A Method of Evaluating Atmospheric Models Using Tracer Measurements

Darko Koračin Desert Research Institute, Reno, Nevada

Search for other papers by Darko Koračin in
Current site
Google Scholar
PubMed
Close
,
James Frye Desert Research Institute, Reno, Nevada

Search for other papers by James Frye in
Current site
Google Scholar
PubMed
Close
, and
Vlad Isakov DynTel, Research Triangle Park, North Carolina

Search for other papers by Vlad Isakov in
Current site
Google Scholar
PubMed
Close
Restricted access

Abstract

The authors have developed a method that uses tracer measurements as the basis for comparing and evaluating wind fields. An important advantage of the method is that the wind fields are evaluated from the tracer measurements without introducing dispersion calculations. The method can be applied to wind fields predicted by different atmospheric models or to wind fields obtained from interpolation and extrapolation of measured data. The method uses a cost function to quantify the success of wind fields in representing tracer transport. A cost function, “tracer potential,” is defined to account for the magnitude of the tracer concentration at the tracer receptors and the separation between each segment of a trajectory representing wind field transport and each of the tracer receptors. The tracer potential resembles a general expression for a physical potential because the success of a wind field trajectory is directly proportional to the magnitude of the tracer concentration and inversely proportional to its distance from this concentration. A reference tracer potential is required to evaluate the relative success of the wind fields and is defined by the initial location of any trajectory at the source. Then the method is used to calculate continuously the tracer potential along each trajectory as determined by the wind fields in time and space. Increased potential relative to the reference potential along the trajectory indicates good performance of the wind fields and vice versa. If there is sufficient spatial coverage of near and far receptors around the source, then the net tracer potential area can be used to infer the overall success of the wind fields. If there are mainly near-source receptors, then the positive tracer potential area should be used. If the vertical velocity of the wind fields is not available, then the success of the wind fields can be estimated from the vertically integrated area under the tracer potential curve. A trajectory with a maximum tracer potential is constructed for each daily tracer measurement, and this tracer potential is used to normalize the relative success of the wind fields in reproducing the transport of tracers. The method is not sensitive to the exact form of the cost function because a test with an inverse square root dependence in the cost function rather than an inverse linear distance dependence ranked the wind fields in the same order. The method requires sufficient spatial coverage of tracer receptors in the vicinity of a source and primarily gives credit to the wind fields that are able to approach areas with high tracer concentrations. The method can quantitatively determine which wind fields are best able to reproduce the main transport of tracers and can be used to determine the most successful wind fields to serve as a solid base for necessary improvement of dispersion models. It can also be used as a screening method prior to using dispersion models. Since the measured tracer concentrations are affected by both transport and dispersion, however, the method does not evaluate the capabilities of successful wind fields, as input to dispersion algorithms, to create tracer concentrations at receptors that are similar to measured ones. The tracer potential method has been applied to data from a comprehensive field program that included tracer measurements and was conducted in the Colorado River Valley area in the southwestern United States in 1992. Wind fields obtained from four atmospheric models as well as those derived from the wind profiler measurements were tested, and the results of their comparison are presented. Since data from the tracer experiment are publicly available, this developed method can be used to test other atmospheric models.

Corresponding author address: Dr. Darko Koračin, Desert Research Institute, 2215 Raggio Parkway, Reno, NV 89512.

Abstract

The authors have developed a method that uses tracer measurements as the basis for comparing and evaluating wind fields. An important advantage of the method is that the wind fields are evaluated from the tracer measurements without introducing dispersion calculations. The method can be applied to wind fields predicted by different atmospheric models or to wind fields obtained from interpolation and extrapolation of measured data. The method uses a cost function to quantify the success of wind fields in representing tracer transport. A cost function, “tracer potential,” is defined to account for the magnitude of the tracer concentration at the tracer receptors and the separation between each segment of a trajectory representing wind field transport and each of the tracer receptors. The tracer potential resembles a general expression for a physical potential because the success of a wind field trajectory is directly proportional to the magnitude of the tracer concentration and inversely proportional to its distance from this concentration. A reference tracer potential is required to evaluate the relative success of the wind fields and is defined by the initial location of any trajectory at the source. Then the method is used to calculate continuously the tracer potential along each trajectory as determined by the wind fields in time and space. Increased potential relative to the reference potential along the trajectory indicates good performance of the wind fields and vice versa. If there is sufficient spatial coverage of near and far receptors around the source, then the net tracer potential area can be used to infer the overall success of the wind fields. If there are mainly near-source receptors, then the positive tracer potential area should be used. If the vertical velocity of the wind fields is not available, then the success of the wind fields can be estimated from the vertically integrated area under the tracer potential curve. A trajectory with a maximum tracer potential is constructed for each daily tracer measurement, and this tracer potential is used to normalize the relative success of the wind fields in reproducing the transport of tracers. The method is not sensitive to the exact form of the cost function because a test with an inverse square root dependence in the cost function rather than an inverse linear distance dependence ranked the wind fields in the same order. The method requires sufficient spatial coverage of tracer receptors in the vicinity of a source and primarily gives credit to the wind fields that are able to approach areas with high tracer concentrations. The method can quantitatively determine which wind fields are best able to reproduce the main transport of tracers and can be used to determine the most successful wind fields to serve as a solid base for necessary improvement of dispersion models. It can also be used as a screening method prior to using dispersion models. Since the measured tracer concentrations are affected by both transport and dispersion, however, the method does not evaluate the capabilities of successful wind fields, as input to dispersion algorithms, to create tracer concentrations at receptors that are similar to measured ones. The tracer potential method has been applied to data from a comprehensive field program that included tracer measurements and was conducted in the Colorado River Valley area in the southwestern United States in 1992. Wind fields obtained from four atmospheric models as well as those derived from the wind profiler measurements were tested, and the results of their comparison are presented. Since data from the tracer experiment are publicly available, this developed method can be used to test other atmospheric models.

Corresponding author address: Dr. Darko Koračin, Desert Research Institute, 2215 Raggio Parkway, Reno, NV 89512.

Save
  • Blumen, W., Ed., 1990: Atmospheric Processes over Complex Terrain, Meteor. Monogr., No. 45, Amer. Meteor. Soc., 323 pp.

  • Brier, G. W., 1990: A historical and personal perspective of model evaluation in meteorology. Bull. Amer. Meteor. Soc.,71, 349–351.

  • Briggs, G., 1975: Plume rise predictions. NOAA-ERL ATDL 75/15, 53 pp. [Available from NOAA Environmental Research Laboratory, Oak Ridge, TN 37831.].

  • Clements, W. E., and D. E. Hoard, 1989: Mean structure of the nocturnal drainage flow in a deep valley. J. Appl. Meteor.,28, 457–462.

  • Doran, J. C., and T. W. Horst, 1983: Observations and models of simple nocturnal slope flows. J. Atmos. Sci.,40, 708–717.

  • Enger, L., and D. Koračin, 1995: Simulations of dispersion in complex terrain using a higher-order closure model. Atmos. Environ.,29, 2449–2466.

  • Enger, L., D. Koračin, and X. Yang, 1993: A numerical study of boundary layer dynamics in a mountain valley. Part 1. Model validation and sensitivity experiments. Bound.-Layer Meteor.,66, 357–394.

  • Fast, J. D., and C. M. Berkowitz, 1997: Evaluation of back trajectories associated with ozone transport during the 1993 North Atlantic Regional Experiment. Atmos. Environ.,31, 825–837.

  • Green, M. C., 1999: The Project MOHAVE tracer study: Study design, data quality, and overview of results. Atmos. Environ.,33, 1955–1968.

  • Grell, G. A., J. Dudhia, and D. R. Stauffer, 1995: A description of the Fifth-Generation Penn State/NCAR Mesoscale Model (MM5). NCAR Tech. Note TN-398, 122 pp. [Available from NCAR, P. O. Box 3000, Boulder, CO 80307.].

  • Haagenson, P. L., Y.-H. Kuo, M. Skumanich, and N. L. Seaman, 1987: Tracer verification of trajectory models. J. Climate Appl. Meteor.,26, 410–426.

  • Haagenson, P. L., K. Gao, and Y.-H. Kuo, 1990: Evaluation of meteorological analyses, simulations, and long-range transport calculations using ANATEX surface tracer data. J. Appl. Meteor.,29, 1268–1283.

  • Hanna, S. R., 1988: Air quality model evaluation and uncertainty. J. Air Pollut. Control Assoc.,38, 406–412.

  • Hanna, S. R., 1994: Mesoscale meteorological model evaluation techniques with emphasis on needs of air quality models. Mesoscale Modeling of the Atmosphere, Meteor. Monogr., No. 47, Amer. Meteor. Soc., 47–58.

  • Hoecker, W. H., 1977: Accuracy of various techniques for estimating boundary layer trajectories. J. Appl. Meteor.,16, 374–383.

  • Kao, C. Y. J., and T. Yamada, 1988: Use of the CAPTEX data for evaluations of a long-range transport numerical technique. Mon. Wea. Rev.,116, 293–306.

  • Klug, W., G. Graziani, G. Grippa, D. Pierce, and C. Tassone, 1992:Evaluation of long term atmospheric transport models using environmental radioactivity data from Chernobyl accident. The ATMES Report, Elsevier, 366 pp.

  • Koračin, D., and L. Enger, 1994: A numerical study of boundary layer dynamics in a mountain valley. Part 2. Observed and simulated characteristics of atmospheric stability and local flows. Bound.-Layer Meteor.,69, 249–283.

  • Koračin, D., V. Isakov, and J. Frye, 1998a: A method of evaluation of atmospheric and dispersion models by using tracer measurements. Proc. 10th Joint Conf. on the Applications of Air Pollution Meteorology with the AWMA, Phoenix, AZ, Amer. Meteor. Soc., 11–16.

  • Koračin, D., V. Isakov, and J. Frye, 1998b: A method of evaluating atmospheric models by using tracer measurements. Proc. Fifth Int. Conf. on Harmonisation within Atmospheric Dispersion Modeling for Regulatory Purposes, Rhodes, Greece, 79–86.

  • ——, ——, and ——, 1998c: A Lagrangian particle dispersion model (LAP) applied to transport and dispersion of chemical tracers in complex terrain. Proc. 10th Joint Conf. on the Applications of Air Pollution Meteorology with the AWMA, Phoenix, AZ, Amer. Meteor. Soc., 227–230.

  • Kuhns, H., M. Green, M. Pitchford, L. Vasconcelos, W. White, and V. Mirabella, 1999: Attribution of particulate sulfur in the Grand Canyon to specific point sources using tracer-aerosol gradient interpretive technique (TAGIT). J. Air Waste Manag. Assoc.,49, 906–915.

  • Lu, X., and T. Yamada, 1998: Numerical simulation of airflows and tracer transport in an arid western mountain area. Proc. 10th Joint Conference on the Applications of Air Pollution Meteorology with the AWMA, Phoenix, AZ, Amer. Meteor. Soc., 364–368.

  • Pielke, R. A., 1984: Mesoscale Meteorological Modeling. Academic Press, 612 pp.

  • Pitchford, M., M. C. Green, and R. J. Farber, 1997: Characterization of regional transport and dispersion using Project MOHAVE tracer data. Proc. Visual Air Quality Conf., Bartlett, NH, 181–200.

  • Scire, J. S., E. M. Insley, R. J. Yamartino, and M. E. Fernau, 1995:User’s guide for the CALMET Meteorological Model. USDA Forest Service Tech. Rep. 1406-01, 302 pp. [Available from Earth Tech, Inc., 196 Baker Ave., Concord, MA 01742.].

  • Stocker, R. A., R. A. Pielke, A. J. Verdon, and J. T. Snow, 1990: Characteristics of plume releases as depicted by balloon launchings and model simulations. J. Appl. Meteor.,29, 53–62.

  • Uliasz, M., 1993: The atmospheric mesoscale dispersion modeling system. J. Appl. Meteor.,32, 139–149.

  • Venkatram, A., 1988: Model evaluation. Lectures on Air Pollution Modeling, A. C. Venkatram and J. C. Wyngaard, Amer. Meteor. Soc., 308–321.

  • Vimont, J., 1997: Evaluation of the CALMET/CALPUFF modeling system using Project MOHAVE tracer and implications for sulfate contributions. Proc. Visual Air Quality Conf., Bartlett, NH, 436–446.

  • Whiteman, C. D., 1982: Breakup of temperature inversions in deep mountain valleys. Part I: Observations. J. Appl. Meteor.,21, 270–289.

  • Whiteman, C. D.,, 1989: Morning transition tracer experiments in a deep narrow valley. J. Appl. Meteor.,28, 620–635.

  • Yamada, T., 1992: A numerical simulation of airflows and SO2 concentration distributions in an arid southwestern valley. Atmos. Environ.,26, 1771–1781.

  • Yamada, T., and S. Bunker, 1988: Development of a nested grid, second-moment turbulence closure model and application to the 1982 ASCOT Brush Creek data simulation. J. Appl. Meteor.,27, 562–578.

  • Yamada, T., and S. Bunker, 1989: A numerical model study of nocturnal drainage flows with strong wind and temperature gradients. J. Appl. Meteor.,28, 545–554.

  • Yamada, T., and T. Henmi, 1994: HOTMAC: Model performance evaluation by using project WIND Phase I and II Data. Mesoscale Modeling of the Atmosphere, Meteor. Monogr., No. 47, Amer. Meteor. Soc., 123–135.

  • Yamada, T., S. Bunker, and S. Moss, 1992: Numerical simulation of atmospheric transport and diffusion over coastal complex terrain. J. Appl. Meteor.,31, 565–578.

All Time Past Year Past 30 Days
Abstract Views 0 0 0
Full Text Views 241 51 8
PDF Downloads 85 36 4