Ma Juan de Fuca plate, using formation fluid pressure variations in sealed subseafloor boreholes caused by seismic surface waves from distant earthquakes. These observations are sensitive to formation compressibility of the upper couple of hundreds of meters of the igneous crust. The observed azimuthal variation in fluid pressurization reveals a contrast in compressibility across versus along the structural trend of roughly a factor of five, and a much higher degree of seismic anisotropy (>50%) than that determined from standard seismic velocity measurements.



Amplification and Tuning of Ground Motion at the Outer Cascadia Accretionary Prism

May 2021

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130 Reads

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4 Citations

Ground‐motion amplification in the outer Cascadia subduction zone accretionary prism has been documented previously by comparing earthquake and microseismic vertical ground‐motion and pressure records from an ONC/NEPTUNE Canada cabled observatory site on the outer prism to those from a site on the flank of the Juan de Fuca Ridge. Since then, four additional instruments became operational, and data, now spanning 10 years, include more than 100 large (Mw > 7) distant earthquakes. Well‐tuned response at the outer prism sites is observed in both vertical and horizontal components, with peaks in the spectral ratio of vertical velocity relative to nearby ocean crustal and continental bedrock sites (V/Vref) at 9 s, and in the intra‐site horizontal to vertical spectral ratio horizontal‐to‐vertical spectral ratio at 14 s, both with band widths of ±10% to 15% at half amplitude. The vertical response is consistent with ¼ wavelength compressional wave reinforcement, while the horizontal motion tuning most likely reflects the effects of the low velocity prism sediments on surface‐wave propagation. At the periods of maximum relative motion, outer prism surface‐wave vertical and horizontal accelerations are enhanced by factors of up to 15 and 25, respectively. Similar behaviour is seen in microseismic records from these sites, and, to a lesser extent, in earthquake records from temporarily deployed Cascadia Initiative seismometers along the outer Cascadia prism to the south. Such tuning and amplification must be accounted for when assessing the dynamic behavior of the prism and its basal fault at the time of large local earthquakes.


A Long-Term Geothermal Observatory Across Subseafloor Gas Hydrates, IODP Hole U1364A, Cascadia Accretionary Prism

December 2020

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103 Reads

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8 Citations

We report 4 years of temperature profiles collected from May 2014 to May 2018 in Integrated Ocean Drilling Program Hole U1364A in the frontal accretionary prism of the Cascadia subduction zone. The temperature data extend to depths of nearly 300 m below seafloor (mbsf), spanning the gas hydrate stability zone at the location and a clear bottom-simulating reflector (BSR) at ∼230 mbsf. When the hole was drilled in 2010, a pressure-monitoring Advanced CORK (ACORK) observatory was installed, sealed at the bottom by a bridge plug and cement below 302 mbsf. In May 2014, a temperature profile was collected by lowering a probe down the hole from the ROV ROPOS. From July 2016 through May 2018, temperature data were collected during a nearly two-year deployment of a 24-thermistor cable installed to 268 m below seafloor (mbsf). The cable and a seismic-tilt instrument package also deployed in 2016 were connected to the Ocean Networks Canada (ONC) NEPTUNE cabled observatory in June of 2017, after which the thermistor temperatures were logged by Ocean Networks Canada at one-minute intervals until failure of the main ethernet switch in the integrated seafloor control unit in May 2018. The thermistor array had been designed with concentrated vertical spacing around the bottom-simulating reflector and two pressure-monitoring screens at 203 and 244 mbsf, with wider thermistor spacing elsewhere to document the geothermal state up to seafloor. The 4 years of data show a generally linear temperature gradient of 0.055°C/m consistent with a heat flux of 61–64 mW/m². The data show no indications of thermal transients. A slight departure from a linear gradient provides an approximate limit of ∼10⁻¹⁰ m/s for any possible slow upward advection of pore fluids. In-situ temperatures are ∼15.8°C at the BSR position, consistent with methane hydrate stability at that depth and pressure.



Citations (42)


... Becker et al. (2025) review the technological evolution of these observatories and the scientific findings in oceanic basement enabled by them in the Ocean Drilling Program and the Integrated Ocean Dis- covery Program. Davis et al. (2025) review their applications to subduction zone settings and resultant scientific discoveries. Roy was also a world leader of the study of subsea methane hydrates using controlled-source seismic imaging (e.g., Hyndman and Davis 1992). ...

Reference:

Geophysical studies of the lithosphere and plate boundaries: special issue in honour of Roy D. Hyndman
Deep-sea borehole fluid pressure and temperature observations at subduction zones and their geodynamic implications

... Two review articles in this volume cover a field of research inspired by Roy's work, the use of borehole observatories to study the thermal, hydrological, and mechanical state of the subsea lithosphere and their variations in tectonic and nontectonic processes. Becker et al. (2025) review the technological evolution of these observatories and the scientific findings in oceanic basement enabled by them in the Ocean Drilling Program and the Integrated Ocean Dis- covery Program. Davis et al. (2025) review their applications to subduction zone settings and resultant scientific discoveries. ...

Monitoring subseafloor temperature and fluid pressure in sealed ODP/IODP boreholes to constrain in situ hydrological state and processes in igneous oceanic crust

... Researchers have used a variety of measurement systems to acquire seafloor heat-flow data since the 1950s, when the earliest measurements were made (Bullard 1954), such as high strength probes deployed at the end of a drill string for deep measurements in boreholes, and various styles of multipenetration tools for shallow measurements in marine sediments. The latter includes outrigger temperature sensors mounted on the outside of gravity-driven sediment corers, small probes controlled by submersibles or ROVs, and "violinbow" probes that consist of a steel lance for strength and an offset tube that houses temperature sensors (Bullard 1954;Langseth 1965;Hyndman et al. 1979;Davis and Fisher 2020). Many modern probes use the violin-bow design (Fig. 1), a robust configuration that allows for high spatial resolution and in situ thermal conductivity determinations made by firing a calibrated heat pulse into the sediment and measuring the thermal decay (Hyndman et al. 1979;Lister 1979). ...

Heat Flow, Seafloor: Methods and Observations
  • Citing Chapter
  • March 2020

... The Cascadia Subduction Zone (CSZ) that stretches 700 miles from Vancouver Island, Canada to Northern California is capable of producing up to a 9.0 magnitude (M9) megathrust earthquake [1] that would cause expansive damage and disruption across southern British Columbia, Washington, Oregon and north California [2]. As the interval since the last M9 earthquake in 1700 exceeds the average interval between CSZ events, local, state, regional, and federal emergency management professionals have conducted planning conferences and emergency response exercises to increase awareness of potential impacts and build preparedness for an M9 Cascadia megathrust earthquake. ...

Long‐Term Offshore Borehole Fluid‐Pressure Monitoring at the Northern Cascadia Subduction Zone and Inferences Regarding the State of Megathrust Locking

... Where high sampling rates have been possible at CORK installations (e.g., via ONC and DONET connections), and where co-located observations of seismic ground motion have been made, the magnitude and phase relations between ground motion and fluid-pressure oscillations can be determined in offshore settings. This has led to a confirmation of the high fidelity of CORK formation pressure observations at seismic frequencies, and to novel constraints on formation mechanical properties (Sun et al. 2021;Sun and Davis 2022). In this section, we provide examples of recent progress in studying the dynamic fluid pressure signals associated with the passage of seismic waves. ...

Monitoring the 2021 M w 8.2 Alaska Earthquake by an Offshore Seismic and Fluid Pressure Observation Network and Implications for Ocean‐Crust Dynamic Coupling

... Intense mixing of AABW has been documented in the neighboring Romanche Fracture Zone (Polzin et al., 1996); most likely, the same processes should occur in other channels and fracture zones of the abyssal tropical Atlantic, where fast AABW flows are observed (Morozov et al., 2018). The long-term changes in AABW properties have also been measured in a small isolated basin west of the Mid-Atlantic Ridge (Becker et al., 2021), where geothermal heating and cooling by AABW inflows influence the temperature of abyssal waters. ...

Geothermal heating and episodic cold-seawater intrusions into an isolated ridge-flank basin near the Mid-Atlantic Ridge

... Where high sampling rates have been possible at CORK installations (e.g., via ONC and DONET connections), and where co-located observations of seismic ground motion have been made, the magnitude and phase relations between ground motion and fluid-pressure oscillations can be determined in offshore settings. This has led to a confirmation of the high fidelity of CORK formation pressure observations at seismic frequencies, and to novel constraints on formation mechanical properties (Sun et al. 2021;Sun and Davis 2022). In this section, we provide examples of recent progress in studying the dynamic fluid pressure signals associated with the passage of seismic waves. ...

Seismic Formation Fluid Pressure Observations Reveal High Anisotropy of Oceanic Crust

... Horizontal-component spectra used in the ratios are computed using the geometric mean of the transverse-and radial-component spectra. A listing of the earthquakes and details of the processing are given in Davis and Farrugia (2021). An example pressure spectral ratio (P fm /P sf ) for a single earthquake at Hole U1364A is shown for comparison. ...

Amplification and Tuning of Ground Motion at the Outer Cascadia Accretionary Prism

... After the perturbation caused by drilling had dissipated, the temperature profile, determined with sensors distributed along the length of a thermistor cable suspended inside the casing, was generally linear, reaching the temperature expected at the regionally defined depth of the bottom simulating reflector (BSR; Fig. 5a), but showed signs of local transient flow where the hole intersected a thrust fault (Davis et al. 1995). A hole farther north in the Cascadia prism, drilled and instrumented with an ACORK in 2010 in Hole U1364A (near Hole 889C where that CORK installation was not fully sealed), showed no resolvable departure from a steady conductive thermal state whatsoever, and a temperature at the depth of the BSR that also precisely matched the theoretical limit for gas hydrate stability for a methane-seawater mixture (Becker et al. 2020;Fig. 5a). ...

A Long-Term Geothermal Observatory Across Subseafloor Gas Hydrates, IODP Hole U1364A, Cascadia Accretionary Prism

... In the IODP (Integrated Ocean Drilling Program), the long-term borehole monitoring system has been installed into boreholes, comprising an array of volumetric strain-meters, broadband seismometers, tiltmeters, three-component geophones, three-component accelerometers, and thermometers (Kimura et al., 2013;Solomon et al., 2019). Long-term borehole monitoring systems and permanent seafloor observatories have multiple sensors installed throughout the water column, seafloor surface, and subsurface. ...

Listening Down the Pipe
  • Citing Article
  • March 2019

Oceanography