Conditions of the Simulations
Background Information
Journal papers describing the 10 July 1996 storm are as follows:
Dye, J. E., B. A. Ridley, K. Baumann, W. C. Skamarock, M. C. Barth, M.
Venticinque, E. Defer, P. Blanchet, C. Thery, P. Laroche, G. Hubler, D.
D. Parrish, T. Ryerson, M. Trainer, G. Frost, J. S. Holloway, F. C.
Fehsenfeld, A. Tuck, T. Matejka, D. Bartels, S. A. Rutledge, T.
Lang, J. Stith, R. Zerr, 2000: An Overview of the STERAO--Deep
Convection Experiment with Results for the 10 July Storm, J. Geophys. Res., 105, 10,023-10,045. (PDF)
Skamarock, W. C., J. Powers, M. C. Barth, J. E. Dye, T. Matejka, D.
Bartels, K. Baumann, J. Stith, D. D. Parrish, and G. Hubler, 2000:
Numerical simulations of the 10 July STERAO/Deep Convection Experiment
Convective System: Kinematics and transport, J. Geophys. Res., 105, 19,973--19,990. (PDF)
Barth, M. C., A. L. Stuart, and W. C. Skamarock, 2001: Numerical
simulations of the July 10 Stratospheric-Tropospheric Experiment:
Radiation, Aerosols and Ozone/Deep Convection storm:
Redistribution of soluble tracers, J.
Geophys. Res., 106,
12,381-12,400. (PDF)
Skamarock, W. C., J. E. Dye, E. Defer, M. C. Barth, J. L. Stith, B. A.
Ridley, and K. Baumann, 2003: Observational- and Modeling-Based
budget of lightning-produced NOx in a continental thunderstorm, J. Geophys. Res., 108(D10), 4305,
doi10.1029/2002JD002163. (PDF)
Dye et al. (2000) describe the observed storm.
Skamarock et al. (2000) describe simulations of tracer transport.
The simulation discussed in this paper will be repeated for the
intercomparison case. The observed CO and O3
concentrations shown
in this paper will be used to evaluate the participating models.
Skamarock et al. (2003) describe an analysis of lightning-produced
NOx. The analyzed CO, O3, and NOx fluxes (analyzed
from the
measurements) will be used to evaluate the participating models.
Barth et al. (2001) describe transport of soluble tracers.
Please simulate the following tracers:
CO, O3, NO, NO2 (or NOx), and tracer-NOx.
tracer-NOx is NOx which is only transported in the simulation.
Other species may also be simulated, if so desired.
Optional tracers to simulate:
HNO3,
H2O2, and CH2O to examine the fate of
soluble tracers.
These can be simulated either with or without chemistry. Because
measurements of these 3 species were not made in the anvil of the storm
nor in the precipitation, comparisons of these model results will be
done only among models. A link to the initial
concentrations of these species is provided below.
The following initial conditions are taken from Skamarock et al. (2000,
2003). The altitudes provided are values above ground level and
match the model levels presented in Skamarock et al. (2000). If
you need initial conditions at other altitudes, simply perform a linear
interpolation.
Meteorological Initial Conditions:
Sounding data is contained in a Html
version,
or ASCII
version table.
To initiate convection, place 3 positively buoyant thermals
aligned NW to SE and spaced approximately 20 km apart, following these
equations.
θ' = 0.5 Δθ (cos(πr) +
1)
for r < 1
r is the distance from (xr, yr, zr)
where xr = yr = 10 km and zr = 1.5
km. Δθ = 3
K
The surface pressure is 860 mb. Storm speed is us =
1.5 m/s, vs = -5.5 m/s .
Chemistry Initial Conditions:
Vertical profiles are contained in a Html
version or ASCII
version table.
Ice Nuclei (IN) initial concentration: 0.1 cm-3.
Condensation Nuclei (CN) concentrations are provided in the following
table. These values are from the WP3D NOAA aircraft.
Altitudes are given in km, mean sea level. The surface is 1.5 km,
m.s.l.. The data are average CN values out-of-cloud for the
specific altitude ± 0.5 km.
z
(km, m.s.l.)
|
CN
(cm-3)
|
1.5
|
6609
|
2.7
|
4388
|
4.0
|
410
|
5.0
|
195
|
6.0
|
108
|
6.5
|
128
|
Above 6.5 km, m.s.l. set CN concentrations to 128 cm-3.
Those who simulate aerosols have assumed a log-normal distribution
(Dmean = 50-100 nm, std dev = 2.0 in boundary layer; Dmean = 10-30 nm,
std dev = 1.5-1.7 above boundary layer) composed of ammonium
bisulfate. There are no measurements to confirm these
assumptions, but they are quite reasonable for the location.
You are strongly encourage to predict CO, O3 and NOx mixing
ratios. In addition, the soluble species H2O2,
CH2O and HNO3 can be predicted to examine both
transport and scavenging.
Output:
Simulate storm and tracers for about 3 hours. The results from
the model simulations will be compared to observations
measured in the anvil of the storm. Please provide the following
results:
1. Peak updraft velocities as a function of time and
location. Email an ASCII file with this data and I will plot it
alongside results from other participants.
2. Radar reflectivity (dBZ) cross sections that can be compared
to Figures 6 and 7 in Skamarock et al. (2000).
A. x-y cross section (W-E, N-S) at
a) z = 4.5 km m.s.l. (3 km above ground
level) at
1) t = 2312 UTC
(approximately 1 hour after start of simulation)
2) t = 0128 UTC
(approximately 9000 s after start of simulation)
b) z = 10.5 km m.s.l. (9 km above
ground level) at
1) t = 2312 UTC (approximately 1
hour after start of simulation)
2) t = 0128 UTC
(approximately 9000 s after start of simulation)
B. xy-z cross section (NW-SE,
top-bottom) at
a) t = 2312 UTC (approximately 1 hour
after start of simulation)
b) t = 0128 UTC (approximately 9000 s after
start of simulation)
This cross section is along the line of cells. In Skamarock et
al. (2000) the cross section was placed at a 130 deg angle from north
(-40 degrees from east) -- note that the 9000 s simulation
cross-section is at a 115 degree angle from north. Choose the
angle that best fits your simulation.
Code
to calculate radar reflectivity using bulk-water microphysics
Fortran
code to interpolate model results to a cross section
Email output files of values so that I can plot the results
consistently with other participants. Be sure to provide a height
and
horizontal coordinate (either in email or in the attached file).
Be
sure to explain the format of your output file.
3. Volume mixing ratios (ppbv) across the anvil for CO, O3,
and
NOx :
- During the multicellular stage of the storm (~1
hour into the simulation) at approximately 10 km downwind of the
southeasternmost cell (with a SW-NE orientation)
- Approximately 1/2 hour later at ~50 km downwind
of the southeasternmost cell (with a N-S orientation)
These observations are shown in Dye et al. (2000) Figure 9 and
Skamarock et al. (2000) Figure 11.
Email an ASCII file with these results and I will plot it alongside
results from other participants.
4. Vertical cross section of particle concentration (per liter),
CO (ppbv), O3 (ppbv), NO (pptv), and NOx (pptv) at approximately
6000 s and 50-60 km downwind of convective core. See Figure 1 of
Skamarock et al. (2003) for location of observed analysis plane.
The analyzed measurements are shown in Figure 4 of Skamarock et al.
(2003). If your model does not predict particle concentration,
use one of the following methods for determining the particle
concentration:
If the water reservoir is assumed to have the same size particles, then
N = q/M
where q = mixing ratio (kg/kg) of water reservoir and M = mass of
particle = ρparticle * π/6 * (Dparticle)3
If the water reservoir has an assumed size distribution, then
N = ∫ (N(D) dD
Email output files of values so that I can plot the results
consistently with other participants. Be sure to provide a height
and
horizontal coordinate (either in email or in the attached file).
Be
sure to explain the format of your output file.
5. Fluxes of air mass (kg/s/m2), CO (moles/s/m2)
and
NOx
(moles/s/m2) integrated over the anvil through the analysis
plane (see
#3) divided by the cross-sectional area of the anvil. Provide
instantaneous and cumulative flux densities at 10 minute intervals
between 1 hour and 2 hours
of the integration. The analyzed observations of flux densities
are given in Table 1 of
Skamarock et al. (2003).
How to do the flux calculation: 3
slides explaining geometry and flux calculation
Email these results in an ASCII file.
Output for Soluble Species:
1. Volume mixing ratios (ppbv) across the anvil for HNO3,
H2O2 and CH2O :
- During the multicellular stage of the storm (~1
hour into the simulation) at approximately 10 km downwind of the
southeasternmost cell (with a SW-NE orientation)
- Approximately 1/2 hour later at ~50 km downwind
of the southeasternmost cell (with a N-S orientation)
Email an ASCII file with these results and I will plot it alongside
results from other participants.
2. Vertical cross section of HNO3 (ppbv), H2O2
(ppbv), and CH2O (ppbv) at approximately
6000 s and 50-60 km downwind of convective core. See Figure 1 of
Skamarock et al. (2003) for location of observed analysis plane.
Email output files of values so that I can plot the results
consistently with other participants. Be sure to provide a height
and horizontal coordinate (either in email or in the attached
file). Be sure to explain the format of your output file.
3. Fluxes of HNO3,
H2O2 and CH2O ((moles/s/m2)
integrated over the anvil through the analysis
plane (see above) divided by the cross-sectional area of the
anvil. Provide
instantaneous and cumulative flux densities at 10 minute intervals
between 1 hour and 2 hours
of the integration. If needed, see flux calculation slides
(link in #5 above).
Email these results in an ASCII file.
Send email to barthm@ucar.edu.
Last updated: February 18, 2005