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Instrument Development

posted Jul 6, 2011, 1:32 PM by mikutas   [ updated Dec 20, 2012, 11:22 AM by Matthew Alford ]

Mooring Technology

Deployment of the HOT Profiling Mooring, Hawaii Current moored profiling technology is severely limited by battery power. This means that if we want to observe with a profiling mooring for a year, one must suffice with daily profiles - or worse. Since internal waves, which contain about half the ocean's energy, have higher frequencies than this, we wish to profile at least once an hour or so - resulting in a short (44-day) time series. To improve on this situation, we are developing a next-generation moored profiling system. With Bruce Howe and Time McGinnis (also at APL), we are modifying a McLane profiler, to be inductively charged from an external power supply. This can be a cabled observatory node, or a large moored battery pack for deployment at non-cabled sites. We are also developing the needed inductive, acoustic and radio communication technologies to allow real-time telemetry back to a nearby ship or shore.

We are also working with McLane to add new instruments and capability to the McLane whenever we can, beginning with different gearbox ratios for faster profiling speeds, rechargeable battery packs, a Nitrate sensor, and a Nortek aquadopp velocity sensor.  Working with our colleagues at OSU, we have successfully integrated chi-pods for direct turbulence measurements into two of our profiler.

Finally, check out our state-of-the-art mooring system we maintain off the Washington Coast.

Fiber-optic Salinity/Density Sensor: the ocean refractometer

refractometer image  Understanding the smallest motions in the ocean, which have scales smaller than a millimeter, is important to advance our understanding of the climate, since circulation models cannot resolve turbulence and have to parameterize it. These scales are poorly understood because they are so small, and because salinity is very hard to measure. Using technology modified from AIDS research, Alford developed a sensor half the diameter of a human hair to sense these smallest-scale fluctuations in ocean refractive index. These are closely related to salinity fluctuations, which to-date have been measured by conductivity and temperature measurements. Measuring salinity from one small sensor reduces "spiking" resulting from mismatched sensor responses. Testing began summer 2001 in Puget Sound, Washington, and initial results showed that in fact the so-called Batchelor cutoff for salinity could be resolved. In addition, however, the sensor responds to the velocity signal of the turbulence, making it an optical "shear probe," but precluding resolution of low-frequency signals. I was able to reduce, but not eliminate, this effect.
Schematic diagram of a coupler used as a refractometer. Light shone into one fiber enters the 1-cm long, 30-µm-radius fused section in the center, and couples into the two output fibers in a ratio which depends sensitively on the refractive index in a one-wavelength-wide (~ 1.5 µm) surrounding radius.  

Northwest Coastal Oceanography

posted Jul 6, 2011, 1:32 PM by mikutas   [ updated Dec 19, 2012, 9:20 PM ]

Embedded in the California Current System (CCS), the low-frequency oceanography of the Washington (WA) continental shelf (Figure 1) has been studied in a great detail over the last several decades owing in part to its high productivity, and lately owing to its sensitivity to harmful alga blooms, hypoxic and anoxic events, and ocean acidification. Overall biological productivity in the CCS, which flow along the western boundary of the United States and southern Canadian Pacific coast, is generally attributed to seasonal upwelling of nutrient-rich deep waters to the continental shelf (Hickey and Banas, 2003). This upwelling is usually caused by the stress of winds blowing equatorward on the ocean's surface along the coastal boundary. It might be expected that overall productivity along the boundary coast would be correlated with the strength of the upwelling-favorable wind stress at a given location. However, in the CCS, this relationship does not hold in a way that the seasonal average coastal chlorophyll concentrations increase fivefold from northern California to southern Vancouver Island, counter to
the magnitude of alongshelf wind stress, which decreases by a factor of eight over this region (Hickey and Banas, 2008).

Figure 1: Map showing the location of the NEMO moorings(star) and gliderline (blackline), as well as the NDBC Cape Elizabeth meteorological buoy 46021.
Observed barotropic tidal flow and time-mean vector of the California Current are shown with  a black ellipse and arrow, respectively, with scaleas indicated.
The red and blue arrows are the semidiurnal energy flux computed from observations and model, respectively. The colormap shows conversion of barotropic
 tidal energy to baroclinic tides. The black and yellow dashed line is the boundary of the Olympic Coast National Marine Sanctuary. Contour levels are each
100m until 500m, then each 200m thereafter.

Previous studies suggested that the northern CCS has several mechanisms that can produce upwelled nutrient concentrations comparable to those in regions with much greater wind stress. Top candidates include a persistent nutrient supply through the dynamics of the Strait of Juan de Fuca (Crawford and Dewey, 1988), freshwater input from the Columbia river plume (MacCready et al., 2009), the presence of the Juan de Fuca eddy, and enhanced upwelling by the Juan de Fuca canyon (MacFadyen and Hickey, 2010). In ways that are not yet fully understood, the unique aspects of the Washington continental shelf may conspire to boost its productivity (Hickey and Banas, 2008).

Internal waves and mixing are likely key players in transportation of nutrients and DO from the deep layer to the eutrophic zone. Limited by the observation data on the WA continental shelf, no previous studies have reported a detailed study on the internal waves or mixing in this regions. We have recently designed and deployed a new three-component observing system consisting of two moorings and a glider line off the Washington coast. A rich, variable internal wave field is seen, appearing to feature some of the stronger nonlinear internal waves (NLIW) yet reported on continental shelves, when viewed
as a fraction of the water depth. I propose to study the characteristics of internal waves on the WA continental shelf, the generation mechanism and dissipation of NLIWs and their potential influence on the nutrient supply in this region.

We're interested in the oceanography off our coast.  As part of the NANOOS program, we now maintain the Cha-Ba surface buoy, its subsurface analogue, and a glider line.  We collectively refer to these systems as NEMO.

NEMO schematic

Figure 2: Schematic of the NEMO (Northwest Enhanced Moored Observatory) system, with Seaglider, NEMO-subsurface, and the surface mooring Cha' Ba.

Figure 3: Large, ubiquitous nonlinear internal waves (NLIW) have been observed at the NEMO mooring location---associated with rapid vertical movement of density surfaces and strong velocities and velocity shear.  These waves may be an important key to the increased productivity on the Washington coast, with prior research showing that they may be important to supplying nutrients to the shelf.

Figure 4:  Top: Synthetic Aperture Radar (SAR) satellite image showing sea-surface roughness patterns off the Washington Coast offshore of Olympic National Park (Lake Ozette and Point of Arches). The image shows two regions ("a" and "b" in black boxes) of nonlinear internal waves (NLIW), as indicated by coherent bands of rough and smooth water associated with wave troughs (convergence) and crests (divergence) respectively.  White bathymetry contours suggest topographic steering of the waves in box "b" similar to the refraction of surface waves as they approach the beach.  Bottom: A time series of temperature at a depth of 15 m on the NEMO surface mooring (Cha' Ba), verifying that this is a propagating NLIW.

Global Internal Waves

posted Jul 6, 2011, 1:31 PM by mikutas   [ updated Dec 14, 2011, 1:00 PM by WaveChasers APL ]

General circulation models (e.g. Samelson, 1998) indicate that the thermohaline circulation is highly sensitive to the global magnitude and distribution of mixing. Recent observations (e.g. Polzin et al 1997) highlight the inhomogeneity of mixing. Therefore, a global map of mixing would benefit climate modeling, as well as our understanding of biological productivity and pollutant dispersal. Since global measurements of mixing are impractical, another way of estimating the global mixing distribution is to map the energy flux into internal waves, and then to measure their subsequent long-range propagation.

Figure 1: 
(top) Depth-integrated, annual-mean near-inertial energy-flux vectors are plotted from 60 historical moored records. The length of each arrow is logarithmic, with references indicated at upper left. Moorings with |F|< 0.1 kW/m appear as a black dot without an arrow; white dots indicate moorings which were unusable. The few instances of poleward propagation are plotted in white. Color map indicates annual-mean energy-flux from the wind to near-inertial mixed-layer motions from Alford (2001). The color scale is logarithmic and is indicated at upper left. The box in the NW Pacific is discussed in the text.

(bottom) Arrows are as in (a) but for the M2-tidal band. Color map denotes internal-tide conversion using the TPXO5 model (Egbert and Ray, 2000), courtesy of G. D. Egbert. The lines in the western Pacific and near Hawaii are discussed in the text. The inset in each panel shows a histogram of the poleward component of the flux for all moorings.

The first step is to map the distribution of the two primary internal-wave sources, the wind, which generates near-inertial waves, and surface-tidal flow over topography (Egbert and Ray, 2000), leading to internal tides. The wind-flux portion is calculated (Alford, 2001) by using the NCEP/NCAR reanalysis wind fields, which incorporate observations over many years and locations into a dynamically consistent framework, to drive a simple model of the mixed-layer response. The energy flux is then given by the scalar product of the wind stress and the mixed-layer current. Ongoing work involves examining the high-latitude dependence of the fluxes (as the response gets faster at high latitude, the NCEP winds become more and more inadequate for the job), and the interannual variability of the fluxes.

The global distribution of the energy flux available for internal waves is plotted below for the wind (top) and the tides (bottom, courtesy of G. Egbert). The greatest wind inputs occur at midlatitudes during wintertime, associated with travelling storms. Large tidal inputs (red regions) occur where the surface tide flows perpendicular to rough bottom features.

The subsequent horizontal flux for each can be measured using historical moored records by solving for the lowest two modes and computing <u'p'>, where u' is the baroclinic velocity and p' is the baroclinic pressure anomaly. Near-inertial fluxes are large following wintertime storms, and are equatorward, since waves generated at the inertial frequency become evanescent poleward of their generation site. The tidal fluxes are usually directed away from strong topography.

Since then, Zhongxiang Zhao and I have been working on further refining our estimates of the global distribution of internal-tide energy flux from both moorings and altimetry, which has resulted in a series of papers and an exciting new NSF proposal.

Harper Simmons and I are working together to compare models and observations in order to determine the analogous fate of the near-inertial motions.

Abyssal Flows and Mixing

posted Jul 6, 2011, 1:29 PM by mikutas   [ updated Dec 20, 2012, 10:25 AM by Matthew Alford ]

The abyssal ocean was once thought to be stagnant.  Recent work is showing it to be anything but.  This is important since the water that has sunk at the poles must return via tortuous routes to lower latitudes - and then must upwell to complete the loop.  This flow is known as the "conveyor belt" or the "meridional overturning circulation," and is a key element of the ocean's circulation and a vital part of the Earth's climate.  This upwelling appears to occur at least in part due to turbulent mixing - which warms the cold water by mixing with the warmer water above.  This mixing seems to happen at special "hotspots."  This is why internal waves matter (since their breaking often leads to the mixing).  Other processes such as hydraulics are also important.

Observations in the Samoan Passage (Figures 1-2), part of our ongoing work in a critical "choke point" in the conveyor belt.
Figure 1: A breaking lee wave as water spills over a sill 5000 m beneath the surface in the Samoan Passage.  (Top) temperature (colors) and "Thorpe temperatures" (profiles) - think of jagged profiles as showing turbulence as colder water has been swept above warmer water.  (Bottom) velocity (colors) and turbulent dissipation estimated from these overturns (contours).  

Figure 2: Map of the Samoan Passage bathymetry and vectors showing our measurements of the transport of the coldest water (colors refer to two temperature classes).

These flows are also very intermittent in time, as seen by observations from another of our moorings north of Hawaii.  A strong cold flow detected at our profiling mooring at station ALOHA (figure 3) showed a 250-m-high overturn, indicating mixing 10,000 times stronger than usually seen in the open ocean - but only once in a 2-1/2 year record.  This suggests that mixing in the deep flows is intermittent not only in space, but time too.

Figure 3: A cold event at station ALOHA detected in October 2010.  (Upper left) Bathymetry and flow vectors.  Gray indicates depth < 4400 m.  Arrows are mean velocity averaged from 4000 m to the sill depth from the selected time periods (indicated at upper right).  (Bottom) Entire 2.5-year time-series from the combined thermistor chain records.   (Upper right) measured eastward and northward velocity.

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