Newly recognized turbidity current structure can explain prolonged flushing of submarine canyons

Runaway turbidity currents stretch into the deep ocean to form the largest sediment accumulations on Earth. Seabed-hugging flows called turbidity currents are the volumetrically most important process transporting sediment across our planet and form its largest sediment accumulations. We seek to understand the internal structure and behavior of turbidity currents by reanalyzing the most detailed direct measurements yet of velocities and densities within oceanic turbidity currents, obtained from weeklong flows in the Congo Canyon. We provide a new model for turbidity current structure that can explain why these are far more prolonged than all previously monitored oceanic turbidity currents, which lasted for only hours or minutes at other locations. The observed Congo Canyon flows consist of a short-lived zone of fast and dense fluid at their front, which outruns the slower moving body of the flow. We propose that the sustained duration of these turbidity currents results from flow stretching and that this stretching is characteristic of mud-rich turbidity current systems. The lack of stretching in previously monitored flows is attributed to coarser sediment that settles out from the body more rapidly. These prolonged seafloor flows rival the discharge of the Congo River and carry ~2% of the terrestrial organic carbon buried globally in the oceans each year through a single submarine canyon. Thus, this new structure explains sustained flushing of globally important amounts of sediment, organic carbon, nutrients, and fresh water into the deep ocean.

[1]  C. Cooper,et al.  Turbidity Current Measurements in the Congo Canyon , 2013 .

[2]  Lionel Carter,et al.  Damaging sediment density flows triggered by tropical cyclones , 2017 .

[3]  Sébastien Migeon,et al.  Marine hyperpycnal flows: initiation, behavior and related deposits. A review , 2003 .

[4]  D. Hanes,et al.  Comparison of field observations of the vertical distribution of suspended sand and its prediction by models , 1996 .

[5]  Peter J. Talling,et al.  How are subaqueous sediment density flows triggered, what is their internal structure and how does it evolve? Direct observations from monitoring of active flows , 2013 .

[6]  Peter D. Thorne,et al.  Interpreting acoustic backscatter from suspended sediments of different and mixed mineralogical composition , 2012 .

[7]  Lionel Carter,et al.  Insights into Submarine Geohazards from Breaks in Subsea Telecommunication Cables , 2014 .

[8]  Gerard V. Middleton,et al.  Sediment Deposition from Turbidity Currents , 1993 .

[9]  Yu-Huai Wang,et al.  Cyclone-induced hyperpycnal turbidity currents in a submarine canyon , 2012 .

[10]  Ben Kneller,et al.  The structure and fluid mechanics of turbidity currents: a review of some recent studies and their geological implications , 2000 .

[11]  J. de Leeuw,et al.  Morphodynamics of submarine channel inception revealed by new experimental approach , 2016, Nature Communications.

[12]  D. Mastbergen,et al.  Breaching in fine sands and the generation of sustained turbidity currents in submarine canyons , 2003 .

[13]  Octavio E. Sequeiros,et al.  Experimental study on self‐accelerating turbidity currents , 2009 .

[14]  W. M. Ewing,et al.  Congo Submarine Canyon , 1964 .

[15]  R. Schneider,et al.  Transport of terrestrial organic carbon to the oceans by rivers: re-estimating flux- and burial rates , 2000 .

[16]  D. Inman,et al.  Currents in Submarine Canyons: An Air-Sea-Land Interaction , 1976 .

[17]  Albert Palanques,et al.  Flushing submarine canyons , 2006, Nature.

[18]  Dick R. Mastbergen,et al.  The importance of breaching as a mechanism of subaqueous slope failure in fine sand , 2002 .

[19]  N. L. Bue,et al.  Different types of sediment gravity flows detected in the Var submarine canyon (northwestern Mediterranean Sea) , 2012 .

[20]  W. D. McCaffreya,et al.  Spatio-temporal evolution of velocity structure , concentration and grain-size stratification within experimental particulate gravity currents , 2002 .

[21]  H. G. Greene,et al.  Caught in the act: the 20 December 2001 gravity flow event in Monterey Canyon , 2002 .

[22]  R. T. Casey,et al.  Designing for Turbidity Currents in the Congo Canyon , 2016 .

[23]  P. Thorne,et al.  An overview on the use of backscattered sound for measuring suspended particle size and concentration profiles in non-cohesive inorganic sediment transport studies , 2014, CSR 2014.

[24]  J. Syvitski,et al.  Hyperpycnal plume formation from riverine outflows with small sediment concentrations , 2001 .

[25]  B. Dennielou,et al.  Morphology, structure, composition and build-up processes of the active channel-mouth lobe complex of the Congo deep-sea fan with inputs from remotely operated underwater vehicle (ROV) multibeam and video surveys , 2017 .

[26]  R. Francois,et al.  Sound absorption based on ocean measurements: Part I: Pure water and magnesium sulfate contributions , 1982 .

[27]  P. Faure,et al.  Efficient organic carbon burial in the Bengal fan sustained by the Himalayan erosional system , 2007, Nature.

[28]  J. Syvitski,et al.  Turbidity Currents Generated at River Mouths during Exceptional Discharges to the World Oceans , 1995, The Journal of Geology.

[29]  R. Bagnold Auto-suspension of transported sediment; turbidity currents , 1962, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[30]  J. Syvitski,et al.  Cyclone‐driven deep sea injection of freshwater and heat by hyperpycnal flow in the subtropics , 2010 .

[31]  D. S. Mueller,et al.  Validation of Streamflow Measurements Made with Acoustic Doppler Current Profilers , 2007 .

[32]  Peter D. Thorne,et al.  A review of acoustic measurement of small-scale sediment processes , 2002 .

[33]  A. Pruski,et al.  Organic matter characterization and distribution in sediments of the terminal lobes of the Congo deep-sea fan: Evidence for the direct influence of the Congo River , 2015 .

[34]  G. P. Holdaway,et al.  Constraining acoustic backscatter estimates of suspended sediment concentration profiles using the bed echo , 1995 .

[35]  L. Rosenfeld,et al.  In‐situ measurements of velocity structure within turbidity currents , 2004 .

[36]  R. J. Urick,et al.  The Absorption of Sound in Suspensions of Irregular Particles , 1948 .

[37]  T. Nilsen,et al.  Atlas of Deep-Water Outcrops , 2007 .

[38]  S. Tan,et al.  Errors in the Bed Shear Stress as Estimated from Vertical Velocity Profile , 2006 .

[39]  Yusuke Fukushima,et al.  Self-accelerating turbidity currents , 1986, Journal of Fluid Mechanics.

[40]  P. Thorne,et al.  Backscattering from a suspension in the near field of a piston transducer , 1995 .

[41]  J. Thepaut,et al.  The ERA‐Interim reanalysis: configuration and performance of the data assimilation system , 2011 .

[42]  A. Pruski,et al.  The Congolobe project, a multidisciplinary study of Congo deep-sea fan lobe complex: Overview of methods, strategies, observations and sampling , 2017 .

[43]  Anchun Li,et al.  Event-driven sediment flux in Hueneme and Mugu submarine canyons, southern California , 2010 .

[44]  A. Khripounoff,et al.  Turbidity events observed in situ along the Congo submarine channel , 2009 .

[45]  D. Caress,et al.  Origins of large crescent-shaped bedforms within the axial channel of Monterey Canyon, offshore California , 2010 .

[46]  R. Schiebel,et al.  Onset of submarine debris flow deposition far from original giant landslide , 2007, Nature.

[47]  R. Francois,et al.  Sound absorption based on ocean measurements. Part II: Boric acid contribution and equation for total absorption , 1982 .

[48]  J. H. Hughes Clarke First wide-angle view of channelized turbidity currents links migrating cyclic steps to flow characteristics , 2016, Nature Communications.

[49]  J. Syvitski,et al.  Geomorphic/Tectonic Control of Sediment Discharge to the Ocean: The Importance of Small Mountainous Rivers , 1992, The Journal of Geology.

[50]  J. Eggenhuisen,et al.  Concentration-Dependent Flow Stratification In Experimental High-Density Turbidity Currents and Their Relevance To Turbidite Facies Models , 2012 .

[51]  B. Dennielou,et al.  Direct observation of intense turbidity current activity in the Zaire submarine valley at 4000 m water depth , 2003 .

[52]  P. Talling,et al.  Preconditioning and triggering of offshore slope failures and turbidity currents revealed by most detailed monitoring yet at a fjord-head delta , 2016 .