Contributors | Affiliation | Role |
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Stanley, Rachel | Wellesley College | Principal Investigator |
Spivak, Amanda | Woods Hole Oceanographic Institution (WHOI) | Co-Principal Investigator |
Howard, Evan | Woods Hole Oceanographic Institution (WHOI) | Contact |
Ake, Hannah | Woods Hole Oceanographic Institution (WHOI BCO-DMO) | BCO-DMO Data Manager |
Marsh Pond noble gas concentrations and saturations.
Noble gas concentrations were sampled using copper tube sampling (~13g samples) with a handheld pump, and extracted and analyzed at the WHOI Isotope Geochemistry Facility using peak height manometry and isotope dilution mass spectrometry techniques. Uncertainties are calculated from replicate precision and are similar to expected analytical uncertainties reported by WHOI IGF. Noble gas saturation concentrations are calculated using the unpublished solubility functions of Dempsey Lott III and William Jenkins (WHOI Isotope Geochemistry Facility (http://www.whoi.edu/IGF)), derived for all five gases from the same instrument over conditions near one atmosphere and atmospheric partial pressures of the noble gases. Saturation concentrations were calculated using a Monte Carlo approach in which temperature and salinity (the dominant sources of uncertainty in the saturation concentration) were allowed to randomly vary within the standard deviation bounds for the environmental variability (1 degree Celsius, 0.5 on PSS-78) with 3000 iterations, and the mean variance of all iterations converted to a one standard deviation uncertainty for the saturation concentration based on the measured temperature and salinity at the sonde location. The same approach was used to combine measurement uncertainties with saturation concentration uncertainties and determine the one standard deviation uncertainty of the gas saturation states. These uncertainties were simultaneously determined for all gases at each timepoint, so that the full suite of noble gases vary with respect to each other. Variations of temperature and salinity around the pond were not random with respect to time (i.e. a location with high temperature relative to the sonde at 10am generally had higher temperature at noon and 2pm as well). Therefore the saturation state of any given noble gas varies systematically across each time series; the difference between concentrations at consecutive timepoints is conserved because the random uncertainty associated with the individual measurements is an order of magnitude lower than the systematic uncertainty associated with shifts in temperature and salinity compared to that expected from the sonde.
Because of the sampling method (smaller than usual copper tube samples, relatively slow and uneven flow from hand pumping compared to Niskin sampling), it is possible that atmospheric He was not adequately flushed from the copper tube and contaminated the samples for that gas only—we urge caution in the interpretation of the He results, and do not use these measurements in the associated manuscript (Howard et al., submitted to Limnol. Oceanog. Letters). There was no evidence that this issue would affect the other gases in a detectable manner, because of their higher solubility. One noble gas sample was flagged as having a pattern of saturation states consistent with contamination by a bubble during sampling. He, Ne, and Ar concentrations and saturation states from this sample are likely too large, but Kr and Xe are insensitive to bubble processes and any effect of sample contamination in minor on these more soluble gases.
No recalibration or post processing of sonde data was found to be necessary. Noble gas saturation state is calculated as ([C]/[C]sat-1)*100%, meaning 0% is at atmospheric equilibrium, values >0 are supersaturated, and values <0 are undersaturated with respect to atmospheric equilibrium. All noble gas saturation concentrations are adjusted for local atmospheric pressure using data from a nearby marshtop meteorological tower, with that data available at the link (http://www.whoi.edu/IGF/) described in the analytical methods section.
BCO-DMO Data Processing Notes:
-reformatted column names to comply with BCO-DMO standards
-separated DateTime column into two columns (date and time)
-reformatted date to "yyyy-mm-dd"
-filled in blank cells with "nd"
-added ISO_DateTime_UTC column
File |
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noble_gases.csv (Comma Separated Values (.csv), 4.90 KB) MD5:2a1c3d3b30cea8d43fa82a577cfac5b4 Primary data file for dataset ID 670694 |
Parameter | Description | Units |
date | Sampling date; yyyy-mm-dd | unitless |
time | Sampling time; HH:MM | unitless |
lat | Latitude; N is positive | decimal degrees |
lon | Longitude; E is positive | decimal degrees |
He | Helium (He) concentration | micromoles per kilogram (umol/Kg) |
He_stdev | Standard deviation of He concentration | umol/Kg |
He_sat | Saturated He concentration | umol/Kg |
He_sat_stdev | Standard deviation of saturated He concentration | umol/Kg |
dHe | dHe concentration | percent |
dHe_stdev | Standard deviation of dHe concentration | percent |
He_flag | He concentration flag | unitless |
Ne | Neon (Ne) concentration | umol/Kg |
Ne_stdev | Standard deviation of Ne concentration | umol/Kg |
Ne_sat | Saturated Ne concentration | umol/Kg |
Ne_sat_stdev | Standard deviation of saturated Ne concentration | umol/Kg |
dNe | dNe concentration | percent |
dNe_stdev | Standard deviation of dNe concetration | percent |
Ne_flag | Ne concentration flag | unitless |
Ar | Argon (Ar) concentration | umol/Kg |
Ar_stdev | Standard deviation of Ar concentration | umol/Kg |
Ar_sat | Saturated Ar concentration | umol/Kg |
Ar_sat_stdev | Standard deviation of saturated Ar concentration | umol/Kg |
dAr | dAr concentration | percent |
dAr_stdev | Standard deviation of dAr concentration | percent |
Ar_flag | Ar concentration flag | unitless |
Kr | Krypton (Kr) concentration | umol/Kg |
Kr_stdev | Standard deviation of Kr concentration | umol/Kg |
Kr_sat | Saturated Kr concentration | umol/Kg |
Kr_sat_stdev | Standard deviation of saturated Kr concentration | umol/Kg |
dKr | dKr concentration | percent |
dKr_stdev | Standard deviation of dKr concentration | percent |
Kr_flag | Kr concentration flag | unitless |
Xe | Xenon (Xe) concentration | umol/Kg |
Xe_stdev | Standard deviation of Xe concentration | umol/Kg |
Xe_sat | Saturated Xe concentration | umol/Kg |
Xe_sat_stdev | Standard deviation of saturated Xe concentration | umol/Kg |
dXe | dXe concentration | percent |
dXe_stdev | Standard deviation of dXe concentration | percent |
Xe_flag | Xe concentration flag | unitless |
notes | Notes | unitless |
ISO_DateTime_UTC | Date/Time (UTC) ISO formatted | unitless |
Dataset-specific Instrument Name | Isotope mass spectrometer |
Generic Instrument Name | Isotope-ratio Mass Spectrometer |
Dataset-specific Description | Extracted and analyzed noble gas concentrations |
Generic Instrument Description | The Isotope-ratio Mass Spectrometer is a particular type of mass spectrometer used to measure the relative abundance of isotopes in a given sample (e.g. VG Prism II Isotope Ratio Mass-Spectrometer). |
Dataset-specific Instrument Name | Handheld pump |
Generic Instrument Name | Pump |
Dataset-specific Description | Used with copper tube for noble gas sampling |
Generic Instrument Description | A pump is a device that moves fluids (liquids or gases), or sometimes slurries, by mechanical action. Pumps can be classified into three major groups according to the method they use to move the fluid: direct lift, displacement, and gravity pumps |
Website | |
Platform | shoreside Massachusetts |
Start Date | 2012-07-27 |
End Date | 2012-08-15 |
Description | Plum Island, MA; LTER sites |
Extracted from the NSF award abstract:
This project will address how rates of benthic microalgal production respond to eutrophication and geomorphological changes in human-impacted tidal creeks. Excess nutrient loading increases benthic algal biomass and likely stimulates production rates but the magnitude of nutrient and geomorphological effects on rates of production is unknown. Will changes in benthic algal productivity affect algal-bacterial coupling? Furthermore, how is algal-bacterial coupling affected by geomorphological changes, which may be exacerbated by excess nutrient loading but can also occur in pristine marshes?
This project will take advantage of the infrastructure of the TIDE project, a long-term saltmarsh eutrophication experiment at the Plum Island Ecosystem - Long Term Ecological Research site in Northeastern Massachusetts. Specifically, the PIs will measure benthic metabolism and examine algal- bacterial coupling in fertilized and ambient nutrient tidal creeks in the first field season. The following field season, they will compare sediment metabolism and carbon dynamics on slumped tidal creek walls (i.e. areas where low marsh has collapsed into the tidal creek) to that on the bottom of tidal creeks. In both years, gross and net production will be determined using an innovative triple oxygen isotope technique and traditional dissolved oxygen and inorganic carbon flux measurements. Comparisons between these methods will be useful in informing studies of sediment metabolism. Lipid biomarkers will be used to characterize the sources of organic matter to creek sediments, and stable isotope analysis of bacterial specific biomarkers to identify the sources of organic carbon utilized by sediment bacteria. The biomarkers will reveal whether sediment bacteria use organic matter substrates, such as benthic microalgal carbon, selectively or in proportion to availability. Overall, results from the proposed study will provide important information about how sediment carbon dynamics in shallow tidal creeks respond to long term eutrophication. Furthermore, findings will enhance understanding of the role of tidal creeks in coastal biogeochemistry.
Funding Source | Award |
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NSF Division of Ocean Sciences (NSF OCE) |