NOAA ESRL Physical Sciences Division  

PROGRAMS

Contacts
R.J. Alvarez II
R.M. Banta
C.J. Senff

UV DIAL

Findings

References

1995 Southern Oxidants Study

"Photochemical oxidants are a class of highly reactive chemicals produced in the earth's atmosphere. In the stratosphere, O3 [Ozone], the most abundant of the photochemical oxidants, protects human, plant, and animal life from the harmful effects of ultraviolet light from the sun. In the lower atmosphere, paradoxically, O3 and other photochemical oxidants can have adverse effects on plants, animals, and human health. [. . .] Even though these chemical compounds are normally present only in very low concentrations, their health, economic, and ecological impact can be substantial." -The State of the Southern Oxidants Study (SOS)

The Southern Oxidants Study (SOS) is a strategic alliance of research scientists, engineers, and air quality managers from universities, federal and state governments, industry, and public interest groups formed in 1989 to address the unresolved technical and scientific issues surrounding ozone pollution and ozone pollution management.

The ETL Lidar Division contributed to this alliance during the 1995 Nashville Study through precision measurement and mapping of ozone over the study area with the airborne differential-absorbption lidar (DIAL).

Findings

Urban Stagnation Study

Conditions that lead to the highest hourly photochemical ozone (O3) concentrations for a season in an urban area are light-wind conditions, in which pollutants accumulate near the source region. The very highest concentrations are expected during the lightest winds, i.e., during stagnation conditions. During the 1995 S.O.S. Nashville campaign, a 3-day stagnation episode occurred during mid July. Scientists obtained a rich dataset, including several very revealing flights from the ETL airborne O3 differential-absorption lidar (DIAL).

Key scientific questions included:

  • How high in the atmosphere does the pollution reach during the day?
  • Does pollution remain over the urban source region at night and thus accumulate over the several days of an episode, or does the pollution get blown away from the urban center?
  • If the pollution does not remain over the urban area at night, what is its fate? does it become part of the rural background?

Data from the airborne O3 DIAL system allow us to address these issues. The data provide vertical cross sections of O3 concentration along the flight path of the aircraft. Intercomparison flights have shown that the O3 concentrations measured by the lidar agree with in situ aircraft measurements by 4 ppbv near the airplane and ~10 ppbv near the earth's surface (i.e., farther from the airplane).

Results:

  1. Daytime accumulation: Cross sections over the city on 12 July, the middle day of the 3-day episode [Figure A], showed that the urban pollutants formed a dome over the urban area. Significant O3 reached ~1.9 km above mean sea level (MSL; a mean elevation for the Nashville environs is ~200 m MSL), and O3 concentrations exceeding 120 ppb extended to >1.5 km MSL. A horizontal plot of O3 along the flight track [Figure B] shows that the pollution remained very close to Nashville.
  2. Nighttime wind behavior: winds near the surface remained light and variable at night, suggesting that the pollutant dome might stay put. Radar wind profiler data, however, show that the winds above ~100 m above ground level (AGL) accelerate at night. Because considerable pollution exists at these levels, this flow should transport the O3 away from the urban area at these heights. Overnight trajectories from the profiler data for the night between the first and second days of the episode [Figure C] show the expected effects of this transport. At lower levels between 250 and 500 m AGL pollution should be transported ~80 km to the west of the location of the pollution cloud at sunset.
  3. Early morning flights to the southwest of Nashville verified the presence of high O3 concentrations at lower levels. Figure D shows high O3 in the layer between 400 and 800 m MSL and superimposed trajectories. The trajectories are based on horizontally interpolated profiler winds averaged over the 400- to 800-m layer. At higher levels from 800 to 2000 m MSL, O3 concentrations were low.
  4. Vertical profiles of O3 from four successive identical flight legs over this region show the O3 mixing out in the vertical as the daytime mixed layer grows. [Figure E]

    Other interesting results:

    1. Differences in mixing layer height h between the area northwest of Nashville and the other quadrants around Nashville: differences of ~500 m in h could be seen over a few 10's of km [see aerosol cross sections in Figure A (ii); regions of high aerosol represent the mixed layer].
    2. Urban-rural differences in O3 concentration were highest on the lightest-wind day.
    3. The stagnation episode consisted of 3 days when the radar wind profilers showed light and variable winds throughout the depth of the daytime convective boundary layer. Even though the winds were light, the pollution cloud was observed to drift to varying degrees on the 3 days. This affected ground-level concentrations: the day with the least drift (12 July) had the highest O3 concentrations.

    Conclusions:

    O3 cross sections from airborne DIAL system have allowed us to address the questions above:

    1. During daytime the processes are relatively straightforward to interpret. Photochemical pollutants accumulate over or near the urban area and mix vertically to the top of the urban mixed layer, which may reach 2 km ASL.
    2. At night processes are more complex. Inertial accelerations of the winds in the layer that had been the previous day's mixed layer distribute pollutants from the urban pollution dome over the nearby countryside. Pollutants appear as patches or layers at different levels in the vertical for different directions of transport from the source.
    3. The layers or patches of urban pollution are mixed in the vertical the next day, as surface heating drives the growth of the daytime mixed layer.

    These measurements have allowed us to characterize the fate of photochemical pollutants during a stagnation episode. As pollutants from the previous days' dome are mixing into today's rural background, a new pollutant dome is forming over the urban area.

    Another important result of the light horizontal winds during stagnation is that local differences in land use can express themselves as local differences in mixing height h. On the middle day of the episode a difference of ~500 m in h was noted over a horizontal distance of a few 10's of km between the forested land to the west through northwest of Nashville and the farming and pasture land in the other directions around the city.

    More details on all these issues can be found in the article by Banta et al. (1998)

(i) 

(ii) 

(iii) 

Figure A. Vertical cross sections of O3 concentration and aerosol backscatter for the NW-SE flight legs passing over Nashville for the afternoon flights on 12 July. (i) O3 concentrations (ppbV) for the first pass (1220-1248 CDT, (ii) aerosol backscatter (10-5 m-1 sr-1) for the first pass, and (iii) O3 concentration for the second pass (1405-1433 CDT).

Figure B. Horizontal maps of the ozone distribution from the ozone lidar reveal the distinct increase in ozone concentrations (yellow, orange, red and black) over urban Nashville against the lower (blue and green) levels of the surrounding suburban and rural areas.

Figure C. Overnight forward trajectories calculated from the hourly horizontally interpolated winds, averaged over 400-m vertical intervals. Symbols indicate hourly positions beginning at 2000 CDT on July 11 and ending at 0800 CDT on July 12. Trajectory was calculated from an origin ~20 km southwest of Nashville at 36.0 N, 86.9 W.

Figure D. Flight-track O3 data averaged over 800-m vertical intervals for the first flight track (0708-0805 CDT) on July 12: (a) lower level from 400 to 1200 m asl, and (b) upper level from 1200 to 2000 asl. Trajectory in Figure D was calculated from mean winds in the 800 m layer from 400 to 1200 m asl.

Figure E. Profiles of O3 averaged horizontally over the region of high O3 in the western part of the flight track shown in Figure D, for each of the four repetitions of the track during the morning flight on July 12.


Power Plant Plume Study

Figure 1 Figure 2
Fig.1:  Time-height cross sections of lidar ozone concentrations showing multiple crossings of the Cumberland power plant plume at different distances downwind of the plant. Data were taken on July 7, 1995. The boundary layer height was estimated from the lidar data and is overplotted as a black line. Fig.2:  Same as Fig. 1 except data were taken on July 19, 1995.

The role of airborne lidar in power plant plume studies
To investigate chemical processes in power plant plumes, airborne in situ sensors are typically the instruments of choice because of their ability to detect a multitude of chemical species with high accuracy. However, coverage of the plume area is limited, since the plume is usually only transected at a single height. This means that often assumptions must be made about plume properties when the in situ data are interpreted. An airborne lidar, on the other hand, can map out the cross section of the plume during a single overpass yielding information on plume size, shape, and the vertical distribution of certain pollutants in the plume. Thus, an airborne lidar can provide crucial information on power plant plumes properties which, in concert with in situ measurements, can help further our understanding of power plant plume chemistry and its impact on air quality.

Measurement capabilities
We used NOAA/ETL's airborne ozone and aerosol lidar to investigate power plant plumes in the Nashville area during the 1995 SOS campaign. The downward-looking lidar was typically flown at an altitude of around 3000 m above sea level crossing the power plant plume at multiple distances downwind of the plant. The aerosol backscatter and ozone data gathered while flying across the plume give a detailed picture of the vertical and lateral extent of the plume. Also, the plume location with respect to the top of the boundary layer can be determined because the lidar aerosol returns provide information on the boundary layer height. In addition, we used the lidar ozone data to calculate ozone production rates in the plume as a function of distance downwind.

Key findings

  • The evolution of a power plant plume depends strongly on the local meteorological conditions. In one case study, the plume was spread quickly across the entire depth of the boundary layer due to strong vertical mixing but did not reach into the overlying free troposphere. The plume was shaped symmetrically and had a clearly defined, single core (Fig. 1). In another case, part of the power plant plume had penetrated the inversion capping the boundary layer shortly after release from the stack. Subject to different meteorological conditions the two portions of the plume above and below the boundary layer top evolved differently as they advected downwind resulting in a very irregular shape and a near breakup of the plume (Fig. 2).

  • We found that close to the power plant ozone was destroyed creating an ozone deficit by which the plume can be readily identified. This is a well known effect caused by titration of ozone in the presence of elevated NO levels. Farther downwind, where ozone is formed in the plume due to reaction of NOx with ozone precursor gases, we observed ozone production rates of up to 4 ppbV/h. The latter confirms that NOx-rich power plant plumes have the potential of raising local ozone levels significantly over the course of a day.

References:

SOS Homepage
Questions and Answers about Ozone Pollution (PDF)
1995 Nashville/Middle Tennessee Ozone Study (PDF)

AlvarezII, R.J., C.J. Senff, R.M. Hardesty, D.D. Parrish, W.T. Luke, T.B. Watson, P.H. Daum, and N. Gillani, 1998: Comparisons of airborne lidar measurements of ozone with airborne in situ measurements during the 1995 Southern Oxidants Study, J. Geophys. Res., 103, 31,155 - 31,171.

Banta, R.M., C.J. Senff, A.B. White, M. Trainer, R.T. McNider, R.J. Valente, S.D. Mayor, R.J. Alvarez, R.M. Hardesty, D. Parrish, and F.C. Fehsenfeld, 1998: Daytime buildup and nighttime transport of urban ozone in the boundary layer during a stagnation episode, J. Geophys. Res., 103, 22,519 - 22,544.

Senff, C.J., R.M. Hardesty, R.J. AlvarezII, and S.D. Mayor, 1998: Airborne lidar characterization of power plant plumes during the 1995 Southern Oxidants Study, J. Geophys. Res., 103, 31,173 - 31,189.

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