Physical controls on hypoxia in Chesapeake Bay : a numerical modeling study
Physical controls on hypoxia in Chesapeake Bay : a numerical modeling study
dc.contributor.author | Scully, Malcolm E. | |
dc.date.accessioned | 2013-07-29T16:05:39Z | |
dc.date.available | 2014-10-22T08:57:21Z | |
dc.date.issued | 2013-03-14 | |
dc.description | Author Posting. © American Geophysical Union, 2013. This article is posted here by permission of American Geophysical Union for personal use, not for redistribution. The definitive version was published in Journal of Geophysical Research 118 (2013): 1239–1256, doi:10.1002/jgrc.20138. | en_US |
dc.description.abstract | A three-dimensional circulation model with a relatively simple dissolved oxygen model is used to examine the role that physical forcing has on controlling hypoxia and anoxia in Chesapeake Bay. The model assumes that the biological utilization of dissolved oxygen is constant in both time and space, isolating the role that physical forces play in modulating oxygen dynamics. Despite the simplicity of the model, it demonstrates skill in reproducing the observed variability of dissolved oxygen in the bay, highlighting the important role that variations in physical forcing have on the seasonal cycle of hypoxia. Model runs demonstrate significant changes in the annual integrated hypoxic volume as a function of river discharge, water temperature, and wind speed and direction. Variations in wind speed and direction had the greatest impact on the observed seasonal cycle of hypoxia and large impacts on the annually integrated hypoxic volume. The seasonal cycle of hypoxia was relatively insensitive to synoptic variability in river discharge, but integrated hypoxic volumes were sensitive to the overall magnitude of river discharge at annual time scales. Increases in river discharge were shown to increase hypoxic volumes, independent from the associated biological response to higher nutrient delivery. However, increases in hypoxic volume were limited at very high river discharge because increased advective fluxes limited the overall length of the hypoxic region. Changes in water temperature and its control on dissolved oxygen saturation were important to both the seasonal cycle of hypoxia and the overall magnitude of hypoxia in a given year. | en_US |
dc.description.embargo | 2013-09-14 | en_US |
dc.description.sponsorship | The funding for this research was obtained from NSF Grant OCE-0954690 and supported by NOAA via the U.S. IOOS Office (Award Numbers NA10NOS0120063 and NA11NOS0120141) and managed by the Southeastern Universities Research Association. | en_US |
dc.format.mimetype | application/pdf | |
dc.identifier.citation | Journal of Geophysical Research 118 (2013): 1239–1256 | en_US |
dc.identifier.doi | 10.1002/jgrc.20138 | |
dc.identifier.uri | https://hdl.handle.net/1912/6123 | |
dc.language.iso | en_US | en_US |
dc.publisher | John Wiley & Sons | en_US |
dc.relation.uri | https://doi.org/10.1002/jgrc.20138 | |
dc.subject | Hypoxia | en_US |
dc.subject | Stratification | en_US |
dc.subject | Mixing | en_US |
dc.subject | Wind | en_US |
dc.title | Physical controls on hypoxia in Chesapeake Bay : a numerical modeling study | en_US |
dc.type | Article | en_US |
dspace.entity.type | Publication | |
relation.isAuthorOfPublication | 0b665fcc-025c-4b03-aae9-d61bbeb030c9 | |
relation.isAuthorOfPublication.latestForDiscovery | 0b665fcc-025c-4b03-aae9-d61bbeb030c9 |