Project based at
Leibniz Institute for Tropospheric Research (TROPOS), Phase 2
TROPOS (Observations): Kevin Ohneiser (PostDoc) and Patric Seifert (PI)
TROPOS (Simulations): Willi Schimmel (PostDoc) and Fabian Senf (PI)
The project PolarCAP aims to uncover the complex entanglement of aerosol- and cloud-microphysical processes by exploring the evolution of the ice phase at slightly supercooled conditions of $T > -10\,°\text{C}$ in a thermodynamically and aerosol-controlled natural environment using radar polarimetry and spectral-bin modelling.
PolarCAP collaborates with the ERC research project CLOUDLAB of ETH Zurich to investigate the evolution of the artificially triggered ice phase in supercooled stratus layers (see Fig. 1). Thereby, CLOUDLAB applies cloud seeding with silver iodide to initialize the freezing of cloud droplets, whose evolution is then monitored by means of in-situ measurements of drones and the unique holographic cloud-hydrometeor in-situ sensor HOLIMO, as well as by means of standard ground-based cloud remote sensing instrumentation.
In the framework of the collaboration between PolarCAP and CLOUDLAB, a unique data set will be produced and analyzed that includes polarimetric radar and lidar observations from the Leipzig Aerosol and Cloud Remote Observing System (LACROS) as well as data from the cloud-resolving spectral bin model COSMO-SPECS. PolarCAP will benefit strongly from the available cloud in-situ measurements. Progress will be achieved in the ability to constrain the efficiency of different ice nucleating substances, to link the time scales of microphysical processes and stratus dissipation, and to evaluate and develop remote-sensing-based retrievals for cloud properties.
Figure 1: Layout of the PolarCAP project, with the main instrumentation of TROPOS (LACROS, COSMO-SPECS) and ETH Zurich indicated.
Two winter campaigns with the mobile exploratory platform LACROS of TROPOS in 2022/23 and 2023/24 were conducted near Eriswil in the center of Switzerland. For more information, also about the experimental setup and the comparison with model data, click on “Status Summer 2024”.
One of the highlights of the campaign was the measurement of a seeder-feeder cloud system. The seeder-feeder case study is utilized to study how natural seeding (with ice crystals) into a lower supercooled liquid cloud affects precipitation formation and cloud properties. The knowledge gained in this study is not only useful for the region of Eriswil. As seeder-feeder interactions are frequent phenomena worldwide, it can help to improve weather models and weather forecasts worldwide. It turned out that the seeder-feeder process is misrepresented in weather models. The conditions were ideal for applying state-of-the-art remote-sensing and in-situ retrieval techniques and evaluating their consistency.
Figure 1: Schematic overview of the instruments and methods and the physical process derived from these methods. In brackets the required measurement device is highlighted.
Figure 1 gives an overview of the applied retrievals. The applied approaches of the fall streak tracking algorithm, VOODOO (reVealing supercOOled liquiD beyOnd lidar attenuatiOn), dual-wavelength ratio (DWR), Eddy dissipation rate (EDR), peakTree (Doppler-peak-separation algorithm), ice crystal shape retrieval (Vertical Distribution of Particle Shape, VDPS), riming retrievals, and ice crystal number concentration (ICNC) retrievals are shown. In addition, model results of HYSPLIT (Hybrid Single-Particle Lagrangian Integrated Trajectory) and ICON-D2 are used. Each of the mentioned retrievals contributes to a better understanding of the microphysical processes within the cloud. All retrievals together give a clear picture on the ice crystal habits and the changes in ice crystal properties along their way through the cloud. The results of this study are shown in Ohneiser et al., 2025a[1].
Another highlight of the campaign was the measurement of ice-nucleating particles in Eriswil (Eri, coordinates: $47.07°\text{N}, 7.87°\text{E}$, $921\text{m}$ a.s.l.) and Hohenpeißenberg (HPB, coordinates: $47.80°\text{N}, 11.01°\text{E}$, $945\text{m}$ a.s.l.). The results are shown in Fig. 2. First, during the warm-Bise period, the INP population was found to be similar at Eri and HPB, no matter if a Bise cloud was present or not. Second, during cold-Bise, no INP contrast was found when both HPB and Eri were within or below the cold-Bise cloud and thus within the planetary boundary layer (PBL). Nevertheless, the INP concentration was overall found to be much lower than during the warm-Bise situations. Third, when the HPB site was located in the free troposphere during a cold-Bise situation, INP concentrations were also much higher compared to Eri that was still within the PBL. These observations led to the conclusion that during cold-Bise situations the INP reservoir is depleted. The inversion-capped winterly PBL is apparently not capable to replenish the INP reservoir. As remote-sensing and in-situ measurements at Eri revealed, the concentration of pristine ice crystals was higher than the available INP concentration. It is thus likely that a fraction of the ice crystals is formed by INP that were entrained from the free-troposphere into the Bise cloud, or alternatively that secondary ice formation mechanisms were active. The results of this study are shown in Ohneiser et al., 2025b[2].
Figure 2: INP conc. activated in air for the temperature range $0$ to $-30°\text{C}$, $a+b+c$) both in cold Bise (cloud top temperatures below $0°\text{C}$), $d+e+f$) Eri in cold Bise, HPB directly above Bise cloud in the free troposphere, $g+h+i$) Both in warm Bise situation.
We continue with an update on the modelling aspect of the cloud seeding missions, conducted by CLOUDLAB over the last three winter seasons. A significantly more efficient immersion freezing parameterization[3] specifically designed for silver iodide (AgI) particles was implemented into the COSMO-SPECS model, which is based on an exponential fit to laboratory measurements[4], of the temperature dependent freezing fraction.
Figure 3 provides a composition of remote-sensing (radar), in-situ (HOLIMO; holographic imager) and model data (COSMO-SPECS 5D output) from the 25 January, 2023 in Eriswil, Switzerland, which was introduced in the last blog-post. Panel (a) shows the radar reflectivity factor $Z_e$ of MBR7, a $35\,\text{GHz}$ Doppler cloud radar shows three distinct enhancements in the radar signal of $10$ – $25\,\text{dBZ}$ above the (supercooled liquid) background cloud, which were induced by three cloud seeding missions. The black linen shows the altitude where (in-cloud) in-situ observations were collected, providing liquid droplet and ice crystal PSDs.
A large variety of ensemble simulations were conducted to optimize the set of model parameters to match the observations from the holographic imager (HOLIMO) best. We can confirm, that the DeMott parameterization[5] (which is the default) leads to a need to release an exaggerated amount of flare particles to produce comparable INP values to the observations. However, the Omanovic freezing, requires much more realistic values, reducing the flare particle rate by $10^5$. For visual comparison of cloud radar and the model, the liquid and ice water contents (panel b), are plotted below, which shows good agreement in macrophysical parameters (cloud base/top height). Depending on the choice of model parameters, COSMO-SPECS is able to replicate the seeding events in terms of (liquid and ice particle) number concentration and contents well. For CDNC $(c)$, the deviation ranges from factor $3$ $(=300%)$, down to $10%$ error, same holds for ICNC $(d)$. In panels $(e)$ and $(f)$ we compare the model ensembles PSD of liquid and ice particles to the in-situ observations. The liquid particle spectra $(e)$ show deviations up to a factor of $12$, where the error in mean droplet diameters ranges from $5%$ to $20%$. COSMO-SPECS closely matches the observations of the frozen particle spectra, with a deviation of $<10%$ and number concentrations by $<30%$. Still, the narrow ice peak in the model spectra leaves more room for investigations of COSMO-SPECS. In a next step, the model PSDs are forward simulated using the Passive and Active Microwave radiative TRAnsfer tool (PAMTRA), to compute the corresponding “virtual” radar reflectivity factor $\tilde{Z}_e$. Preliminary results with deviations ($|Z_e-\tilde{Z}_e|$) up to $10\,\text{dBZ}$ indicate that there is still potential to improve the PAMTRA configuration to better align the forward model setup with actual observed hydrometeor type descriptions.
Figure 3: Composite of $(a)$ cloud radar reflectivity factor and $(b)$ liquid water content overlayed with ice water content of a COSMO-SPECS run on $400\,\text{m}$ horizontal resolution. Panels $(c)$ and $(d)$ show the cloud droplet and ice crystal number concentration of ensemble simulations, varying in flare particle emission and initial CCN and INP values. Panels $(e)$ and $(f)$ provide the mean particle size distribution of liquid and frozen hydrometeors for the time frame marked by the red dashed lines. Black lines in panels $(a)$ and $(b)$ indicate the height of the holographic imager over time.
References
In winter 2022/23 and 2023/24, the mobile exploratory platform LACROS of TROPOS was part of a series of winter campaigns near Eriswil in the centre of Switzerland. LACROS joint the two 3-months campaigns, which were conducted under the umbrella of the ERC research project CLOUDLAB of ETH Zurich, in the framework of the PolarCAP (Polarimetric Radar Signatures of Ice Formation Pathways from Controlled Aerosol Perturbations) project.
The CLOUDLAB campaign jointly brought together a unique set of ground-based and airborne in-situ cloud and precipitation sensors and remote sensing instruments. During the campaigns, LACROS was on site with a large number of remote sensing equipment. In winter 2022/23, among other instruments, a scanning 35-GHz and vertical-pointing 94GHz cloud radar, as well as the 35-GHz scanning cloud radar of ETH Zurich were on site.
During the campaign 2023/24 two more cooperations took place. The PROM project CORSIPP of LIM (Leipzig Institute for Meteorology) joined the campaign in Eriswil with their scanning 94GHz polarimetric cloud radar. In addition, EPFL (École Polytechnique Fédérale de Lausanne) joined the campaign with a scanning polarimetric X-band radar. In the end, the campaign was one of the largest joint deployments of multi-wavelength radar and lidar systems. An overview of the campaign can be seen in Figure 1. An additional side project of TROPOS and the Hohenpeißenberg Meteorological Observatory of the German Weather Service (DWD) dealt with the characterization of the aerosol conditions during the supercooled stratus cloud events. Aerosol in-situ samplers were installed at Hohenpeißenberg observatory and Eirswil to characterize potential contrasts in the concentration of ice nucleating particles (INP) between the two sites. The analysis of these datasets (2 weeks of samples were taken) is ongoing in 2024.
Figure 2: Temporal evolution of the ice crystal number concentration of COSMO-SPECS Run2 with artificial seeding at 10:52:00 UTC. The ruler shows the distance of the plume over time, with marks units of km. The x shows the location of the observational site.
Figure 3: 35-GHz cloud radar observations from 25 January 2023. Upper panel shows the radar reflectivity factor, the lower panel shows the linear depolarization ratio. Red dashed line corresponds to the seeding height within the COMSO-SPECS simulations.
Figure 3 illustrates a time-height cross-section, of the 35-GHz radar reflectivity factor and linear depolarization ratio from 10:30 to 11:40 UTC on the corresponding day as the simulations. The occurrence of the plume event above the radar at 11:02 UTC closely aligns with the simulations. Next steps involve the evaluation of this event through a comprehensive model-observation comparison. This step aims to investigate deeper into the characteristics and dynamics of the observed phenomenon, enhancing our understanding through analysis and validation against simulated data.