DEPOSITION AND RESUSPENSION OF FINE PARTICLES IN A RIVERINE DEAD ZONE

Citation
E. Tipping et al., DEPOSITION AND RESUSPENSION OF FINE PARTICLES IN A RIVERINE DEAD ZONE, Hydrological processes, 7(3), 1993, pp. 263-277
Citations number
NO
Categorie Soggetti
Water Resources
Journal title
ISSN journal
08856087
Volume
7
Issue
3
Year of publication
1993
Pages
263 - 277
Database
ISI
SICI code
0885-6087(1993)7:3<263:DAROFP>2.0.ZU;2-L
Abstract
Particulate matter suspended in the River Severn (Shropshire, UK) cons ists chiefly of clay-sized mineral particles, together with living and dead micro-organisms (algae and bacteria). Its concentration depends strongly on discharge, but the particle size distribution shows no sys tematic variability. For most samples, the particle volume is log-norm ally distributed with respect to diameter, the mean diameter being ca. 9 mum. The particles are mainly aggregates, including some with linea r dimensions of the order of tens or hundreds of micrometres. Particle density depends appreciably on size, decreasing from ca. 2.5 x 10(6) g m-3 at a diameter of 2.5 mum to ca. 1.3 x 10(6) g m-3 at 20 mum. The collision efficiency factor for particle aggregation is estimated to be 0.01-0.03. At low discharge, the 'dead zone' in the River Severn at Leighton is a well defined region of stagnant water behind a gravel b ar. The rate of deposition of fine particles on its bed is of the orde r of tens of grams per square metre per day. Resuspension requires a c ritical bed shear velocity of 0.03-0.04 m s-1, which occurs at main ri ver discharges greater than about 150 m3 s-1. Under such conditions th e gravel bar is underwater and the dead zone is a region of highly tur bulent return flow. A simple mechanistic model of particle dynamics in the dead zone accounts reasonably well for particle accumulation rate s when run with parameter values based on measured particle and hydrau lic properties. Calculations with the model suggest that most of the s edimentation flux to the dead zone bed is due to particles with equiva lent sphere diameters in the range 30-240 mum. Simulations indicate th at deposition proceeded continuously during spring and summer, whereas repeated deposition and resuspension occurred in autumn and winter.