Contrail Regions 101 (Part I)
This post is the first in a series breaking down the structure of persistent contrail regions and how these shapes inform navigational avoidance strategies. In this first post, we look at the thickness of contrail regions.
            The thickness of persistent contrail regions
Navigational contrail avoidance is built on the premise that persistent contrail regions are (relatively) easy to avoid. These regions are generally pancake-shaped, thin vertically and broad horizontally. This post is the first in a series where we break down the structure of persistent contrail regions and how these shapes inform navigational avoidance strategies. This first post looks at the thickness of contrail regions. Stay tuned for more!
Condensation trails ("contrails") are the wispy white clouds formed behind aircraft in cold, humid patches of airspace. These man-made clouds are generally harmless, but in particularly cold and humid regions of the atmosphere they can persist and grow for hours into significant cirrus cloud formations (cirrus homogenitus).
On average, the web of contrails from the 25,000 aircraft flying around the globe produces roughly the same amount of warming as all the CO2 emitted by aviation since 1940 (Lee et al. 2021, see our previous post Comparing Contrails and CO2).
The good news is that it may be simple to reduce contrail warming. We can often fly around these icy regions that form persistent, harmful contrails. Re-routing flights like this is often called navigational contrail avoidance.
Navigational avoidance is built on the premise that persistent contrail regions are sparse and (relatively) easy to avoid. These regions are often pancake-shaped—very thin vertically, and broad horizontally—and can be bypassed by moving aircraft slightly up, down, or occasionally around. For the new parents out there, it's the opposite of We're Going on a Bear Hunt. We can go over it, we can go under it, we can go around it, but we mustn't go through it.
For persistent contrails to form, a region of airspace must:
- Be cold enough to cause wet, hot engine exhaust to form ice crystals on engine emissions or pre-existing atmospheric aerosols (i.e., tiny particles). The Schmidt-Appleman Criterion (SAC) predicts these conditions.[1] Most contrails that initially form will vaporize in a few minutes (harmless).
 - Be humid enough to freeze additional water vapor onto the initial contrail. The technical term for these atmospheric regions is ice super-saturated regions (ISSRs). When contrails form in ISSRs, they can persist and grow for many hours (potentially harmful).
 
When an aircraft satisfies the Schmidt-Appleman Criterion in a region of atmosphere that is ice super-saturated, we call it a persistent contrail region (PCR).
Can we avoid persistent contrails by flying higher or lower?
We often hear that ice super-saturated regions and persistent contrail regions are ~1,000 feet (or a few hundred meters) thick on average.
To put that in a relevant context, aircraft fly at specific altitudes called flight levels (FL). Flight levels are spaced out every 1,000 feet (~300 m) and labelled in hundreds of feet, e.g., FL300 = 30,000 ft, FL410 = 41,000 ft, etc. In most air traffic regimes, aircraft alternate direction every flight level (typically East-West),[2] so if an aircraft wants to fly higher or lower, it actually must move two flight levels (2,000 ft, or ~600 m) up or down.[3]
If contrail regions are only around a thousand feet thick, then aircraft should only have to move up or down one vertical movement (two flight levels) to avoid them.
But what's the evidence for this premise? Given the magnitude of contrail impacts and the potential to reduce them, we'd expect to see a wide literature studying the thickness of contrail regions. Surprisingly, there are only a few comprehensive studies to reference (outside a few with limited geographies).[4]
For the rest of this post, we'll look at some of the best vertical atmospheric measurements (atmospheric soundings) to gain intuition around the thickness of contrail regions and how this informs navigational avoidance strategies.
What measurements are available?
Unsurprisingly, measuring the temperature and humidity profile of a column of airspace 30,000 feet up (10,000 m) is not easy. The best data we have with any degree of coverage comes from radiosondes (or weather balloons).
Thousands of radiosondes are launched every day from all over the world, including mega-cities and remote islands. The balloons gently float up, radioing measurements of temperature, humidity and other properties back to Earth before popping high in the atmosphere, job done.

These global radiosondes would be ideal for measuring contrail region thickness, but most aren't capable of detecting thin subtle ISSRs. Luckily, we can use a subset of radiosondes known as the Global Climate Observing System Reference Upper-Air Network (GRUAN). GRUAN is an international effort providing high-quality, reference-grade measurements of the upper atmosphere from a network of stations worldwide.
GRUAN's data are renowned for their rigorous calibration, consistent methodologies, and comprehensive metadata. Crucially, GRUAN's dataset has high vertical-resolution humidity and temperature profiles, which are essential for identifying thin ISSR regions.[5] There are lots of other radiosonde data available, but they just aren't calibrated as well as the GRUAN data, or in many cases, we don't have the raw vertical resolution to detect ISSR thickness.
We use GRUAN data in this post to explore contrail region thickness. The data spans the last decade, over 24 stations on 7 continents, with over 100,000 radiosonde launches:
See Methodology Notes for more details on how the data was processed.
So how thick are contrail regions according to the measurements?
We can look at the thickness distribution of ice super-saturated regions (ISSRs) and persistent contrail regions (PCR = SAC & ISSR) in the GRUAN data. According to the radiosondes, more than 80% of ISSRs and PCRs are less than 2,000 feet thick (2 flight levels) and about two-thirds are less than 1,000 feet thick. A very small minority—about 5%—are more than 4,000 feet thick:
Persistent contrail regions are less frequent than ISSRs but tend to be thicker than ISSRs—a conclusion also found in other radiosonde studies.[4:1] PCRs are less frequent because they are a subset of ISSRs, and they tend to be thicker because many of the thinnest ISSRs are less likely to form contrails (i.e., satisfy SAC).
In general, PCR thickness doesn't vary much with season, time of day, and geography. Winter produces the thickest persistent contrail regions (due to lower temperatures), but the variation across season is negligible for most of the distribution. There is a modest difference in the thickest regions: ~17% of persistent contrail regions are thicker than 2,000 feet in the winter, but this falls to ~14% in the summer. Similar variation occurs between (slightly) thicker contrail regions in polar latitudes (between 60° and 90°) and thinner regions in tropical latitudes (between 0° and 30°).
How does this inform navigational contrail avoidance?
The actual thicknesses of contrail regions might not be the critical question for navigational avoidance. We'd like to know how far we have to move aircraft to find contrail-free airspace. In particular:
- How often do we encounter a PCR at a given flight level?
 - Can we avoid the PCR at this flight level by adjusting up or down one vertical step (2,000 feet, or 2 flight levels)?
 - How often do we need to move 4,000 feet or more?
 
The chart below shows the likelihood of running into a PCR (based on GRUAN data) at typical commercial aircraft cruising altitudes (FL250—FL400). The chart also shows the likelihood of avoiding the PCR with 1, 2, or 3 vertical steps (2, 4, or 6 flight levels) for an aircraft flying at a specific flight level.
Remember this analysis is only looking at PCR avoidance in one vertical column of space. In practice, avoidance might be more complicated. There might be another PCR at a different altitude slightly downstream, or we might not be able to move up or down due to traffic. We also might be at the current ceiling of the aircraft for it's payload. All these considerations have to be taken into account by trajectory and traffic optimizers. Luckily we don't have to limit ourselves to single vertical maneuvers to avoid PCRs.
The likelihood of running into a PCR on any flight level varies from about 5% to 10%, with the highest probability in FL320 and FL330. In reality, the flight level with the highest PCR probability varies a little with season and latitude, and so the peak shown here is more a reflection of the time and locations of the GRUAN dataset.
In about 30% of PCRs, one step (2,000 feet) in either direction could avoid the region (the dark grey bar). In around half of PCRs, the region could be avoided by one step up or down (2,000 feet), but not both (the dark blue bar).
So 80% of the time, a flight level change of 2,000 feet (the minimum allowed in most air traffic control systems) avoids the contrail region. Of the remaining 20% of PCRs, over 80% could be avoided by a flight level change of 4,000 feet (2 steps).
The probability that an aircraft requires three vertical steps (6,000+ feet) to avoid a PCR is less than 5% (the orange bar), typically around 3% in the most common cruise altitudes for commercial aircraft.
Conclusion
The radiosonde data clearly supports the claim that persistent contrail regions (and ice super-saturated regions) are around 1,000 feet thick. Over 80% of the PCRs and ISSRs in the GRUAN data were less than 2,000 feet. Only 5% of regions exceed 4,000 feet thick.
The data also suggests that a single vertical step (2,000 feet, or 2 flight levels) is often sufficient to move a flight out of a persistent contrail region. While this may be hard to achieve in practice, it provides empirical support for intuition built on numerical weather prediction models.[6]
In the rest of this series, we'll look at other characteristics of contrail regions (e.g., vertical spacing of regions, breadth, frequency) and how they affect the potential for navigational avoidance.
Methodology Notes
For those interested in reproducing these results:
- Dataset includes all GRAUN data up to July 2025 from all four instruments available (Vaisala RS41 & RS92, and Meisei iMS-100 & RS-11G radiosondes).
 - Pressure levels converted to geopotential height (flight levels) using International Standard Atmosphere. Radiosonde data filtered for valid temperature and humidity readings between 25,000 and 45,000 feet.
 - pycontrails used to convert humidity readings to RHice and determine SAC using an engine efficiency of 30%.
 - Persistent contrail regions were defined as where SAC is satisfied and RHice > 100%.
 - We used a continuous region tolerance of 100 feet when defining vertical regions. This means if the data drops below the PCR threshold for less than 100 feet, the algorithm still considers it a continuous contrail region. In other words, at least 100 feet of clear air was required to define the edge of a contrail region. This has a tendency to slightly amalgamate contrail regions, but smooths sensor noise on and relative humidity measurements bouncing around 100%.
 - Seasons were defined purely by date of launch and the sign of the latitude:
- March/April/May (Spring in Northern Hemisphere, Autumn in Southern)
 - June/July/August (Northern Summer; Southern Winter)
 - September/October/November (Northern Autumn; Southern Spring)
 - December/January/February (Northern Winter; Southern Summer).
 
 
Glossary
- FL: Flight Level
 - ISSR: Ice super-saturated region
 - PCR: Persistent contrail region
 - SAC: Schmidt-Appleman criteria
 
Footnotes
The Schmidt-Appleman Criteria (SAC) is named after Ernst Schmidt (German scientist) and Herbert Appleman (American meteorologist) who independently developed similar theories of contrail formation in the 1940s and 1950s. It's sometimes assumed to be a pure statement of thermodynamic equilibrium, but this is not quite true. The SAC is a simplified model of the complex non-equilibrium phase change process going on in the wake of a jet engine, with significant simplifying assumptions. While it's generally a good predictor of initial contrail formation, it's not perfect. ↩︎
There are some exceptions to the "semi-circular rule", where eastbound flights use odd flight levels (e.g., FL310, FL330, etc.) and westbound flights use even ones. The most significant exception is the North Atlantic track system (NAT OTS). These are the tracks available for eastbound flights over the Atlantic at (European) night-time and for westbound flights in the European afternoon. In the NAT OTS, every flight level (i.e., odds and evens) is used, even though all flights are going in one direction. ↩︎
To make things even more confusing, it's not really 1,000 feet either. FL300 is actually a pressure level, meaning an altitude of constant atmospheric pressure. The aircraft flies at the ambient pressure that would be at 30,000 feet if the atmosphere matched the International Standard Atmosphere model (effectively, a fixed pressure). That means on any given day, FL300 is not exactly 30,000 feet above sea level, nor is it at the same altitude above sea level everywhere on Earth at any point in time. Luckily, meteorology also works in pressure levels for the simple reason that it's much easier to measure than actual height above sea level. ↩︎
There are, of course, many studies that quote the thickness of ISSRs, typically from one radiosonde site or a handful of sites in one region. The original studies we've found use radiosonde data like we have here, but often without the high resolution we now have in the GRUAN datasets. Without the high resolution datasets, studies can't pick up thinner ISSRs (typically less then around 400m). This will tend to make the mean and medium thicknesses larger. Here are a few annotated references:
- Ebright, B.C. et al. (2024) “Climatology of ice supersaturation and contrail formation conditions in Washington, DC airspace,” Aerospace, 11(7), p. 656.
- This recent 2024 study uses a similar methodology to this post, but with 2015-2020 radiosondes primarily launched from Washington Dulles airport and some surrounding mid-Atlantic launch sites. They find an ISSR thickness of around 600m, but note that the vertical resolution is only 250 - 400 m. The study also finds (like this post - spoiler!) that the PCR thickness distribution is a little thicker than ISSR (~1200m)
 
 - Sausen, R. et al. (1998) “A diagnostic study of the global distribution of contrails,” Journal of Geophysical Research: Atmospheres, 103(D12), pp. 15749–15760.
- This 1998 study used high-resolution data from UK Met Office radiosondes in Bracknell to estimate contrail layer depths, finding a mean PCR thickness of ~1,100m.
 
 - Gierens, K. et al. (2020) “Climatology of ice-supersaturated regions in the Arctic: vertical extent and temporal variability,” Meteorologische Zeitschrift, 29(6), pp. 465–482.
- This 2020 study uses radiosondes in 4 Arctic sites, finding median ISSR thicknesses around 150m.
 
 - Stuefer, M. and Wendler, G. (2005) “Climatology of contrail occurrence over Fairbanks, Alaska, derived from radiosonde data,” Proceedings of the 13th AMS Conference on Aviation, Range, and Aerospace Meteorology. American Meteorological Society.
- This study uses radiosondes from Fairbanks, Alaska from 1998-2002 to find mean arctic PCR thicknesses of 1.7 km in summer and 3.7 km in winter. However, the radiosonde data has a resolution of ~400-800m.
 
 - Minnis, P. et al. (1997) “Contrail formation regions derived from radiosonde data,” Journal of Climate, 10(10), pp. 2414–2424.
- This 1997 study uses radiosonde data from Boulder, CO, USA. The study found contrail formation layer depths varying from 600m in summer to 1300m in winter. The study did not use high resolution radiosonde data, so vertical resolution was around 400-800m.
 
 - Treffeisen, R. et al. (2007) “Ice supersaturation occurrence and related statistics in the upper troposphere over Lindenberg/Ny-Ålesund,” Atmospheric Chemistry and Physics Discussions, 7(5), pp. 13097–13136.
- This 2007 study uses radiosondes in Lindenberg, Germany (lead center for GRAUN!) to place ISSR thickness into 200m bins.
 
 - Spichtinger, P. et al. (2005) “Ice supersaturation in the UT/LS: results from radiosonde data and implications for circulation and chemistry,” Atmospheric Chemistry and Physics, 5(1), pp. 97–110.
- Similarly, this 2005 study uses radiosondes from Lindenberg to find typical ISSR thickness is a few hundred meters. They presented case studies with exceptionally thick layers of 2,000m or more found in special synoptic situations.
 
 
- Ebright, B.C. et al. (2024) “Climatology of ice supersaturation and contrail formation conditions in Washington, DC airspace,” Aerospace, 11(7), p. 656.
 More details on GRUAN data quality in Immler et al. (2010) and Bodeker et al. (2016) ↩︎
Teoh, R., Schumann, U. and Stettler, M.E.J. (2020) “Beyond Contrail Avoidance: Efficacy of Flight Altitude Changes to Minimise Contrail Climate Forcing,” Aerospace, 7(9), p. 121. Available at: https://doi.org/10.3390/aerospace7090121. ↩︎