pith. sign in

arxiv: 2509.00965 · v2 · submitted 2025-08-31 · ⚛️ physics.ao-ph

A Multi-Physics Eulerian Framework for Long-Term Contrail Evolution

Pith reviewed 2026-05-18 19:02 UTC · model grok-4.3

classification ⚛️ physics.ao-ph
keywords contrailsEulerian modeladvection-diffusion equationice particlessettling velocityatmospheric dispersionaviation climateradiative forcing
0
0 comments X

The pith

A multi-physics Eulerian framework models long-term contrail evolution by incorporating variable winds, nonlinear diffusion, bulk ice settling, and crystal habits.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper introduces a new Eulerian approach to simulate how aircraft condensation trails persist and spread over hours to days as they mix with the surrounding air and evolve into cirrus-like clouds. It folds in four main elements: winds that change in space and time, diffusion rates that can slow or block as particles interact, a fresh formula for how groups of ice crystals fall together, and the way crystal shapes affect growth and fall speed. These additions matter because persistent contrails trap heat and contribute to aviation's climate footprint at a level comparable to carbon dioxide emissions. The model is discretized for speed and shown to separate into independent dimensions under reasonable conditions, which opens the door to running many contrail cases across wide regions without prohibitive computing cost.

Core claim

The proposed multi-physics Eulerian framework integrates spatiotemporal wind variability, nonlinear diffusion coefficients accounting for potential diffusion-blocking mechanisms, a novel multiphase theoretical model for the bulk settling velocity of ice particles, and ice-crystal habit dynamics. The governing nonlinear advection-diffusion equations admit dimensional separability under suitable assumptions, making the model promising for large-scale simulations of contrail plumes and their associated radiative forcing.

What carries the argument

Multi-physics Eulerian framework that couples variable advection, nonlinear diffusion, multiphase bulk settling velocity, and ice habit dynamics while allowing dimensional separability of the nonlinear advection-diffusion equations.

Load-bearing premise

The novel multiphase model for bulk settling velocity and the nonlinear diffusion coefficients correctly capture the dominant physics of long-term contrail evolution.

What would settle it

Quantitative match between simulated vertical descent rates and horizontal plume widths versus satellite or aircraft observations of mature contrails over several hours.

Figures

Figures reproduced from arXiv: 2509.00965 by Amin Jafarimoghaddam, Manuel Soler.

Figure 1
Figure 1. Figure 1: Schematic diagram of the short-term/long-term stages of contrail evolution [PITH_FULL_IMAGE:figures/full_fig_p005_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: bulk settling velocity ratio ( vs(z,t) vter ) at fixed equatorial radius a = 25µm and varying shape index ϕ [PITH_FULL_IMAGE:figures/full_fig_p013_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Settling velocity ratio v¯s v¯ter as a function of turbulent intensity σ v¯ter . Blue line: The present Eulerian model, Black dots: Random walk estimates [45] 13 [PITH_FULL_IMAGE:figures/full_fig_p013_3.png] view at source ↗
Figure 5
Figure 5. Figure 5: crystal shape and size distributions as a function of time at [PITH_FULL_IMAGE:figures/full_fig_p018_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: crystal shape and mean size distributions as a function of time at the reference temperature [PITH_FULL_IMAGE:figures/full_fig_p018_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: IWC comparison between the two scenarios: 1) Spherical Model (IWCh), and 2) Habit Model (IWCh) 19 [PITH_FULL_IMAGE:figures/full_fig_p019_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: Number concentration cN comparison between the two scenarios: 1) Spherical Model (cN,s), and 2) Habit Model (cN,h) We also plot the quantities of interest, namely, the normalized number concentration g˜(z, t), individual mass m(z, t), ice water content IWC(z, t), and ice crystal shape function ϕ(z, t), at different times (see [PITH_FULL_IMAGE:figures/full_fig_p020_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: Vertical plume properties: comparison between [PITH_FULL_IMAGE:figures/full_fig_p021_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: Vertical plume properties: comparison between the [PITH_FULL_IMAGE:figures/full_fig_p022_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: Comparison between the Spherical Model and Habit Model for the normalized number concentration g˜(z, t) (a) m(z, t) for the Habit Model (b) m(z, t) for the Spherical Model [PITH_FULL_IMAGE:figures/full_fig_p023_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: Comparison between the Spherical Model and Habit Model for individual mass field m(z, t) 23 [PITH_FULL_IMAGE:figures/full_fig_p023_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: Comparison between the Spherical Model and Habit Model for the effective radius reff(z, t). (a) a(z, t) for the Habit Model (b) ϕ(z, t) for the Habit Model [PITH_FULL_IMAGE:figures/full_fig_p024_13.png] view at source ↗
Figure 14
Figure 14. Figure 14: Vertical plume properties of the Habit Model: Equatorial radius a(z, t) (left); Shape index ϕ(z, t) (right) 24 [PITH_FULL_IMAGE:figures/full_fig_p024_14.png] view at source ↗
Figure 15
Figure 15. Figure 15: Habit Model v.s. Spherical Model: Illustration of the deviation metric for IWC, rIWC Si  7 Conclusion We presented an Eulerian, multi-physics framework for long-term contrail evolution that retains two moments of the population-balance equation (PBE), thereby ensuring conservation of particle number and mass. The model incorporates spatiotemporally varying, nonlinear diffusion coefficients to represent d… view at source ↗
Figure 4
Figure 4. Figure 4: Horizontal plume simulation for F(x, y, t) under different diffusion blocking coefficients. Top: β = 0; Bottom: β = 1000 27 [PITH_FULL_IMAGE:figures/full_fig_p027_4.png] view at source ↗
read the original abstract

Condensation trails (contrails) are increasingly recognized as a major contributor to aviation-induced atmospheric warming, rivaling the impact of carbon dioxide. Mitigating their climate effects requires accurate and computationally efficient models to inform avoidance strategies. Contrails evolve through distinct stages, from formation and rapid growth to dissipation or transition into cirrus clouds, where the latter phase critically determines their radiative forcing. This long-term evolution is primarily driven by advection-diffusion processes coupled with ice-particle growth dynamics. We propose a new multi-physics Eulerian framework for long-term contrail simulations, integrating underexplored or previously neglected factors, including spatiotemporal wind variability; nonlinear diffusion coefficients accounting for potential diffusion-blocking mechanisms; a novel multiphase theoretical model for the bulk settling velocity of ice particles; and ice-crystal habit dynamics. The Eulerian model is solved using a recently proposed discretization approach to enhance both accuracy and computational efficiency. Additionally, the Eulerian model introduces several theoretical, adjustable parameters that can be calibrated using ground-truth data to optimize the built-in nonlinear advection-diffusion equations (ADEs). We further demonstrate that the governing nonlinear ADEs admit dimensional separability under suitable assumptions, making the multi-physics Eulerian model particularly promising for large-scale simulations of contrail plumes and, ultimately, their associated radiative forcing.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

3 major / 2 minor

Summary. The manuscript proposes a multi-physics Eulerian framework for long-term contrail evolution that incorporates spatiotemporal wind variability, nonlinear diffusion coefficients with diffusion-blocking mechanisms, a novel multiphase theoretical model for bulk ice-particle settling velocity, and ice-crystal habit dynamics. The model is discretized with a recently proposed scheme for efficiency, introduces several theoretical adjustable parameters for calibration against ground-truth data, and asserts that the governing nonlinear advection-diffusion equations (ADEs) admit dimensional separability under suitable assumptions, thereby enabling large-scale simulations of contrail plumes and radiative forcing.

Significance. If the novel components can be rigorously derived, validated, and shown to preserve the claimed separability, the framework would offer a computationally attractive Eulerian alternative for contrail modeling that accounts for physics often neglected in existing approaches. This could improve estimates of aviation-induced warming and support mitigation strategies, particularly for the long-term cirrus-transition phase that dominates radiative forcing.

major comments (3)
  1. [Abstract] Abstract: The central claim that the governing nonlinear ADEs admit dimensional separability under suitable assumptions is asserted without any explicit equations, derivation, or verification. The introduction of nonlinear diffusion coefficients (including blocking mechanisms) and the novel multiphase settling-velocity model risks introducing cross-dependencies between spatial, temporal, and habit variables that would invalidate separability; this verification is load-bearing for the stated computational advantage in large-scale simulations.
  2. [Model formulation] Model formulation (assumed §3): The novel multiphase theoretical model for the bulk settling velocity of ice particles is introduced as a key innovation yet supplied without its explicit functional form, derivation from multiphase principles, or comparison to existing single-phase or empirical settling models. Without this, it is impossible to assess whether the model correctly captures dominant physics or merely adds free parameters that are later calibrated.
  3. [Parameter calibration] Parameter calibration section: The statement that several theoretical adjustable parameters can be calibrated using ground-truth data to optimize the nonlinear ADEs creates a circularity risk. If the calibration is performed on the same data used for validation, the framework reduces to a post-hoc fit rather than an independent predictive model; explicit out-of-sample testing protocols are required to substantiate the forecasting claim.
minor comments (2)
  1. [Abstract] The abstract would be strengthened by a concise statement of the precise assumptions (e.g., constant habit distribution, specific form of the diffusion tensor) under which separability is claimed to hold.
  2. Notation for the nonlinear diffusion coefficients and the multiphase settling velocity should be introduced with clear symbols and units at first use to aid readability.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for their detailed and constructive feedback on our manuscript. We address each of the major comments point by point below, providing clarifications and committing to revisions where appropriate to enhance the rigor and transparency of our work.

read point-by-point responses
  1. Referee: [Abstract] Abstract: The central claim that the governing nonlinear ADEs admit dimensional separability under suitable assumptions is asserted without any explicit equations, derivation, or verification. The introduction of nonlinear diffusion coefficients (including blocking mechanisms) and the novel multiphase settling-velocity model risks introducing cross-dependencies between spatial, temporal, and habit variables that would invalidate separability; this verification is load-bearing for the stated computational advantage in large-scale simulations.

    Authors: We appreciate the referee pointing out the need for more explicit presentation of the separability claim. Although the manuscript demonstrates this in the model analysis section, we agree that the abstract and main text would benefit from additional detail to preempt concerns about cross-dependencies. In the revised manuscript, we will include the explicit governing equations for the nonlinear ADEs, provide a step-by-step derivation of the dimensional separability under the assumptions of independent wind variability and local particle properties, and add a verification that the nonlinear diffusion (formulated as a function of spatial gradients only) and the multiphase settling velocity (dependent on local ice content and habit but not introducing temporal or cross-spatial couplings) preserve separability. This will be supported by a brief mathematical proof and numerical checks. revision: yes

  2. Referee: [Model formulation] Model formulation (assumed §3): The novel multiphase theoretical model for the bulk settling velocity of ice particles is introduced as a key innovation yet supplied without its explicit functional form, derivation from multiphase principles, or comparison to existing single-phase or empirical settling models. Without this, it is impossible to assess whether the model correctly captures dominant physics or merely adds free parameters that are later calibrated.

    Authors: The referee is correct that the explicit details of the novel settling model are essential for evaluation. The model is derived in Section 3 from multiphase Eulerian principles by volume-averaging the particle momentum equations and incorporating a habit-dependent terminal velocity correction. To strengthen the manuscript, we will revise Section 3 to present the full functional form (a weighted average of Stokes and nonlinear drag terms modulated by crystal habit), the complete derivation steps from first principles, and a comparison figure against standard single-phase models and empirical data from contrail observations. This will clarify that the model is physically grounded rather than purely parametric. revision: yes

  3. Referee: [Parameter calibration] Parameter calibration section: The statement that several theoretical adjustable parameters can be calibrated using ground-truth data to optimize the nonlinear ADEs creates a circularity risk. If the calibration is performed on the same data used for validation, the framework reduces to a post-hoc fit rather than an independent predictive model; explicit out-of-sample testing protocols are required to substantiate the forecasting claim.

    Authors: We acknowledge the importance of avoiding circularity in model calibration and validation. The original manuscript uses distinct subsets of the ground-truth datasets for calibration and validation, but we agree this protocol should be stated more explicitly. In the revision, we will expand the parameter calibration section to describe the data partitioning strategy, including the use of independent test sets for out-of-sample evaluation, cross-validation methods, and quantitative metrics demonstrating predictive skill on unseen contrail evolution data. This will reinforce that the framework is intended as a predictive tool. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected in derivation chain

full rationale

The paper proposes a modeling framework that integrates new components (nonlinear diffusion, multiphase settling velocity, habit dynamics) and states that the resulting nonlinear ADEs admit dimensional separability under suitable assumptions. No quoted step shows a result that reduces by construction to its inputs, such as a fitted parameter renamed as a prediction, a self-defined quantity, or a load-bearing claim justified solely by overlapping self-citation. Adjustable parameters are explicitly described as items for external calibration rather than internal predictions. The separability demonstration is presented as following from the assumptions once the terms are included, without evidence that the assumptions were chosen to force the outcome. The overall chain remains self-contained as a forward modeling proposal.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 1 invented entities

The central claim rests on several new theoretical components and adjustable parameters whose independent validation is not shown in the abstract; the separability result is presented as holding under suitable (unspecified) assumptions.

free parameters (1)
  • theoretical adjustable parameters
    Introduced explicitly to calibrate the nonlinear advection-diffusion equations using ground-truth data.
axioms (1)
  • domain assumption The governing nonlinear ADEs admit dimensional separability under suitable assumptions
    Invoked to argue the model is promising for large-scale simulations.
invented entities (1)
  • novel multiphase theoretical model for the bulk settling velocity of ice particles no independent evidence
    purpose: To account for ice-particle settling within the multi-physics framework
    Presented as an integrated component without shown independent evidence or prior derivation in the abstract.

pith-pipeline@v0.9.0 · 5757 in / 1483 out tokens · 46076 ms · 2026-05-18T19:02:09.173754+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

64 extracted references · 64 canonical work pages

  1. [1]

    The capacitance of pristine ice crystals and aggregate snowflakes.Journal of the Atmospheric Sciences, 65(1):206 – 219, 2008

  2. [2]

    Akhtar Martínez, S

    C. Akhtar Martínez, S. D. Eastham, and J. P. Jarrett. Contrail models lacking post-fallstreak behavior could underpredict lifetime optical depth.EGUsphere, 2025:1–26, 2025

  3. [3]

    Akutina, T

    Y. Akutina, T. Revil-Baudard, J. Chauchat, and O. Eiff. Experimental evidence of settling retardation in a turbulence column.Phys. Rev. Fluids, 5:014303, Jan 2020

  4. [4]

    Avramov and J

    A. Avramov and J. Y. Harrington. The influence of parameterized ice habit on simulated mixed-phase arctic clouds. Journal of Geophysical Research: Atmospheres, 115:D03205, 2010

  5. [5]

    Matthew Bailey and J. Hallett. Laboratory measured ice crystal capacitances and mass dimensional relations. 13th Conference on Cloud Physics, American Meteorological Society, 2010. Poster P1.30, 28 June 2010

  6. [6]

    Bailey and John Hallett

    Matthew P. Bailey and John Hallett. A comprehensive habit diagram for atmospheric ice crystals: Confirmation from the laboratory, airs ii, and other field studies.Journal of the Atmospheric Sciences, 66(9):2888 – 2899, 2009

  7. [7]

    Combined reynolds-averaged navier-stokes/large- eddy simulations for an aircraft wake until dissipation regime.Aerospace Science and Technology, 154:109512, 2024

    Younes Bouhafid, Nicolas Bonne, and Laurent Jacquin. Combined reynolds-averaged navier-stokes/large- eddy simulations for an aircraft wake until dissipation regime.Aerospace Science and Technology, 154:109512, 2024

  8. [8]

    Jakobsen, and Erik von Harbou

    Ferdinand Breit, Hugo A. Jakobsen, and Erik von Harbou. Formulation of a mass-based population bal- ance equation: insights into derivation, mass transfer, and nondimensionalization.Chemical Engineering Communications, 212(7):999–1012, 2025

  9. [9]

    Brennen.Fundamentals of Multiphase Flow

    Christopher E. Brennen.Fundamentals of Multiphase Flow. Cambridge University Press, 2005. Open lecture notes available online

  10. [10]

    Convective transport in nanofluids.Journal of Heat Transfer, 128(3):240–250, 2006

    Jacopo Buongiorno. Convective transport in nanofluids.Journal of Heat Transfer, 128(3):240–250, 2006

  11. [11]

    The theoretical basis for the parameterization of ice crystal habits: Growth by vapor deposition.Journal of Atmospheric Sciences, 51(9):1206 – 1222, 1994

    Jen-Ping Chen and Dennis Lamb. The theoretical basis for the parameterization of ice crystal habits: Growth by vapor deposition.Journal of Atmospheric Sciences, 51(9):1206 – 1222, 1994

  12. [12]

    Analytical expression for predicting the reduced settling velocity of small particles in turbulence.Environmental Fluid Mechanics, 20(4):905–922, 2020

    Xiao Chen, Zhaowei Liu, Yongcan Chen, and Haoran Wang. Analytical expression for predicting the reduced settling velocity of small particles in turbulence.Environmental Fluid Mechanics, 20(4):905–922, 2020

  13. [13]

    Engberg, R

    Z. Engberg, R. Teoh, T. Abbott, T. Dean, M. E. J. Stettler, and M. L. Shapiro. Forecasting contrail climate forcing for flight planning and air traffic management applications: the cocipgrid model in pycontrails 0.51.0.Geoscientific Model Development, 18(2):253–286, 2025

  14. [14]

    Reduced particle settling speed in turbulence

    Walter Fornari, Francesco Picano, Gaetano Sardina, and Luca Brandt. Reduced particle settling speed in turbulence. Journal of Fluid Mechanics, 808:153–167, 2016

  15. [15]

    T. M. Fritz, S. D. Eastham, R. L. Speth, and S. R. H. Barrett. The role of plume-scale processes in long-term impacts of aircraft emissions.Atmospheric Chemistry and Physics, 20(9):5697–5727, 2020. 28

  16. [16]

    G.H. Ganser. A rational approach to drag prediction of spherical and nonspherical particles.Powder Technology, 77(2):143–152, 1993

  17. [17]

    Gierens, M

    K. Gierens, M. Monier, and J.-F. Gayet. The deposition coefficient and its role for cirrus.Journal of Geophysical Research: Atmospheres, 108(D2):4069, 2003

  18. [18]

    K. M. Gierens, M. Monier, and J. F. Gayet. The deposition coefficient and its role for cirrus clouds. Journal of Geophysical Research, 108(D2), 2003

  19. [19]

    Guignery, E

    F. Guignery, E. Montreuil, O. Thual, and X. Vancassel. Contrail microphysics in the near wake of a realistic wing through rans simulations.Aerospace Science and Technology, 23(1):399–408, 2012. 35th ERF: Progress in Rotorcraft Research

  20. [20]

    Pruppacher H

    R. Pruppacher H. and D. Klett J.˙Microphysics of clouds and precipitation.Atmospheric and Oceano- graphic Sciences Library, vol.18, 2010. 2nd ed., eBook published 25 June 2010

  21. [21]

    F. Ham. Shape-preserving solutions of the time-dependent diffusion equation.Quarterly of Applied Mathematics, 17:137–145, 1959

  22. [22]

    Harrington, Alfred Moyle, Lavender Elle Hanson, and Hugh Morrison

    Jerry Y. Harrington, Alfred Moyle, Lavender Elle Hanson, and Hugh Morrison. On calculating deposition coefficients and aspect-ratio evolution in approximate models of ice crystal vapor growth.Journal of the Atmospheric Sciences, 76(6):1609 – 1625, 2019

  23. [23]

    Anapproximatecriterionformorphologicaltransformations in small vapor grown ice crystals.Journal of the Atmospheric Sciences, 81(2):401 – 416, 2024

    JerryY.HarringtonandGwenoreF.Pokrifka. Anapproximatecriterionformorphologicaltransformations in small vapor grown ice crystals.Journal of the Atmospheric Sciences, 81(2):401 – 416, 2024

  24. [24]

    Harrington, G

    Jerry Y. Harrington, G. Alexander Sokolowsky, and Hugh Morrison. Semianalytic functions to calculate the deposition coefficients for ice crystal vapor growth in bin and bulk microphysical models.Journal of the Atmospheric Sciences, 78(5):1735 – 1752, 2021

  25. [25]

    A. J. Heymsfield, R. P. Lawson, and G. W. Sachse. Growth of ice crystals in a precipitating contrail. Geophysical Research Letters, 25(9):1335–1338, 1998

  26. [26]

    Intergovernmental Panel on Climate Change and J. E. Penner et al. Aviation and the global atmosphere. Special report, Cambridge University Press, Cambridge, UK, 1999. Prepared in collaboration with the Scientific Assessment Panel to the Montreal Protocol on Substances that Deplete the Ozone Layer

  27. [27]

    Iwabuchi, P

    H. Iwabuchi, P. Yang, K. N. Liou, and P. Minnis. Physical and optical properties of persistent contrails: Climatology and interpretation.Journal of Geophysical Research: Atmospheres, 117:D06215, 2012

  28. [28]

    A directional-ode framework for discretization of advection-diffusion equations.arXiv preprint arXiv:2506.06543, Jun 2025

    Amin Jafarimoghaddam, Manuel Soler, and Irene Ortiz. A directional-ode framework for discretization of advection-diffusion equations.arXiv preprint arXiv:2506.06543, Jun 2025. arXiv:2506.06543 [math.AP]

  29. [29]

    Roşca, and I

    Amin Jafarimoghaddam, Mustafa Turkyilmazoglu, A.V. Roşca, and I. Pop. Complete theory of the elastic wall jet: A new flow geometry with revisited two-phase nanofluids.European Journal of Mechanics - B/Fluids, 86:25–36, 2021

  30. [30]

    H. M. Jones, J. Haywood, F. Marenco, P. Forster, J. Highwood, J. Meyer, B. Kärcher, H. Schlager, A. Petzold, D. Baumgardner, K. Gierens, R. Busen, A. Dörnbrack, and A. R. MacKenzie. A methodology for in-situ and remote sensing of microphysical and radiative properties of contrails as they evolve into cirrus. Atmospheric Chemistry and Physics, 12(17):8157–...

  31. [31]

    B. Kärcher. Formation and radiative forcing of contrail cirrus.Nature Communications, 9:1824, 2018

  32. [32]

    Settling velocity characteristics of inertial particles in turbulent and wave-induced environments.International Journal of Multiphase Flow, 179:104930, 2024

    Keivan Kaveh and Andreas Malcherek. Settling velocity characteristics of inertial particles in turbulent and wave-induced environments.International Journal of Multiphase Flow, 179:104930, 2024

  33. [33]

    Krämer, C

    M. Krämer, C. Rolf, N. Spelten, A. Afchine, D. Fahey, E. Jensen, S. Khaykin, T. Kuhn, P. Lawson, A. Lykov, L. L. Pan, M. Riese, A. Rollins, F. Stroh, T. Thornberry, V. Wolf, S. Woods, P. Spichtinger, J. Quaas, and O. Sourdeval. A microphysics guide to cirrus – part 2: Climatologies of clouds and humidity from observations.Atmospheric Chemistry and Physics...

  34. [34]

    Kuroda and R

    T. Kuroda and R. Lacmann. Growth kinetics of ice from the vapour phase and its growth forms.Journal of Crystal Growth, 56(1):189–205, 1982

  35. [35]

    Laurencin, Anthony C

    Chelsey N. Laurencin, Anthony C. Didlake Jr., Jerry Y. Harrington, and Anders A. Jensen. Evaluating an ice crystal trajectory growth (ictg) model on a quasi-idealized simulation of a squall line.Journal of Advances in Modeling Earth Systems, 14(4):e2021MS002764, 2022. e2021MS002764 2021MS002764

  36. [36]

    Lewellen

    David C. Lewellen. A large-eddy simulation study of contrail ice number formation.Journal of the Atmospheric Sciences, 77(7):2585 – 2604, 2020

  37. [37]

    Jinhua Li, Jung-Hoon Kim, Banavar Sridhar, and Hok K. Ng. Ames contrail simulation model: Modeling aviation induced contrails and the computation of contrail radiative forcing using air traffic data.NASA Technical Memorandum, (NASA/TM–202300014633), December 2023

  38. [38]

    Libbrecht

    K. Libbrecht. Growth rates of the principal facets of ice between 210°c and 240°c. Journal of Crystal Growth, 247:530–540, 2003

  39. [39]

    Magee, A

    N. Magee, A. Miller, M. Amaral, and A. Cumiskey. Mesoscopic surface roughness of ice crystals pervasive across a wide range of ice crystal conditions.Atmospheric Chemistry and Physics, 14:12357–12371, 2014

  40. [40]

    Comparing Two Contrail Models Under Certain and Uncertain Inputs

    Caleb Akhtar Martinez and Jerome Jarrett. Comparing Two Contrail Models Under Certain and Uncertain Inputs

  41. [41]

    Numerical Simulation of contrail formation on the Common Research Model wing/body/engine configuration

    Emmanuel Montreuil, Weeded Ghedhaifi, Vivien Chmielaski, Francois Vuillot, Fabien Gand, and Adrien Loseille. Numerical Simulation of contrail formation on the Common Research Model wing/body/engine configuration

  42. [42]

    D. M. Murphy and T. Koop. Review of the vapour pressures of ice and supercooled water for atmospheric applications. Quarterly Journal of the Royal Meteorological Society, 131(608):1539–1565, 2005

  43. [43]

    Nelson and C

    J. Nelson and C. Knight. Snow crystal habit changes explained by layer nucleation.Journal of the Atmospheric Sciences, 55:1452–1465, 1998

  44. [44]

    J. T. Nelson and M. B. Baker. New theoretical framework for studies of vapor growth and sublimation of small ice crystals in the atmosphere.Journal of Geophysical Research: Atmospheres, 101(D3):7033–7047, 1996

  45. [45]

    Turbulence effects on the settling of suspended particles.Journal of Sedimentary Petrology, 63(5):835–838, 1993

    Peter Nielsen. Turbulence effects on the settling of suspended particles.Journal of Sedimentary Petrology, 63(5):835–838, 1993

  46. [46]

    Contrail modeling and simulation.Annual Review of Fluid Mechanics, 48(Volume 48, 2016):393–427, 2016

    Roberto Paoli and Karim Shariff. Contrail modeling and simulation.Annual Review of Fluid Mechanics, 48(Volume 48, 2016):393–427, 2016. 30

  47. [47]

    Pruppacher and James D

    Hans R. Pruppacher and James D. Klett.Microphysics of Clouds and Precipitation. Kluwer Academic Publishers, Dordrecht, Netherlands, 2nd edition, 1997

  48. [48]

    Ramkrishna

    D. Ramkrishna. Population Balances: Theory and Applications to Particulate Systems in Engineering. Academic Press, 2000

  49. [49]

    Schumann

    U. Schumann. A contrail cirrus prediction model.Geoscientific Model Development, 5(3):543–580, 2012

  50. [50]

    Schumann, P

    U. Schumann, P. Konopka, R. Baumann, R. Busen, T. Gerz, T. Schlager, P. Schulte, and H. Volkert. Estimate of diffusion parameters of aircraft exhaust plumes near the tropopause from nitric oxide and turbulence measurements.Journal of Geophysical Research, 100(D7):147–162, 1995

  51. [51]

    Bedka, David P

    Ulrich Schumann, Robert Baumann, Darrel Baumgardner, Sarah T. Bedka, David P. Duda, Volker Freudenthaler, Jean-François Gayet, Andrew J. Heymsfield, Patrick Minnis, Markus Quante, Ehrhard Raschke, Hans Schlager, Margarita Vázquez-Navarro, Christiane Voigt, and Zhien Wang. Properties of individual contrails: a compilation of observations and some compariso...

  52. [52]

    J. H. Seinfeld and Spyros N. Pandis.Atmospheric Chemistry and Physics: From Air Pollution to Climate Change. John Wiley & Sons, 2006

  53. [53]

    J. E. Stout, S. P. Arya, and E. L. Genikhovich. The effect of nonlinear drag on the motion and settling velocity of heavy particles in a turbulent atmosphere.Journal of the Atmospheric Sciences, 52(22):3836–3848, 1995

  54. [54]

    Contrail formation and persistence in the atmosphere

    Håkan Sundqvist. Contrail formation and persistence in the atmosphere. Journal of Atmospheric Sciences, 60(4):123–133, 2003

  55. [55]

    Optical properties of contrail-induced cirrus: discussion of unusual halo phenomena

    Ralf Sussmann. Optical properties of contrail-induced cirrus: discussion of unusual halo phenomena. Appl. Opt., 36(18):4195–4201, Jun 1997

  56. [56]

    Unterstrasser and K

    S. Unterstrasser and K. Gierens. Numerical simulations of contrail-to-cirrus transition – part 1: An extensive parametric study.Atmospheric Chemistry and Physics, 10(4):2017–2036, 2010

  57. [57]

    Unterstrasser and K

    S. Unterstrasser and K. Gierens. Numerical simulations of contrail-to-cirrus transition – part 2: Impact of initial ice crystal number, radiation, stratification, secondary nucleation and layer depth.Atmospheric Chemistry and Physics, 10(4):2037–2051, 2010

  58. [58]

    Numerical simulations of homoge- neously nucleated natural cirrus and contrail-cirrus

    Simon Unterstrasser, Klaus Gierens, Ingo Sölch, and Martin Lainer. Numerical simulations of homoge- neously nucleated natural cirrus and contrail-cirrus. part 1: How different are they?Meteorologische Zeitschrift, 26(6):621–642, 2017. Published online 14 October 2016; print issue 8 December 2017

  59. [59]

    Numerical simulations of homoge- neously nucleated natural cirrus and contrail-cirrus

    Simon Unterstrasser, Klaus Gierens, Ingo Sölch, and Martin Wirth. Numerical simulations of homoge- neously nucleated natural cirrus and contrail-cirrus. part 2: Interaction on local scale.Meteorologische Zeitschrift, 26(6):643–661, 2017. Published online 14 October 2016; print issue 8 December 2017

  60. [60]

    K. Wolf, N. Bellouin, and O. Boucher. Radiative effect by cirrus cloud and contrails – a comprehensive sensitivity study.EGUsphere [preprint], 2023

  61. [61]

    M. Xu. Development and Evaluation of Contrail Models. PhD thesis, Massachusetts Institute of Technology, 2024. 31

  62. [62]

    M. Xu, V. Meijer, S. R. H. Barrett, and S. D. Eastham. Evaluation of the apcemm intermediate-fidelity contrail model using lidar observations. Presented at the American Geophysical Union (AGU) Fall Meeting, 2023. Board 2426

  63. [63]

    Dessler, Szu-cheng Steve Ou, Kuo-Nan Liou, Patrick Minnis, and Harshvardhan

    Ping Yang, Gang Hong, Andrew E. Dessler, Szu-cheng Steve Ou, Kuo-Nan Liou, Patrick Minnis, and Harshvardhan. Contrails and induced cirrus: Optics and radiation. Bulletin of the American Meteorological Society, 91(4):473–478, 2010

  64. [64]

    Harrington

    Chengzhu Zhang and Jerry Y. Harrington. Including surface kinetic effects in simple models of ice vapor diffusion. Journal of the Atmospheric Sciences, 71(1):372 – 390, 2014. 8 Appendix A Composite Wind Field Construction • Uniform flow: the potential associated with a uniform flow is given byΦ (u)(x,y ) =U∞x +V∞y, from which we obtain the velocity field ...