| Contributors | Affiliation | Role |
|---|---|---|
| Frossard, Amanda | University of Georgia (UGA) | Co-Principal Investigator |
| Rauch, Shannon | Woods Hole Oceanographic Institution (WHOI BCO-DMO) | BCO-DMO Data Manager |
Particles were generated using a high-capacity marine aerosol generator. Briefly, the generator consists of a 20 centimeter (cm) diameter model ocean-atmosphere system entirely made of borosilicate glass and Teflon. The "ocean" holds ~40 liters (L) of seawater, with a total depth of 90 cm. Unmodified seawater from the ship’s clean seawater line, ~3 meters (m) below the sea surface, was continuously pumped at 4 liters per minute (L min-1) into the bottom of the generator. Seawater continuously drained over the annular rim, constantly refreshing the surface of the "ocean" and preventing the formation of bubble rafts. Seawater from the base of the generator was pumped through the conical inlet of the Venturi at a flow rate of 3 L min-1. Hydrated ultrapure air was pumped through two ports at the constricted throat of the Venturi at a combined air flow rate of 5 L min-1.
The Venturi produced bubbles at a depth of 74 cm below the air-water interface. Bubble bursting at the air-water interface emitted mPMA into the model "atmosphere" of the generator. The model atmosphere is the 97-cm deep, open headspace above the water surface. Ultrapure hydrated sweep air flowed through the headspace above the water surface at 70 L min-1 and transported particles for sizing. Air was sampled through three glass ports at the top of the generator at ~6 L min-1 for the particle sizing instrumentation. Sweep air at a flow rate of 70 L min-1 was hydrated and maintained at ~80% relative humidity by modulating the temperature applied to the mist chambers.
To measure particle numbers and sizes, air was sampled from the glass port in the generator's headspace directly to a custom-fabricated, 46 cm length, diffusion dryer with 1.91 cm inner diameter stainless steel mesh. This air was directly pulled into the Aerodynamic Particle sizer (APS; TSI Model 3321) at a rate of 4 L min-1 for the sheath flow and 1 L min-1 for the sample flow. Prior to entering the APS, air was sub-sampled at a flow rate of ~0.5 L min-1 to the Scanning Electrical Mobility Spectrometer (SEMS; Brechtel Manufacturing, Inc. Model 2100) using a custom-fabricated, stainless-steel splitter (1.59 cm ID with a 0.476 cm ID sidearm sampling port). After passing through the 1 micrometer (µm) size-cut impactor, air flowed through an additional Nafion dryer, before entering the SEMS neutralizer.
The diffusion dryer combined with the Nafion dryer dehydrated the particles entering the SEMS to ~50% relative humidity. The silica gel in the dryer was changed each day after ~23 hours of sampling. The difference between the initial relative humidity at the start of each sampling period and the final relative humidity, after ~23 hours, measured by the SEMS was ~5% relative humidity. Dry particle number size distributions for the SEMS were calculated from the measured relative humidity and a size-dependent hygroscopicity for submicron mPMA. The temperature difference between the generator and the APS instrument caused heating and drying of the particles. Dry particle number size distributions for the APS were corrected using a size-dependent hygroscopicity for supermicron mPMA. The relative humidities used to apply the hygroscopicity parameters were calculated from the partial pressure difference calculated using the Clausius-Clapeyron equation and the measured temperature difference.
The scan times for both instruments were ~1 min, with an additional delay time of 20 seconds for each scan in the SEMS. After the relative humidity corrections were applied, particle number size distributions were averaged over 5 min intervals for the routine sampling periods. For the flow characterizations, the particle number size distributions were averaged over the total number of scans at each Venturi air flow set point (~10 scan for each). The SEMS measured the size and number of mPMA with diameters between 0.010 and ~0.85 µm. The APS measured the size and number of mPMA with aerodynamic diameters between ~0.52 µm and 20 µm. Aerodynamic diameters from the APS were converted to mobility diameters using an average assumed density of sea spray particles in that size range of 2.12 grams per cubic centimeter (g cm-3). Mobility diameters were assumed to be equal to geometric mean diameters, under the assumption that the particles were spherical. Particle number size distributions from the APS and SEMS were then merged at the size bins greater and smaller than 0.235 µm geometric mean diameters, respectively. Distributions were not smoothed at the merge point.
The number production efficiency (PEnum) and mass production efficiency (PEmass) of mPMA particles were calculated. The PEnum was calculated for each size bin as the product of the particle number concentration of the bin and the total flow rate from the Venturi plus sweep air, all divided by the air detrainment rate. The PEmass was calculated similarly but with the product of the calculated volume concentration and the assumed mPMA density for each bin (1.84 g cm-3 for submicron; 2.14 g cm-3 for supermicron) in place of the number concentration. The resulting PEnum has units of L-1 and PEmass has units of µg L-1.
- Imported original file "Frossard PE Combined.csv" into table "999300_v1_penum_and_pemass" to the BCO-DMO system.
- Converted "Atlantic Standard Date Time" from M/D/YY H:MM format to ISO 8601 format (%Y-%m-%dT%H:%M), representing AST/ADT.
- Created new column "ISO_DateTime_UTC" by converting the Atlantic Standard Time values (UTC-4/UTC-3) to UTC, formatted as %Y-%m-%dT%H:%MZ.
- Renamed columns to comply with BCO-DMO naming conventions.
- Saved the final file as "999300_v1_penum_and_pemass.csv".
| File |
|---|
999300_v1_penum_and_pemass.csv (Comma Separated Values (.csv), 328.38 KB) MD5:e4fda60376c1ee12b2815b72d87e862c Primary data file for dataset ID 999300, version 1 |
| Parameter | Description | Units |
| Cruise_Number | Cruise number AE2113 (summer) or AE2303 (winter) | unitless |
| Atlantic_Standard_Date_Time | Date time (Atlantic Standard Time (AST)) of each measurement in ISO 8601 format | unitless |
| ISO_DateTime_UTC | Date time (UTC) of each measurement in ISO 8601 format | unitless |
| PE_mass | Mass production efficiency | micrograms per liter (ug/L) |
| PE_number | Number production efficiency | per liter (1/L) |
| Dataset-specific Instrument Name | Scanning Electrical Mobility Spectrometer (SEMS; Brechtel Manufacturing, Inc. Model 2100) |
| Generic Instrument Name | Brechtel 2100 scanning electrical mobility spectrometer |
| Dataset-specific Description | Prior to entering the APS, air was sub-sampled at a flow rate of ~0.5 L min-1 to the Scanning Electrical Mobility Spectrometer (SEMS; Brechtel Manufacturing, Inc. Model 2100) using a custom-fabricated, stainless-steel splitter (1.59 cm ID with a 0.476 cm ID sidearm sampling port). |
| Generic Instrument Description | The Brechtel 2100 scanning electrical mobility spectrometer is an ultra-fast particle mobility spectrometer used to measure particle number size distributions. Applications include identifying key properties of air pollution and aerosol-cloud interactions. This instrument outputs measurements of aerosol number size distribution in addition to real-time measurements of temperature, relative humidity, and pressure. The SEMS 2100 operates by classifying particles based on their electrical mobility, which is influenced by their size and charge. Aerosol sample flow range: 0.1 - 2.0 lpm; sheath flow range: 2.5 - 12 lpm; particle concentration range: 1 - 10 million per cubic centimetre. It is fully automated for long-term unattended operation. Selectable particle diameter size range: 0.005-0.3 um; 0.005 - 1.0 um; 0.01 - 2.0 um. Operating temperature: 15 - 35 degC. Operating pressure: 200 - 1000 mb. |
| Dataset-specific Instrument Name | marine aerosol generator |
| Generic Instrument Name | Marine Aerosol Generator |
| Dataset-specific Description | Particles were generated using a high-capacity marine aerosol generator. |
| Generic Instrument Description | A high-capacity marine aerosol generator deployed at sea, using near-surface seawater and purified air to create a lab-based approximation of ocean-atmosphere aerosol systems.
Example device described here:
Frossard, A. A., Long, M. S., Keene, W. C., Duplessis, P., Kinsey, J. D., Maben, J. R., Kieber, D. J., Chang, R. Y. ‐W., Beaupré, S. R., Cohen, R. C., Lu, X., Bisgrove, J., & Zhu, Y. (2019). Marine Aerosol Production via Detrainment of Bubble Plumes Generated in Natural Seawater With a Forced‐Air Venturi. Journal of Geophysical Research: Atmospheres, 124(20), 10931–10950. Portico. https://doi.org/10.1029/2019JD030299 |
| Dataset-specific Instrument Name | Aerodynamic Particle sizer (APS; TSI Model 3321) |
| Generic Instrument Name | TSI 3321 Aerodynamic Particle Sizer |
| Dataset-specific Description | To measure particle numbers and sizes, air was sampled from the glass port in the generator's headspace directly to a custom-fabricated, 46 cm length, diffusion dryer with 1.91 cm inner diameter stainless steel mesh. This air was directly pulled into the Aerodynamic Particle sizer (APS; TSI Model 3321) at a rate of 4 L min-1 for the sheath flow and 1 L min-1 for the sample flow. |
| Generic Instrument Description | The TSI 3321 Aerodynamic Particle Sizer (APS) measures the size distribution and concentration of aerosol particles in the diameter range 0.5 - 20 um. The aerosol sample is accelerated toward the detection area, where it crosses two slightly overlapping laser beams. The rate of acceleration is determined by the particle size. Larger particles accelerate more slowly due to their greater inertia. Light scattered by each particle is focused onto a photodiode. The use of twin lasers results in a two-crested signal. The peak-to-peak time-of-flight is used to determine the particle velocity, and thus its aerodynamic size. The amplitude of the signal may be used to provide an alternative measure of particle size through light-scattering techniques. |
| Website | |
| Platform | R/V Atlantic Explorer |
| Start Date | 2021-07-22 |
| End Date | 2021-08-01 |
| Description | See additional information at R2R: https://www.rvdata.us/search/cruise/AE2113 |
| Website | |
| Platform | R/V Atlantic Explorer |
| Start Date | 2023-01-18 |
| End Date | 2023-01-28 |
| Description | See additional information at R2R: https://www.rvdata.us/search/cruise/AE2303 |
NSF Award Abstract:
The oceans hold a massive quantity of organic carbon that is greater than all terrestrial organic carbon biomass combined. Nearly all marine organic carbon is dissolved. On average, it is thousands of years old, chemically stable, and carried throughout the entire ocean several times before complete removal. However, little is known about the processes that produce and remove this old carbon, referred to as refractory dissolved organic carbon (RDOC). One potential removal pathway involves RDOC adhering onto the surfaces of rising bubbles produced by breaking waves. The bubbles ultimately burst at the sea surface, ejecting tiny particles (primary marine aerosol, “PMA”) that carry the RDOC into the atmosphere. Most of this PMA organic carbon is associated with the smallest particles (less than 1 μm diameter) that drift in the atmosphere for several days to weeks. During this time, RDOC in these particles can be degraded photochemically (by sunlight), partially transported landward, and/or returned to the sea. When this RDOC is converted to inorganic carbon (e.g., carbon dioxide) or degraded to more reactive constituents in the atmosphere, it is effectively removed from the marine RDOC reservoir. Based on preliminary results, the annual rate at which RDOC is removed from the ocean by this process is similar to all other known RDOC losses (interactions with particles, biological degradation, and hydrothermal circulation), except for photochemical degradation in seawater. Building on this prior research, this project will identify seasonal changes in the removal of RDOC from the oceans through this process during three research cruises to the northwestern Atlantic Ocean. Results from this project will provide important findings about the coupled ocean-atmosphere loss of RDOC and improve understanding of the role of RDOC in the global carbon cycle and Earth's climate. The research will involve two early career faculty, and will provide training for undergraduate, graduate, and postdoctoral researchers.
Radiocarbon (C-14) measurements indicate that RDOC comprises 19 to 40 % of the organic carbon associated with PMA produced by bursting bubbles at the sea surface. Injection of RDOC into the atmosphere in association with PMA is a potentially important process that removes as much as 2 to 20 Tg RDOC yr-1 from the oceans. This project will measure seasonal variations in the PMA-mediated emission of marine RDOC to the atmosphere by quantifying: (1) the fraction of RDOC in PMA OC and (2) its relationship to the abundance of biologically produced labile and semi-labile dissolved organic matter in near surface seawater. These relationships will be evaluated at the Bermuda Atlantic Time-series Station during three research cruises (one in July, two in January). During the cruises, the investigators will measure: (1) the natural abundance C-14 values for PMA and its organic source materials in seawater; (2) the dynamic and equilibrium surface tension and physical properties of seawater, including bubble size distributions; (3) concentrations of major ions, organic carbon, carbohydrates, peptides and proteins, and surfactants in PMA; and (4) chromophoric dissolved organic matter (CDOM) and the concentrations of dissolved organic carbon, chlorophyll a, major ions, carbohydrates, peptides and proteins, and surfactants in near-surface seawater and in the sea-surface microlayer. Based on these chemical measurements and physical properties, this study will reveal the magnitude and potential controls on RDOC inputs into the atmosphere as a component of PMA.
This award reflects NSF's statutory mission and has been deemed worthy of support through evaluation using the Foundation's intellectual merit and broader impacts review criteria.
The Surface Ocean Lower Atmosphere Study (SOLAS) program is designed to enable researchers from different disciplines to interact and investigate the multitude of processes and interactions between the coupled ocean and atmosphere.
Oceanographers and atmospheric scientists are working together to improve understanding of the fate, transport, and feedbacks of climate relevant compounds, and also weather and hazards that are affected by processes at the surface ocean.
Oceanographers and atmospheric scientists are working together to improve understanding of the fate, transport, and feedbacks of climate relevant compounds.
Physical, chemical, and biological research near the ocean-atmosphere interface must be performed in synergy to extend our current knowledge to adequately understand and forecast changes on short and long time frames and over local and global spatial scales.
The findings obtained from SOLAS are used to improve knowledge at process scale that will lead to better quantification of fluxes of climate relevant compounds such as CO2, sulfur and nitrogen compounds, hydrocarbons and halocarbons, as well as dust, energy and momentum. This activity facilitates a fundamental understanding to assist the societal needs for climate change, environmental health, weather prediction, and national security.
The US SOLAS program is a component of the International SOLAS program where collaborations are forged with investigators around the world to examine SOLAS issues ubiquitous to the world's oceans and atmosphere.
» International SOLAS Web site
US-SOLAS (4 MB PDF file)
Other SOLAS reports are available for download from the US SOLAS Web site
The Ocean Carbon and Biogeochemistry (OCB) program focuses on the ocean's role as a component of the global Earth system, bringing together research in geochemistry, ocean physics, and ecology that inform on and advance our understanding of ocean biogeochemistry. The overall program goals are to promote, plan, and coordinate collaborative, multidisciplinary research opportunities within the U.S. research community and with international partners. Important OCB-related activities currently include: the Ocean Carbon and Climate Change (OCCC) and the North American Carbon Program (NACP); U.S. contributions to IMBER, SOLAS, CARBOOCEAN; and numerous U.S. single-investigator and medium-size research projects funded by U.S. federal agencies including NASA, NOAA, and NSF.
The scientific mission of OCB is to study the evolving role of the ocean in the global carbon cycle, in the face of environmental variability and change through studies of marine biogeochemical cycles and associated ecosystems.
The overarching OCB science themes include improved understanding and prediction of: 1) oceanic uptake and release of atmospheric CO2 and other greenhouse gases and 2) environmental sensitivities of biogeochemical cycles, marine ecosystems, and interactions between the two.
The OCB Research Priorities (updated January 2012) include: ocean acidification; terrestrial/coastal carbon fluxes and exchanges; climate sensitivities of and change in ecosystem structure and associated impacts on biogeochemical cycles; mesopelagic ecological and biogeochemical interactions; benthic-pelagic feedbacks on biogeochemical cycles; ocean carbon uptake and storage; and expanding low-oxygen conditions in the coastal and open oceans.
| Funding Source | Award |
|---|---|
| NSF Division of Ocean Sciences (NSF OCE) |