The IEEE Seventh Working Conference on Current Measurement Technology

Current and Wave Monitoring and Emerging Technologies

March 13-15 | Bahia Hotel | San Diego, CA, USA

 
     

ADCP estimates of Reynolds and bottom stress

M.J. Howarth

Status: Accepted

Bidston Observatory
Bidston Hill
Prenton , Wirral United Kingdom
CH43 7RA

Phone: + 44 151 653 8633
Email: mjh@pol.ac.uk

Co-Authors:

Field measurements of Reynolds and bottom stress are rare and difficult to make but are required for studies of large scale dynamical balances and of small scale dissipation and exchange processes, including the concept of the constant stress layer. Recently a simple to apply technique has been reported in which Reynolds stress profiles can be calculated from the variance of along beam data recorded by fast sample, O(1 Hz), high frequency Acoustic Doppler Current Profilers (ADCPs).

The technique has been applied in seven experiments in the north-west European continental shelf seas involving the deployment of 0.6 and 1.2 MHz standard broadband ADCPs mounted in sea-bed frames. The sites ranged from high tidal energy, shallow (20 m deep) to low tidal energy, deeper (110 m). The ADCPs recorded data with a variety of sample regimes, from 2 Hz (recording every ping) to 1 Hz (averaging 8 pings) to 0.5 Hz (averaging over four or five pings); bin sizes ranged from 0.25 to 1 m. For most of the experiments the ADCP estimates of shear production of turbulence were complemented by estimates of turbulence dissipation obtained from repeated deployments from a ship of the FLY microstructure profiler.

In two of the experiments the ADCP near bed Reynolds / bottom stress estimates were tested against independent estimates from toroidal electro-magnetic current meters measuring the three components of current (vertical and both horizontal) at 8 Hz. These current meters were fitted to a frame, at 0.3, 0.6 and 0.9 m above the bed, deployed near the ADCP. In all cases the correlation coefficient squared between the two sets of Reynolds stress estimates was 0.7. In addition the three components of turbulence intensity (and hence the degree of anisotropy) were estimated from the electro-magnetic current meter records. This cannot be estimated from the ADCP data, unless the ADCP is fitted with a vertical beam, but is important for interpretation of the results.

One objective of these studies is to improve representation of processes in 2- and 3-dimensional numerical models and to test the results. At its very simplest bottom stress can be related to the depth-averaged flow via a quadratic drag coefficient  estimates from the different sites were all in the region of 0.001, smaller than the value used in most depth-averaged numerical models (about 0.0025). Three avenues are being explored to understand this result
a) corroborating evidence is being sought, mainly from bulk calculations.
b) possible errors either inherent in the technique or related to the ADCP set up (bin size, sample interval, tilt) are being investigated and, where possible, quantified.
c) physical reasons for the discrepancy are being considered.

Submitted on November 11, 2002