the Creative Commons Attribution 4.0 License.
the Creative Commons Attribution 4.0 License.
A New Method for Estimating Atmospheric Turbulence from Global High-Resolution Radiosonde Data and Comparison with the Thorpe Method
Abstract. This study proposes a new method for estimating atmospheric turbulence from high vertical-resolution radiosonde data (HVRRD) using the minimum Richardson number (Rimin). While previous studies using HVRRD have primarily been based on the Thorpe method, which detects turbulence only in regions of local potential temperature overturning (Ri < 0) and does not explicitly account for wind shear, the proposed approach overcomes these limitations. By incorporating the effects of gravity waves on the static stability and vertical wind shear, this method enables the detection of turbulence not only in regions of Ri < 0 but also within statically stable layers characterized by strong shear (0 < Ri < 0.25), where Kelvin–Helmholtz instability is likely to occur. Additionally, comparison with turbulence observations from commercial flights demonstrates that the time series of turbulence derived from the Rimin method exhibits a significantly higher positive correlation with flight observations than that derived from the Thorpe method. Utilizing 10 years of global operational HVRRD, this study further analyzed the climatological distributions of turbulence derived from the Rimin method. Results show that turbulence under positive Ri conditions occurs most frequently in winter and less frequently in summer, reflecting the seasonal variability of the jet stream. In contrast, negative Ri cases exhibit a summertime maximum and wintertime minimum in the troposphere, and the opposite seasonal variation in the stratosphere. Regionally, turbulence is most pronounced over Asia, South America, and Antarctica for both positive and negative Ri cases. We upload the datasets produced from the current work at publicly available sites: https://doi.org/10.5281/zenodo.16899801 (Ko and Chun, 2025a), https://doi.org/10.5281/zenodo.16899803 (Ko and Chun, 2025b), https://doi.org/10.5281/zenodo.16899805 (Ko and Chun, 2025c), https://doi.org/10.5281/zenodo.16810246 (Ko and Chun, 2025d), and https://doi.org/10.5281/zenodo.16899789 (Ko and Chun, 2025e).
- Preprint
(2176 KB) - Metadata XML
-
Supplement
(1570 KB) - BibTeX
- EndNote
Status: final response (author comments only)
-
RC1: 'Comment on essd-2025-485', Anonymous Referee #1, 02 Dec 2025
- AC1: 'Reply on RC1', Han-Chang Ko, 20 Feb 2026
-
RC2: 'Comment on essd-2025-485', Anonymous Referee #2, 31 Jan 2026
Overall, I find the manuscript and the resulting dataset highly innovative and valuable for both turbulence research and aviation applications.
- Please correct the apparent typo “Using 10 years (2015–2015)” to “2015–2024” in the Conclusions.
- You apply a 60 m-scale moving average (13-point for 1-s; 7-point for 2-s) to multiple variables. Please specify (i) whether the filter is centered, (ii) how end points are handled, and (iii) the effective vertical span after interpolation (since 13×5 m and 7×10 m are slightly >60 m).
- Because all reported layers must be ≥60 m, the method will systematically exclude thin shear layers. Please add a short sensitivity test (e.g., 40/60/80 m) or at least report the fraction of candidate layers removed by this constraint.
- You interpolate 1- and 2-s data to fixed 5- and 10-m spacing. Please state explicitly which coordinate is used for interpolation (geopotential height vs geometric height), and whether pressure is interpolated or recomputed consistently.
- You note that manufacturer smoothing algorithms are proprietary and vary by instrument, and that processed temperature fluctuations may differ substantially from raw data. Please add (i) a brief statement of how this impacts Ri-based detection and ε, and (ii) if possible, the radiosonde types/IDs used (or at least a summary by instrument family) to help users assess heterogeneity.
- The choice of Ri_min < 0.25 is motivated as “stricter” given 5–10 m data. Please add one or two sentences clarifying what changes if a more common threshold (e.g., Ri<1) were used, or provide a brief sensitivity.
- You define a turbulence layer as a vertical segment where Ri consistently remains below 0.25 and take its thickness as L. Please clarify how “consistently” is implemented in practice (e.g., do you allow 1–2-point gaps above 0.25; minimum number of consecutive levels).
- Since EE has physical units and you present log10EE, please clarify the convention (e.g., log10(EE / 1 m² s⁻³)) to avoid ambiguity about taking logs of unitful quantities. Also, please restate Z clearly when switching between figures (troposphere/stratosphere depth vs fixed 1 km).
- Please ensure consistent notation and units formatting throughout (Ri_min, ε, EE; superscripts; “UTLS” definition on first use; consistent use of “turbulence layer” vs “turbulent layer”).
Citation: https://doi.org/10.5194/essd-2025-485-RC2 - AC2: 'Reply on RC2', Han-Chang Ko, 20 Feb 2026
Data sets
High vertical-resolution radiosonde data (HVRRD) National Centers for Environmental Information (NCEI) https://www.ncei.noaa.gov/data/ecmwf-global-upper-air-bufr/
In-situ flight EDR data National Oceanic and Atmospheric Administration (NOAA)'s Meteorological Assimilation Data Ingest System (MADIS) https://madis-data.cprk.ncep.noaa.gov/madisPublic1/data/archive/
Viewed
| HTML | XML | Total | Supplement | BibTeX | EndNote | |
|---|---|---|---|---|---|---|
| 381 | 138 | 37 | 556 | 66 | 32 | 58 |
- HTML: 381
- PDF: 138
- XML: 37
- Total: 556
- Supplement: 66
- BibTeX: 32
- EndNote: 58
Viewed (geographical distribution)
| Country | # | Views | % |
|---|
| Total: | 0 |
| HTML: | 0 |
| PDF: | 0 |
| XML: | 0 |
- 1
Review comments to the manuscript, entitled “A New Method for Estimating Atmospheric Turbulence from Global High-Resolution Radiosonde Data and Comparison with the Thorpe Method" (essd-2025-485).
< Overview >
This paper has a potential of significant and timely contribution that effectively leverages high vertical-resolution radiosonde data (HVRRD) to create a unique global turbulence dataset. The proposed Ri_min method correctly addresses the limitations of the Thorpe method by including turbulence detection in statically stable, strong shear layers (0 < Ri < 0.25). The paper is well-written and the core methodology is sound, satisfying the main scientific requirements for publication in Earth System Science Data (ESSD). I recommend a Minor Revision to address documentation clarity, data usability, and minor scientific detail, ensuring the dataset meets the high standards of long-term data archiving.
< Minor Comments >
Here are five specific comments that require minor revisions:
1. Justification of Two Practical Considerations
While the methodology for deriving EDR from Ri_min is detailed, two practical considerations of using L and VWS instead of Def need to be justified more clearly.
- The authors mentioned that the Thorpe method has a limitation to explicitly consider convectively unstable condition (Ri < 0), which could have a relatively large mixing length (convective overturning of wave or turbulent eddy). But, shear driven KHI is very intermittent, which would have a small mixing length (small-scale eddy). So, it might be necessary to justify more specifically why the authors adapted the length scale from Thorpe method here?
- The authors substitute the def in Eq. (8) by VWS based on simple synoptic-scale analysis, which would make sense in some part. But, it would not be applicable in a case where strong VWS in anticyclonic shear and curvature jet stream (e.g., Knox 1997). Given the simple assumption that the cyclonic and anticyclonic jet streams are equally happening in mid-latitude, anticyclonic curvature jet stream is theoretically stronger than cyclonic jet based on the gradient wind balance. I think the authors need to more carefully justify (or provide some limitations of current method) using VWS instead of DEF in this study.
2. Illustrative Case Study for 0 < Ri < 0.25 Turbulence vs in situ EDR near jet stream
The core scientific advancement of this work is the ability of the Ri_min method to detect turbulence in the statically stable, high-shear region (0 < Ri < 0.25) where the Thorpe method fails. This claim, while theoretically sound, needs compelling direct comparison of Ri_min method with in situ EDR obs. I know it is difficult to find a case that has collocated pairs of HVSSD and in situ EDR. Considering that jet stream is synoptic scale, it will be great to find a CAT outbreak day (last 1-2 days) near jet stream to be captured by both HVRRD and in situ EDR. Then, it will be more convincing that this new method really show a good performance for KHI near upper-level jet system.
3. Explicit Declaration of Data Output Format and Internal Structure
For publication in ESSD, data usability is paramount. The manuscript must explicitly declare the chosen long-term archiving data format and its internal structure for user accessibility. Please state the definitive file format (e.g., NetCDF, HDF5, or another community standard) that will be used for the final dataset. More importantly, provide a clear, dedicated table listing all variable names (e.g., turbulence_edr), their units (e.g., m^2/3 s^-1), and the corresponding CF-compliant metadata for each variable provided in the data files.
4. Clearer Statement on Spatio-Temporal Data Heterogeneity
The dataset is unique because it is global, but its temporal and horizontal resolution is fundamentally constrained by the heterogeneous global radiosonde network (typically 00/12 UTC, geographically sparse). The current description emphasizes the high vertical resolution but downplays the horizontal and temporal sparseness of the overall product. A single sentence or footnote in the Abstract or Data Description section must clearly state that the dataset's spatial and temporal coverage reflects the limitations and heterogeneity of the operational global radiosonde observing network.
5. Final Archival Repository and Versioning Commitment
ESSD requires a strong commitment to long-term data preservation and traceability. Please specify the exact permanent digital repository (e.g., a recognized data center like NOAA NCEI, EUMETSAT, or a major institutional repository with DOIs) where the final dataset will be lodged. Furthermore, provide a clear statement regarding the versioning scheme (e.g., "The dataset presented here will be designated Version 1.0 (v1.0). All future updates will be released as incremental versions, v1.1, v2.0, etc., with associated Digital Object Identifiers (DOIs).").