4.2. Model Studies of Subsonic Aircraft
In this section, we discuss the results of global 3-D CTMs used to assess
the effects of subsonic aircraft on atmospheric concentrations of O3,
NOx, and OH. The models differ in their formulations
of vertical and horizontal resolution, transport, boundary conditions, and chemistry.
Therefore, a wide range of results is to be expected. A short presentation of
models and assumptions follows.
4.2.1. Models Used in Subsonic Aircraft Assessment
Table 4-1 lists the six CTMs used and the names
of the associated investigators.1 Readers are referred to a Technical Report
on Subsonic Aircraft Effects, which is presently available over the Internet
for additional details.
4.2.1.1. Off-Line vs. On-Line Models
All of the models in Table 4-1, except the ECHAm3/CHEM
model, are off-line models; that is, they are driven using meteorological fields
derived either from GCMs or from analysis of observations. The temporal resolution
of the various meteorological fields used to drive the models ranges from 40
minutes to a day. One exception is the IMAGES/ BISA model, which uses monthly-average
meteorological fields and includes a parameterization to account for shorter-term
variability in transport. In all of the off-line models, 1 year of wind fields
is recycled in multiyear simulations to get the steady-state atmosphere. On-line
calculations provide the potential capability of examining chemistry-climate
interactions when model-calculated fields are used in radiation calculations.
In ECHAm3/CHEM, the evolution of chemical fields is calculated on-line in a
GCM, but the calculated chemical fields do not feed back into the dynamic calculations
in this application. The model, therefore, operates in a similar way to the
off-line models.
4.2.1.2. Model Resolution
Typically, these models have horizontal resolutions of 3-6°, with the exception
of the UiO model, which has a horizontal resolution of 8°x10°. In the vertical
dimension, the IMAGES/ BISA model has 25 levels; the Tm3/KNMI and ECHAm3/ CHEM
models have 19 levels; and the HARVARD, UKMO, and UiO models have nine levels.
Four of the models (ECHAm3/CHEM, HARVARD, Tm3/KNMI, UiO) have a top layer located
at 10 mb; the IMAGES/BISA and UKMO models have top layers located at 50 mb and
100 mb, respectively. Because vertical model levels are defined on sigma coordinates
and not on pressure coordinates, the number of model levels between fixed pressure
surfaces can vary in time. Between the surface and 850 mb, the HARVARD, UiO,
and UKMO models have about two vertical levels; the ECHAm3/CHEM and Tm3/KNMI
models have about five vertical levels, and the IMAGES/BISA model has eight
vertical levels. In the UT/LS region between 100 and 300 mb, the HARVARD model
has one vertical level, the UKMO model has about two levels, and the other four
models have about four vertical levels.
4.2.1.3. Coupling to the Stratosphere
With the exception of the ECHAm3/CHEM model, the models have little or no representation
of explicit stratospheric chemistry. Instead, either the cross-tropopause fluxes
of O3 and NOy are specified or the mixing ratios
of these species are specified in the LS based on observations. In the Tm3/KNMI,
UiO, and IMAGES/BISA models, however, the upper boundaries are higher in an
attempt to minimize their influence on regions of maximum perturbations by aircraft.
It should be noted that this condition may not be satisfied for the IMAGES/BISA
model because the model top is at 50 mb.
4.2.1.4. Tropospheric NOx
Sources
All of the models include anthropogenic and biogenic tropospheric NOx
sources. For present-day conditions, the magnitudes of surface NOx
sources in the various models are ~21 Tg nitrogen (N) yr-1 from surface-based
fossil-fuel combustion, 5-12 Tg N yr-1 from biomass burning, and 4-6 Tg N yr-1
from soils. The present-day magnitude of the lightning source is 5 Tg N yr-1
in the IMAGES/BISA, Tm3/KNMI, UKMO, and UiO models; 4 Tg N yr-1 in the ECHAm3/CHEM
model (increased to 5 Tg N yr-1 in the 2015 and 2050 simulations); and 3 Tg
N yr-1 in the HARVARD model. It should be noted, however, that the simulated
impact of lightning on NOy species in the troposphere can differ from model
to model even if the magnitude of the lightning source of NOx
is the same, as a result of differences in factors such as duration and intensity
of convective events, land/ocean differences in convection, height of NOx
emissions, and so forth. Sensitivity tests were run to evaluate the effect of
this lightning assumption on calculated aircraft perturbation.
4.2.1.5. Tropospheric Chemistry
Most of the models include a comprehensive description of the CH4-CO-NOx-HOx-O3
chemical system. With the exception of ECHAm3/CHEM and Tm3/KNMI, the models
include representations of NMHC chemistry. However, the details of NMHC chemistry
differ significantly from model to model. The ECHAm3/CHEM model includes a stratosphere
with a chemistry scheme more suited to the stratosphere, however, it does not
include some of the species that are important for tropospheric chemistry.
Table 4-2: Increase from 1992 to 2015 and 2050 for emissions
of CO, NOx, and VOCs (based on IPCC scenario
IS92a).
|
|
Source |
2015 |
2050 |
|
|
|
|
CO |
Energy
Biomass burning |
+15%
+9% |
+66%
+21% |
|
|
|
|
NOx |
Energy
Biomass burning |
+45%
+7% |
+107%
+22% |
|
|
|
|
VOCs |
Energy-related sources
(not isoprene) |
+23% |
+66% |
|
|
4.2.1.6. Tropospheric Transport
In addition to transport by resolved-scale winds, all models considered here
include parameterizations of vertical transport by sub-grid-scale processes
such as convection and turbulent mixing in the boundary layer. Again, the manner
in which these processes are parameterized differs from model to model. In this
context, it is worth noting that four of the models (or their close counterparts)
used in this exercise (ECHAm3/CHEM, HARVARD, UKMO, and Tm3/KNMI) were also involved
in a model intercomparison exercise sponsored by the World Climate Research
Program (WCRP) in 1993 (Jacob et al., 1997). As part of this exercise, each
model simulated a scenario in which a fictitious tracer with a 5.5-day e-folding
lifetime was emitted in the Northern Hemisphere mid-latitude UT. The vertical
gradient in the simulated fields was similar in several of the participating
models. However, there were significant inter-model differences in the simulated
rates of meridional tracer transport in the UT.
4.2.2. Definition of Scenarios
This section describes the scenarios for aircraft emissions evaluated for this
assessment. The premises for current (circa 1992) and future (roughly 2015 and
2050) aircraft fleet emissions, along with descriptions of actual emissions
databases, are given in Chapter 9. The assumptions used
for the background atmosphere in model calculations of the effects of aircraft
emissions on O3 are important and influence the
results. In the following sections, we discuss the basis for background atmospheres
used in model calculations and the aircraft scenarios evaluated.
4.2.2.1. Background Atmospheres
Boundary conditions for CH4 in the background
atmosphere are 1714, 2052, and 2793 ppbv for the years 1992, 2015, and 2050,
respectively. These amounts are based on the IPCC IS92a scenario (IPCC, 1992,
1995). Updated projections for future CH4 concentrations
(WMO, 1999) are smaller than those assumed here. Recent observations by Dlugokencky
et al. (1998) show that CH4 levels currently
are leveling off. If this trend continues during the next century, with little
or no increase in the CH4 concentration, the
increase in background O3 will also be substantially
less than that calculated in these studies.
Table 4-3: Factors of increase from 1992 to 2050 for energy
sources of CO, NOx, and VOCs as applied to
different regions in sensitivity studies.
|
|
NOx |
|
CO |
|
VOCs |
|
|
|
|
|
|
OECD countries |
0.83 |
|
0.25 |
|
1.06 |
|
|
|
|
|
|
Eastern Europe and
Soviet Union |
1.00 |
|
1.00 |
|
1.50 |
|
|
|
|
|
|
Centrally planned
Asia (excluding Korea) |
3.33 |
|
4.67 |
|
6.00 |
|
|
|
|
|
|
North Korea |
2.19 |
|
1.40 |
|
2.11 |
|
|
|
|
|
|
Middle East |
5.53 |
|
3.54 |
|
5.31 |
|
|
|
|
|
|
Southeast Asia |
2.77 |
|
1.77 |
|
2.66 |
|
|
|
|
|
|
South Asia |
9.25 |
|
5.93 |
|
8.89 |
|
|
|
|
|
|
Africa
(without South Africa) |
7.19 |
|
4.60 |
|
6.91 |
|
|
|
|
|
|
South Africa |
3.17 |
|
2.03 |
|
3.04 |
|
|
|
|
|
|
Latin America |
4.85 |
|
3.10 |
|
4.66 |
|
|
For shorter lived gases-such as CO, NOx, and
volatile organic compounds (VOCs)-the participating models use their standard
boundary conditions for the 1992 cases. For 2015 and 2050, most model calculations
assume that emissions are increased by the same factors at all locations relative
to 1992 emissions, as shown in Table 4-2. Such constant
increases were necessitated by difficulties in 3-D models to readily change
emission inputs for assessment studies.
A special sensitivity study was also conducted for 2050 with the UiO model
using a geographically varying emission increase (IPCC, 1995). A summary of
these factors is presented in Table 4-3. Such regional
differential factors are applied only to energy-related sources; biomass burning
factors are applied as in the standard case (using Table
4-2).
4.2.2.2. Aircraft Emission Scenarios
The 3-D aircraft scenarios described in Chapter 9 form
the basis for the assessment. The scenarios evaluated by the participating models
are summarized in Table 4-4. Summaries of global
emissions for these scenarios are given in Tables 9-4
and 9-5. Only a few scenarios are considered for
subsonic assessment calculations because computational requirements for the
3-D models are high. The subsonic scenarios in Table
4-4 are generally analyzed relative to corresponding background atmospheres
for 1992, 2015, or 2050.
In model calculations, aircraft effluents are put into the models as follows:
Gridded fuel burn data (kg fuel/day) are first mapped into the model grid. The
amount of material emitted into each grid box is given by the product of the
fuel burn and the emission index. The emitted material is put into the grid
box at each time step at the equivalent rate. In this approach, we ignore the
effect of plume processing and assume that emitted material is instantaneously
mixed into the grid box. For the subsonic assessment, NOx
is the only aircraft emission considered. Because most models do not calculate
the hydrological cycle in the troposphere, emitted water is not calculated.
Sulfur, CO, and unburned hydrocarbons are also ignored.
The basic scenarios examine some of the important aspects in understanding
the calculated environmental impact of aircraft. However, a number of uncertainties
remain in the treatment of chemical and physical processes that may influence
the effects from aircraft emissions. Therefore, a series of special sensitivity
calculations was designed to investigate the most important of the recognized
uncertainties. The subsonic aircraft sensitivity scenarios, as described later,
examine uncertainties in the background atmosphere, the treatment of chemical
and dynamical processes in the UT and LS, and different analyses of aircraft
emissions.
It has not been possible (for practical reasons) for each of the modeling groups
to run all of the scenarios set up for these 3-D model studies of aircraft perturbations.
Each modeling group has completed a limited number of model simulations.
Table 4-4: Base background scenarios and subsonic aircraft
scenarios.*
|
Model |
Scenarios |
|
A |
1992 Base (background atmosphere, no aircraft) |
B
|
1992 Base + Subsonic Aircraft (Chapter 9, NASA
1992) |
C |
2015 Base (background atmosphere, no aircraft) |
D
|
2015 Base + Subsonic Aircraft (Chapter 9, NASA
2015) |
E |
2050 Base (background atmosphere, no aircraft) |
F |
2050 Base + Subsonic Aircraft (Chapter 9, Fa1) |
G |
2050 Base + Subsonic Aircraft (Chapter 9, Fe1) |
|
*When these scenarios are used in assessing supersonic aircraft
influences, the sulfate distribution in the stratosphere is set to the
stratospheric background SA0 (see Section 4.3). |
|
|