Articles | Volume 20, issue 8
https://doi.org/10.5194/tc-20-4367-2026
© Author(s) 2026. This work is distributed under the Creative Commons Attribution 4.0 License.
Mapping snow on northern winter roads: a dual-frequency polarimetric radar approach for snow characterization over land, lake and sea ice
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- Final revised paper (published on 12 Aug 2026)
- Preprint (discussion started on 10 Feb 2026)
Interactive discussion
Status: closed
Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor
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RC1: 'Comment on egusphere-2026-212', Anonymous Referee #1, 25 Feb 2026
- AC1: 'Reply on RC1', Julienne Stroeve, 08 Apr 2026
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RC2: 'Comment on egusphere-2026-212', Anonymous Referee #2, 27 Feb 2026
- AC2: 'Reply on RC2', Julienne Stroeve, 08 Apr 2026
Peer review completion
AR – Author's response | RR – Referee report | ED – Editor decision | EF – Editorial file upload
ED: Publish subject to revisions (further review by editor and referees) (21 Apr 2026) by Qinghua Yang
AR by Julienne Stroeve on behalf of the Authors (07 May 2026)
Author's response
Author's tracked changes
EF by Polina Shvedko (26 May 2026)
Manuscript
ED: Referee Nomination & Report Request started (27 May 2026) by Qinghua Yang
RR by Anonymous Referee #3 (21 Jun 2026)
RR by Anonymous Referee #2 (22 Jun 2026)
ED: Publish subject to minor revisions (review by editor) (23 Jun 2026) by Qinghua Yang
AR by Julienne Stroeve on behalf of the Authors (24 Jun 2026)
Author's response
Author's tracked changes
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ED: Publish as is (25 Jun 2026) by Qinghua Yang
AR by Julienne Stroeve on behalf of the Authors (03 Jul 2026)
Manuscript
Review of “Mapping Snow on Northern Winter Roads: A Dual-Frequency Polarimetric Radar Approach for Snow Characterization over Land, Lake and Sea ice” by Julienne Stroeve et al.
The study is comparing different snow depth mapping methods (also described in Willatt et al., 2023…) with the on-ice KuKa radar to magnaprobe measurements over different terrain used for winter roads in Canada (lake ice, sea ice, muskeg). The results are in line with earlier KuKa results on sea ice that the Ku VH-HH peak provides the best snow depth estimates while the Ku – Ka peak or centroid method does not demonstrate much skill. This finding is obviously concerning when the upcoming CRISTAL snow depth product is based on the Ku – Ka method and it is also interesting to imagine what the studies mentioned in the introduction have derived, using the same method with ALTIKA and CRYOSAT data. There are differences between radar measurements from KuKa and satellite, as also mentioned, but one thing that they have in common is the signal attenuation in the snow layer. This KuKa to satellite discussion could be strengthened. Unfortunately, there are no committed future satellite polarimetric altimeters.
The MS is well written and structured but the analysis could be improved and I have some suggestions below. I think that some parts of the discussion could be strengthened and substantiated by including the measured values in Table 3 and computing the reflectivity and penetration depth and potentially scattering, absorption etc.
In addition, I have a number of specific comments:
The abstract should be detailed with main results.
There are some differences and similarities between on-ice and satellite altimeter measurements which should be emphasized in the introduction and strengthened in the last part of the discussion.
Sometimes the discussion is really confusing and I give examples below. I would suggest a conceptual model for what happens with snow - radar interaction to illustrate the main principles. What are the snow/ ice parameters affecting the radar backscatter? And how?
The in-situ measurements have uncertainties, the derived snow depths have uncertainties. Please include a discussion and a quantification of the uncertainties.
L114: please write in the text if Churchill is sea ice or something else. The same for the other sites.
Figure 4: all these parameters could contribute to the uncertainty, I suggest to use them in the analysis for comparing the different sites and for computing reflectivity and penetration depth.
L158: the snow density in Eq. 1 is in [g/cm3]. Please specify that. Otherwise you are using [kg/m3].
L161: The sentence is unclear, please clarify. The “liquid water” which is, I think, brine, is affecting the loss (penetration depth?), but according to Eq. 1 the “wave speed” (speed of light?) is only a function of snow density. Please use the terms consistently (e.g. “liquid water” -> “brine”) and substantiate your statements with references or by computing the “loss”, “Wave speed/ speed of light” with models.
L165: “…we assume c’ values range from 0.77…”: The c’ value is computed using Eq. 1, write that instead of “assume”. The speed of light in snow is not 0.77, it is 0.77 times the speed of light in a vacuum (as written in line 158). Please clarify.
Figures 7 and 8 it is not totally clear what “Range” means. Is it the two-way travel time times the speed of light in a vacuum? Please clarify. Also could you reference these plots to the snow and ice surface? It is very difficult to see if it is a track-point misalignment or an actual variation in the snow and ice surface height. Please also write the average snow and ice thickness in the figure caption.
Figure 7: Judging from the “range” you do not get returns from deep within sea ice. Please clarify. Is it because of sidelobes or other off-nadir returns?
L265: I would suggest to replace “volume scattering” with “rough surface scattering”.
L333: This explanation is confusing. According to Eq. 1 there is no permittivity contrast between Ku- and Ka-band and if there is difference in the air/snow surface scattering then it is the wavelength dependent roughness. Both frequencies scatter at the snow surface but there may be differences in snow penetration at Ku- and Ka-band and how much reaches the snow ice interface (and back). Please clarify.
Table 3 is nice and I would even suggest to include penetration depth and Fresnel reflection coefficient as columns. However, the permittivity is not consistent with Eq. 1. I think that you could even achieve better results if you use the Table 3 permittivity for computing the speed of light in snow (Eq. 1). In any case there should be consistency between Eq. 1 and the permittivity in Table 3.
Table 3: how is the salinity computed/ measured? Density cutter-> bagged sample-> melted->salinity measured->multiplied by the density ratio?
L361: I think that this sentence is misleading. Depolarization is also happening in dry snow, so I am skeptical if it depends on brine pocket scattering. Loss is the sum of absorption (brine) and scattering (snow grains). Please define the “Mie-regime”. What is “rapid depolarization”? Please reformulate these two sentences and substantiate the statements.
L367: Compute the Fresnel reflection coefficient in Table 3 to make a substantiated assessment of the “initial reflection”. According to Eq. 1, the permittivity is only a function of snow density.
L374: why would compacted snow be “high extinction”? Please clarify and define the term extinction here.
L417: I agree that KuKa is not sensitive to large scale surface roughness in the same way as satellite altimeters. However, KuKa is still sensitive to surface roughness. Please clarify and describe what KuKa is sensitive to.
Figure 17. Are there any measurements of ice thickness and can this be used to derive the effective permittivity of the ice… or snow?