Nitrogen Emission/Deposition Ratios for Air Pollution Sources That Contribute to the Nitrogen Loading of Tampa Bay Environmental Protection Commission of Hillsborough County Pollution Recovery Fund Agreement Number 06-02A Mid-Term Progress Report September 21, 2008 Prepared by Noreen D. Poor, Principal Investigator 1. Project Abstract Local agencies, institutions, universities, corporations, and governments that are involved in bay monitoring and management, e.g., as stakeholders in the Tampa Bay Estuary Program or as members of the Tampa Bay Regional Planning Council, have estimated that to prevent further impairment of bay waters, nitrogen flowing into Tampa Bay must be reduced by 17 tons per year (TBNEP, 1996). Assessing the reductions or gains in nitrogen deposition for changes in power plant configurations or for levels of vehicular traffic, e.g., are difficult to assess without atmospheric transport modeling. Conversion factors for major sources and source categories in Hillsborough County that relate tons of nitrogen emitted to tons of nitrogen deposited to Tampa Bay will be developed from atmospheric deposition modeling with the CALMET/CALPUFF modeling system. This will not only aid bay managers in assessing atmospheric nitrogen emission reductions made in recent years, but will reveal which sources/source categories, if controlled, would influence most the bay water quality. 2. Emissions Inventory In the third six months of the project, the CALPUFF model was run with the USEPA 2002 emissions inventory prepared for air pollutants SO2, NOx, and NH3 as described in the previous progress report, with two exceptions: Hillsborough County off-road NOx 1 emissions were reduced from 14,454 tons/year to 1,900 tons/year, consistent with a local estimate of ship traffic through Port of Tampa in 2002; and Pinellas County non-point SO2 emissions were reduced by 24,974 tons/year to omit the combustion emission anomaly. 3. CALPUFF Model File Management The “rule of thumb” applied to solving problems that occurred in running the CALPUFF model was that at the end of the project the files created for the project could be easily transferred to and run by interested parties, e.g., without the need to recompile model or to deal with “bugs” in the model. Attempts were made to run all of the sources (point, area, and hourly emissions from power plants) for one year of meteorological data in one file. This approach was not successful because at some point during a modeling run the number of puffs tracked by the model exceeded the default limit and the run terminated. To solve this problem, the input file was then split into three files: power plant hourly emissions, point source emissions, and area source emissions. The point source emissions included industrial and municipal stationary sources and smaller power plants plus ammonia emissions for all power plants. Area source emissions included on-road, off-road, and non-point source emissions. Initial runs were made using a small number of discrete receptors to represent monitoring sites in Hillsborough and Pinellas Counties and also with a gridded network of 1200 receptors across the Tampa Bay watershed. Concentrations of SO2 and NOx predicted by the CALPUFF model at these receptors were compared with measurements made at area monitors. The earliest model simulations revealed that the line source representations of on-road emissions resulted in unusual spatial gradients, for example, high pollutant concentrations at the ends of the line rather than along the length of the line. The line source representation of on-road emissions was abandoned, and on-road emissions were added to the volume source representation of county-wide emissions. Recall from the second progress report that for each county in the CALPUFF modeling domain, the on-road, offroad, and non-point emissions were summed and input as a volume source centered at the county seat with an effective emission height of zero (0.0) m, an initial lateral 2 dispersion (σy) of 40 km and an initial vertical dispersion (σy) of 100 m. County-level emissions were input as time invariant. 4. Deposition Parameters The CALPUFF model dry deposition parameters were reviewed and updated, where appropriate, for a standard temperature of 25 o C (298 K) and a standard pressure of 1 atm. For nitrogen oxides (NOx=NO+NO2), dry deposition parameters for NO2 were selected rather, e.g., than a weighted average of NO and NO2, an approach which was consistent with the CALPUFF default NOx molecular weight of 46—the molecular weight of NO2. Although NOx is conserved, the fraction of NOx that is NO2 changes rapidly as a pollutant is released from the tailpipe of a car (Kenty et al., 2007) and the 2002 ambient ratio observed at a monitoring site in urban Tampa was 80% (v/v). Gas diffusivities reported by Massman (1998) for SO2, NO2, NH3, and from Durham and Stockberger (1985) for HNO3 were used (Table 1). Henry’s Law coefficients were obtained from Seinfeld and Pandis (1998) and converted to a dimensionless form (v/v) as shown in Equation 1, where is the dimensionless Henry’s Law coefficient (Table 1), H is the Henry’s Law coefficient (M/atm), R is the gas constant (0.08205 atm⋅L/mol⋅K), and T is temperature (298 K). Equation 1: = (H⋅R⋅T)-1 The enhanced gas solubility coefficient α* was calculated from the ratio of H to H*, where H* is the effective Henry’s Law coefficient for reactive gases, e.g., SO2, HNO3, and NH3 absorbing into seawater (pH 7.9). Equilibrium constants for aqueous phase reactions for these gases were taken from Seinfeld and Pandis (1998). 3 Reactivity for NH3 (ANH3) was estimated by first calculating a cuticle resistance (RcuticleNH3) as given by Sutton et al. (1998) (Equation 2), where RH is the relative humidity, and next estimating the relative reactivity according to Equation 3 (Scire et al., 2000). The average relative humidity measured at Tampa International Airport in 2002 was 76% (NCDC, 2008). CALPUFF default values for SO2 reactivity (ASO2) and cuticle resistance (Rcuticle-SO2) were 8 and 30 s/cm, respectively. CALPUFF default reactivities for SO2, NO2, and HNO3 were kept (Table 1). Equation 2: Rcuticle-NH3 = 2⋅exp[(100-RH)/12] Equation 3: ANH3 = ASO2⋅ Rcuticle-SO2/Rcuticle-NH3 Mesophyllic resistances (Rm) were calculated according to Equation 4 (Wesely, 1989), where f0 is defined as the normalized activity. Effective Henry’s Law coefficients were determined at pH 6.5 (e.g., near neutral). Values for f0 were zero for SO2, HNO3, and NH3, and 0.1 for NO2 (Wesely, 1989). The CALPUFF default mesophyllic resistance for NO2 is 5. Equation 4: Rm = (H*/3000+100* f0)-1 Particle diameter controls particle dry deposition rates. Atmospheric particles typically have a log-normal distribution that can be described by a geometric mean diameter and a geometric standard deviation. The CALPUFF default distributions are based on the MESOPUFF II chemistry, where SO2 and NO2 undergo atmospheric reactions with NH3 to form fine particle SO4 and NO3. In a coastal atmospheric, HNO3 reacts with coarse particles of suspended sea salt to form NaNO3 instead of NH4NO3 and thus the NO3 distribution has a coarse particle mode (Table 2) (Dasgupta et al., 2007; Poor et al., 2006). 4 The MESOPUFF II chemistry does not include a pathway for coarse particle nitrate formation, however, to the extent that the model predicts NH4NO3 formation, its deposition velocity will be calculated as that for NaNO3. Preliminary equilibrium modeling suggests that in a warm, humid, coastal environment such as Tampa, for conditions under which CALPUFF will predict NH4NO3 formation— another words, when NH3 is in excess of the amount needed to fully neutralize atmospheric H2SO4—the excess NH3 remains in the gas-phase. Thus, the CALPUFFmodeled fraction of NOx that becomes NH4NO3 is expected to be small. CALPUFF limits the values and formats that can be entered for each of the deposition parameters. For SO2 and HNO3, deposition rates were calculated from CALPUFF simulations with large values for the enhanced gas solubility coefficient α*, e.g. 106, and again with a value of 1,000, with no change observed in the numerical results. Table 1. CALPUFF Model Dry Deposition Parameters for Gases a b Pollutant SO2 NOx/NO2 HNO3 NH3 Diffusivity, cm2/s 0.128 0.159 0.118 0.232 Input into CALPUFF as 1000 Input into CALPUFF as 0.001 α* 6.45E+06a 1.00E+00 1.22E+09a 2.24E+01 Reactivity 8 8 18 16 Mesophyllic Resistance, s/cm 0b 0b 0b 0b Henry' s Law 3.33E-02 4.09E+00 1.95E-07 6.60E-04 Table 2. CALPUFF Model Dry Deposition Parameters for Aerosols Pollutant SO4 NO3 Geometric Mean Diameter, µm 0.48 3.50 Geometric Standard Deviation, µm/µm 2.00 1.90 5 The CALPUFF default values for rainfall scavenging of HNO3, NO3, and NH3 were not changed based on the results of recent research by Calderón et al. (2007, 2008). 5. Receptor Grid With a gridded network of 1200 receptors (2-km grid scale), the power plant, area, and point sources input files took about 1 day, 1 week, and 2 weeks, respectively, to run. The longer runs of 1-2 weeks were on occasion prematurely terminated due to power interruptions, for example, from a local lightning strike. A replacement gridded network with 198 receptors was prepared to provide complete coverage of the Tampa Bay watershed but with more distance between each receptor (Figure 1). This shortened the run times to about 0.5 days, 1 day, and 2 days for the power plant, area, and point source emissions files, respectively. 6 Figure 1. CALPUFF receptor grid across the Tampa Bay watershed used to estimate nitrogen deposition to Tampa Bay. The scale for the terrain map of central Florida has units of meters. 6. Observed versus Modeled Concentrations and Atmospheric Deposition Rates With the above changes to the CALMET model input files, comparisons between predicted and measured concentrations of SO2 and NOx improved, especially for longerterm averages such as an annual average. Emissions of SO2 are predominantly from coal- and oil-fired power plants for which hourly emission data were available; moreover, 7 13 local monitoring sites reported hourly observations for SO2 for all or part of 2002. Figure 2 shows the average annual SO2 concentration gradients from combined CALPUFF modeling of all sources (e.g., power plant, point, and area sources) along with the average annual SO2 concentration measured at local monitoring sites. The disagreement between modeled and measured concentrations tends to be the greatest where such a steep concentration gradient exists and is a likely result of the underlying differences in modeled versus actual meteorology coupled with limitations in the model’s ability to simulate atmospheric turbulence. Figure 2. Modeled and measured average annual SO2 concentrations in the Tampa Bay watershed. Colored contour lines are CALPUFF-modeled and posted numbers are measured SO2 concentrations. Concentration units are µg/m3. 8 Figure 3 shows modeled and measured average annual NOx concentrations for the Tampa Bay watershed. Roughly 50% of the NOx emissions are from power plants for which hourly emission data were available. In Hillsborough and Pinellas Counties fewer monitoring sites reported hourly NOx concentrations as compared with sites reporting SO2 concentrations. As was seen for SO2, steep concentration gradients exist near power plants and other major sources, and the modeled NOx concentrations are in reasonable agreement with observations seen in Hillsborough County, but are lower than observations reported at a monitoring site in Pinellas County. Figure 3. Modeled and measured average annual NOx concentrations in the Tampa Bay watershed. Colored contour lines are CALPUFF-modeled and posted numbers are measured NOx concentrations. Concentration units are µg/m3. 9 A preliminary estimate of the 2002 average ambient air concentrations and atmospheric nitrogen deposition rates are summarized in Tables 3 and 4. Also shown is an estimate of the fraction of the concentrations and nitrogen deposition rates that comes from Hillsborough County emission sources. Table 3. Summary of ambient air pollutant concentrations in the Tampa Bay watershed. Units are µg/m3. a Urban Rurala CALPUFFb a SO2 11 3.0 9.1 SO4 3.5 2.5 0.65 NOx 25 17 12 HNO3 1.3 0.62 1.2 NO3 1.7 1.5 0.46 NH3 1.8 1.6 1.2 NH4 0.72 0.56 0.32 Poor et al., 2006. Data averaged from June 2002 to April 2003 for all but NO3, which was averaged for May 2002. b Averaged for 2002. c Calculated from modeled SO4 and NO3 concentrations. The CALPUFF modeling simulations do not produce as much sulfur and nitrogen as has been locally measured (Table 3). Long-distant transport of particle sulfur and nitrogen, e.g., SO4, NO3, and NH4 to the Tampa Bay watershed is expected and could explain the reason why modeled under-predict measured concentrations. Another explanation is that choices made for CALPUFF modeling parameters cause the underprediction. To evaluate the latter explanation, the CALPUFF model simulations will be done with a change in the volume source dimensions, e.g., from a lateral dispersion of 40 km to 20 km and for a change in the nighttime NOx to HNO3 transformation rate. Kenty et al. (2007) gave evidence that nighttime transformation of NO to NO2, which precedes the oxidation of NOx to HNO3, occurred at rates similar to those seen during daytime when the process is thought to driven by photolytic reactions. 10 Table 4. Summary of nitrogen deposition rates to land surface of the Tampa Bay watershed. Units are kg-S/ha/year or kg-N/ha/year. Inferred Drya Weta CALPUFF Dry Wet SO2-S SO4-S NOx-N HNO3-N NO3-N NH3-N NH4-N 2.04 -- 0.52 6.70 5.09 -- 0.53 -- 0.89 2.72 4.55 -- 0.03 2.33 3.75 5.56 0.01 0.46 1.99b 0.00 0.35 0.45 0.06 0.16 1.23 0.76 0.07 0.46 a Poor et al., 2006. Estimated using CALPUFF deposition velocities but observed concentrations. Calculated as NO2-N. b CALPUFF-modeled dry and wet nitrogen deposition rates are much less than was estimated by Poor et al. (2006); however, Strayer et al. (2007) estimated that 25% or ~1 kg-N/ha/year of wet-deposited inorganic nitrogen to Tampa Bay was from sources near to Tampa Bay. 7. Summary of CALPUFF-Modeled Nitrogen Deposition Estimates In Table 5 are presented the estimates of direct and indirect wet and dry deposition to Tampa Bay. For an estimate of direct nitrogen deposition, annual average wet and dry deposition rates were calculated for receptors located over Tampa Bay, and these average rates were summed, units on these rates were converted from µg/m2/s to kgN/ha/year, and the resulting flux was multiplied by the 101,000-ha surface area of Tampa Bay. Likewise, for an estimate of indirect nitrogen deposition, annual average wet and dry deposition rates were calculated for receptors located over the Tampa Bay watershed, and these average rates were summed, units on these rates were converted from µg/m2/s to kg-N/ha/year, and the resulting flux was multiplied by the 570,000-ha surface area of the watershed and by a transfer coefficient of 18%, based on previous estimates by Pollman and Poor (2003). 11 Ammonium-N (NH4) deposition was computed by assuming 1.5 moles of NH4 for every mole of depositing SO4 (i.e., that SO4 is partially neutralized by NH4) plus 1.0 moles of NH4 for every mole of depositing NO3. Table 5. Summary of CALPUFF-Modeled Nitrogen Deposition Rates to Tampa Bay. Units are metric tons-N/year. Dry-Direct Dry-Indirect Wet-Direct Wet-Indirect Total NOx-N 112 209 0 0 321 HNO3-N 27 37 37 47 147 NO3-N 5 7 15 17 44 NH3-N NH4-N 84 129 58 80 352 6 7 43 49 105 Total N 234 390 153 192 969 From Table 5, direct nitrogen deposition is ~390 metric tons/year, or about 50% of the estimate by Poor et al. (2001), and indirect nitrogen deposition is ~580 metric tons/year, using the 2002 USEPA emissions inventory for central Florida. 8. Hillsborough County’s Contribution to Nitrogen Deposition to Tampa Bay CALPUFF modeling results indicate that, in 2002, sources within Hillsborough County contributed ~26% of the inorganic nitrogen deposited to Tampa Bay (Figure 4). Of this fraction, 52% was from area sources (on-road, off-road, and non-point), 41% came from two power plants, and 7% from point sources. 12 Figure 4. Contribution of Hillsborough County to total nitrogen deposition to Tampa Bay based on a 2002 emissions inventory. Units are metric tons-N/year. 7. Project Progress Report Estimates of air pollutant concentrations and deposition rates reported in this progress report are still preliminary, pending additional model testing and data checking. The project website (http://health.usf.edu/publichealth/eoh/calpuff.htm) was updated with the May 2008 midterm progress report and associated files. Likewise, following EPCHC receipt and review of this progress report, this report will be uploaded to the project website. References Calderón, S. M., Poor, N. D., Campbell, S. W., 2007. Estimation of the particle and gas scavenging contributions to wet deposition of organic nitrogen. Atmospheric Environment 41: 4281-4290. Calderón, S. M., Poor, N. D., Campbell, S. W., Tate, P., Hartsell, B. 2008. Rainfall scavenging coefficients for atmospheric nitric acid and nitrate in a subtropical coastal environment. Atmospheric Environment, doi: 10:1016/j.atmosenv.2008.05.040. 13 Dasgupta, P., Campbell, S., Al-Horr, R., Ullah, S., Li, J., Amalfitano, C., Poor, N., 2007. Conversion of sea salt aerosol to NaNO3, and the production of HCl: Analysis of temporal behavior of aerosol chloride/nitrate and gaseous HCl/HNO3 concentrations with AIM. Atmospheric Environment 41: 4242-4257. Durham, J. L., Stockburger, L., 1986. Nitric acid-air diffusion coefficient: experimental determination. Atmospheric Environment 20: 559-563. Kenty, K. L., Poor, N. D., Kronmiller, K. G., McClenny, W., King, C., Atkeson, T., Campbell, S. W., 2007. Application of CALINE4 to roadside NO/NO2 transformations. Atmospheric Environment 41: 4270-4280. Massman, W. J., 1998. A review of the molecular diffusivities of H2O, CO2, CH4, CO, O3, SO2, NH3, N2O, NO, and NO2 in air, O2, and N2 near STP. Atmospheric Environment 32: 1111-1127. NCDC, 2008. 2002 Local Climatological Data: Annual Summary with Comparative Data, Tampa, Florida (TPA), USA Department of Commerce ISSN 0198-1307, National Climatic Data Center, http://www.ncdc.noaa.gov/oa/climate/stationlocator.html, accessed May 30, 2008. Pollman, C., Poor, N. D., 2003. Export of Atmospherically Derived Nitrogen in the Tampa Bay Watershed. American Geophysical Union (AGU) Fall Meeting, San Francisco, CA, 8-12 December. Poor, N., Pollman, C., Tate, P., Begum, M., Evans, M., Campbell, S., 2006. Nature and magnitude of atmospheric fluxes of total inorganic nitrogen and other inorganic species to the Tampa Bay Watershed, FL, USA. Water, Air, and Soil Pollution 170: 267-283. Poor, N. D., Pribble, R., Greening, H., 2001. Direct wet and dry deposition of ammonia, nitric acid, ammonium and nitrate to the Tampa Bay Estuary, FL, USA. Atmospheric Environment 35: 3947-3955. Scire, J. S., Strimaitis, D. G., Yamartino, R., J., 2000. A User’s Guide for the CALPUFF Dispersion Model (Version 5). Earth Tech, Inc., Concord, MA. Seinfeld, J. H., Pandis, S. N., 1998. Atmospheric Chemistry and Physics: from Air Pollution to Climate Change. John Wiley & Sons, New York. 1326 pp. Strayer, H., Smith, R., Mizak, C., Poor, N., 2007. Influence of air mass origin on the wet deposition of nitrogen to Tampa Bay, Florida—an eight-year study. Atmospheric Environment 41: 4310-4322. Sutton, M. A., Burkhardt, J. K., Guerin, D., Nemitz, E., Fowler, D. 1998. Development of resistance models to describe measurements of bi-directional ammonia surfaceatmosphere exchange. Atmospheric Environment 32: 473-480. 14 Wesely, M. L., 1989. Parameterization of surface resistances to gaseous dry deposition in regional scale numerical models. Atmospheric Environment 23: 1293-1304. 15
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