Ice supersaturation and the potential for contrail formation in a changing climate

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Abstract

Ice supersaturation (ISS) in the upper troposphere and lower stratosphere is important for the formation of cirrus clouds and long-lived contrails. Cold ISS (CISS) regions (taken here to be ice-supersaturated regions with temperature below 233 K) are most relevant for contrail formation. We analyse projected changes to the 250 hPa distribution and frequency of CISS regions over the 21st century using data from the Representative Concentration Pathway 8.5 simulations for a selection of Coupled Model Intercomparison Project Phase 5 models. The models show a global-mean, annual-mean decrease in CISS frequency by about one-third, from 11 to 7% by the end of the 21st century, relative to the present-day period 1979-2005. Changes are analysed in further detail for three subregions where air traffic is already high and increasing (Northern Hemisphere mid-latitudes) or expected to increase (tropics and Northern Hemisphere polar regions). The largest change is seen in the tropics, where a reduction of around 9 percentage points in CISS frequency by the end of the century is driven by the strong warming of the upper troposphere. In the Northern Hemisphere mid-latitudes the multi-model-mean change is an increase in CISS frequency of 1 percentage point; however the sign of the change is dependent not only on the model but also on latitude and season. In the Northern Hemisphere polar regions there is an increase in CISS frequency of 5 percentage points in the annual mean. These results suggest that, over the 21st century, climate change may have large impacts on the potential for contrail formation; actual changes to contrail cover will also depend on changes to the volume of air traffic, aircraft technology and flight routing.

Figures

  • Table 1. Characteristics of the CMIP5 models used in this study. The CISS threshold is the threshold RHi value used in the calculation of the annual-mean, global-mean CISS frequency at 250 hPa in the present-day climate (note a temperature threshold of 233 K is also applied). The change in CISS frequency (in percentage points) is calculated as the global-mean, annual-mean CISS frequency in the RCP8.5 simulation over the period 2073–2099 minus that in the historical simulation over the period 1979–2005.
  • Figure 1. Cumulative frequency distribution of 250 hPa relative humidity with respect to ice for ERA-Interim (solid line) and the CMIP5 models (symbols). Global daily data over the period 1979– 2005 are used. The dashed line marks the 90th percentile of the RHi distribution, used to define the model-dependent RHi threshold for ice-supersaturated regions.
  • Figure 2. Annual-mean CISS frequency at 250 hPa over the present-day period 1979–2005 for (a) ERA-Interim reanalysis and the CMIP5 models (b) EC-EARTH, (c) GFDL-ESM2G, (d) HadGEM2-CC, (e) MIROC5 and (f) MPI-ESM-MR. The CISS fields for the five CMIP5 models are repeated in Fig. 4 as labelled contours.
  • Figure 3. PDFs of temperature, T (left column), and specific humidity, q (right column), at 250 hPa in the present-day climate (1979–2005) in three regions – (a, b) the tropics, (c, d) the NH mid-latitudes and (e, f) the NH polar regions – shown for ERA-Interim reanalysis (black line) and CMIP5 models EC-EARTH (dark blue), GFDL-ESM2G (light blue), HadGEM2-CC (orange), MIROC5 (red) and MPI-ESM-MR (dark red). The 233 K temperature threshold is marked by the dashed line on panels (a), (c) and (e).
  • Figure 4. Change in mean CISS frequency at 250 hPa (colours) in percentage points between the RCP8.5 simulation (average over 2073– 2099) and historical simulation (average over 1979–2005) for the CMIP5 models (a) EC-EARTH, (b) GFDL-ESM2G, (c) HadGEM2-CC, (d) MIROC5 and (e) MPI-ESM-MR. The mean CISS frequency (in %) in each model over the historical period 1979–2005 is overlaid (black contours – starting at 2 %, with a 6 % contour interval).
  • Table 2. Changes to the annual-mean frequency of CISS at 250 hPa from the RCP8.5 simulation minus the historical simulation, for the subregions of interest. The change is shown for two time periods: the middle and end of the 21st century.
  • Figure 5. Time series of the multi-model-mean change in CISS frequency (in percentage points) at 250 hPa from 1979 to 2099, calculated for each year as the mean CISS frequency minus the 1979–2005 average (the historical period, shown by grey shading). The change is calculated separately for the tropics (dashed-dotted lines), NH mid-latitudes (solid lines) and NH polar (dashed lines) regions, for the annual (black lines), DJF (blue lines) and JJA (red lines) mean changes. The changes are calculated separately for each CMIP5 model and averaged to provide a multi-model mean; a 10- year running mean has been applied to each time series before plotting.
  • Figure 6. Time series of the change in 250 hPa CISS frequency (in percentage points) in the tropics in the CMIP5 models (symbols) from 1979 to 2099, calculated for each year as the annual-mean CISS frequency minus the 1979–2005 average (the historical period, shown by grey shading). The colour of the points shows the fraction of points in the tropics which are below the 233 K temperature threshold for CISS. A 10-year running mean has been applied to each time series before plotting.

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APA

Irvine, E. A., & Shine, K. P. (2015). Ice supersaturation and the potential for contrail formation in a changing climate. Earth System Dynamics, 6(2), 555–568. https://doi.org/10.5194/esd-6-555-2015

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