Evaluation of simulated cloud liquid water in low clouds over the Beaufort Sea in the Arctic System Reanalysis using ARISE airborne in situ observations
- 1Science Systems and Applications, Inc., Hampton, VA 23666, USA
- 2NASA Langley Research Center, Climate Science Branch, Hampton, VA 23681-2199, USA
- 3NASA Langley Research Center, Atmospheric Composition Branch, Hampton, VA 23681-2199, USA
- 4NASA Langley Research Center, Chemistry and Dynamics Branch, Hampton, VA 23681-2199, USA
- 5Polar Meteorology Group, Byrd Polar and Climate Research Center, The Ohio State University, Columbus, Ohio 43210, USA
- 6Department of Biology/Chemistry, Springfield College, Springfield, MA 01109, USA
- 7National Suborbital Research Center, NASA AMES Research Center, Moffett Field, CA 94035-0001, USA
Correspondence: Jason Brant Dodson (email@example.com)
Arctic low clouds and the water they contain influence the evolution of the Arctic system through their effects on radiative fluxes, boundary layer mixing, stability, turbulence, humidity, and precipitation. Atmospheric models struggle to accurately simulate the occurrence and properties of Arctic low clouds, stemming from errors in both the simulated atmospheric state and the dependence of cloud properties on the atmospheric state. Knowledge of the contributions from these two factors to the model errors allows for the isolation of the process contributions to the model–observation differences. We analyze the differences between the Arctic System Reanalysis version 2 (ASR) and data taken during the September 2014 Arctic Radiation–IceBridge Sea and Ice Experiment (ARISE) airborne campaign conducted over the Beaufort Sea. The results show that ASR produces less total and liquid cloud water than observed along the flight track and is unable to simulate observed large in-cloud water content. Contributing to this bias, ASR is warmer by nearly 1.5 K and drier by 0.06 g kg−1 (relative humidity 4.3 % lower) than observed. Moreover, ASR produces cloud water over a much narrower range of thermodynamic conditions than shown in ARISE observations. Analyzing the ARISE–ASR differences by thermodynamic conditions, our results indicate that the differences are primarily attributed to disagreements in the cloud–thermodynamic relationships and secondarily (but importantly) to differences in the occurrence frequency of thermodynamic regimes. The ratio of the factors is about to . Substantial sampling uncertainties are found within low-likelihood atmospheric regimes; sampling noise cannot be ruled out as a cause of observation–model differences, despite large differences. Thus, an important lesson from this analysis is that when comparing in situ airborne data and model output, one should not restrict the comparison to flight-track-only model output.
The Arctic Ocean represents a critical component of the Arctic climate system. Moreover, the state and variability of the atmosphere, ocean, and sea ice in the central Arctic have significant implications for the climate across much of the planet (e.g., Deser et al., 2016). The complex interactions between surface properties, meteorological processes, and the surface energy budget are critical to understanding the climate of the Arctic Ocean and making projections of its response to anthropogenic climate change (e.g., Budyko, 1969; Manabe and Wetherald, 1975; Hall, 2004; Boeke and Taylor, 2018; Dai et al., 2019). Clouds represent a key feature of the Arctic climate system and modulate important aspects of ice–atmosphere–ocean coupling processes that strongly influence the evolution of the Arctic Ocean climate (Curry et al., 1996).
The effects of clouds on the Arctic climate system span a wide range of physical processes, such as heating and cooling via cloud radiative effects (CREs), mixing of the boundary layer by generating turbulence, influencing humidity through precipitation, and altering boundary layer stability (Vihma et al., 2014). Through these processes, clouds shape long-term trends in both temperature and sea ice variability in the central Arctic, representing a potentially significant climate feedback. Cloud radiative feedbacks, in particular, remain a key uncertainty in the Arctic climate system (Curry et al., 1996; Wendisch et al., 2019).
Models differ strongly in their simulation of CREs (Karlsson and Svensson, 2011; English et al., 2015; Boeke and Taylor, 2016) and in their representation of the Arctic cloud annual cycle (Taylor et al., 2019). Systematic biases in CREs impact the representation of atmospheric circulation variability and the lifetime of atmospheric circulation regimes (Stramler et al., 2011; Pithan et al., 2014). Moreover, CREs influence sea ice anomalies during both melt and growth seasons (Kay et al., 2008; Hegyi and Taylor, 2018) and reduce shortwave downwelling radiation at the surface (Sledd and L'Ecuyer 2019; Alkama et al., 2020). Sledd and L'Ecuyer (2019) quantify the cloud masking effect on the sea ice albedo perturbation at the top of the atmosphere (TOA) to be ∼50 %. Moreover, Alkama et al. (2020) argue that accurate representation of present-day Arctic cloud properties is necessary for climate models to accurately reproduce the surface radiation budget impact of sea ice variability and change. Thus, accurate representation of Arctic cloud properties in atmospheric models is a necessary but insufficient condition to ensure accurate predictions of Arctic climate change. The understanding of the key processes that give rise to the mean and variability of cloud properties within atmospheric regimes is lacking; this knowledge is needed in order to understand the role of clouds in the atmospheric circulation, understand cloud feedback, and improve the simulations of clouds within models.
A process-oriented approach that moves beyond the analysis of monthly mean properties is required to identify and understand the processes that cause differences between observations and the model representation of clouds. Previous analyses have identified a range of errors in the model simulations at monthly or daily mean scales (e.g., Karlsson and Svensson, 2011; English et al., 2015; Boeke and Taylor, 2016). However, these approaches fail to unequivocally identify the processes responsible for the errors. Detailed observations of cloud properties and the meteorological environments are needed to identify errors in the simulation of Arctic clouds. However, these observations are difficult to obtain from satellites – cloud water retrievals from passive instruments are challenging (Shupe et al., 2005; Ehrlich et al., 2017; Chen et al., 2020), and the cloud presence limits the ability of sounding instruments to sample the thermodynamic properties of the underlying boundary layer. To fill these data gaps, aircraft field campaigns are necessary to collect the unavailable data in situ. One such campaign was the Arctic Radiation–IceBridge Sea and Ice Experiment (ARISE), conducted in the Beaufort Sea region during September 2014 (Smith et al., 2017). In this study, we take a process-oriented approach (e.g., Taylor et al., 2019) by investigating the dependence of in situ cloud properties on varying meteorological regimes, and we use these results to evaluate the Arctic System Reanalysis version 2 (ASR; Bromwich et al., 2018).
The main purpose of this paper is to document the properties of Arctic boundary layer clouds, their meteorological environments, and their relationships using ARISE observations and compare these results with ASR, a reanalysis specifically designed to represent Arctic weather and climate (Bromwich et al., 2018). Model–observation disagreements occur for at least three general reasons. First, the model may produce incorrect meteorological conditions, such as biases in the mean or variability of temperature or humidity. Second, the model may misrepresent the observed relationships between cloud and meteorological conditions. For example, the model may produce too much or too little cloud water at a given humidity value even when the humidity is similar to the observed value. Lastly, flight track sampling can limit the precision and range of conditions over which relationships between clouds and meteorological conditions can be determined. We assess the impact of the flight track to sampling on the ability to assess model realism using flight campaign data. Our analysis addresses three questions.
How do the cloud properties in ARISE and ASR compare?
Can discrepancies between ARISE and ASR be explained by grid-scale disagreements in meteorological conditions and/or errors in the simulated cloud–thermodynamic relationships?
How are ARISE–ASR comparisons affected by flight track sampling?
Section 2 discusses the observational and ASR datasets, as well as the analysis methodology. Section 3 examines flight track cloud properties observed from the aircraft and ASR output. Section 4 discusses the relationships between cloud properties and thermodynamic regimes in situ and in ASR. Section 5 presents the quantification of the effects of sampling, and Sect. 6 presents our conclusions.
2.1 The Arctic Radiation–IceBridge Sea and Ice Experiment
ARISE was conducted during September 2014 to investigate the radiative properties of the Arctic and the interconnections with meteorological conditions (Smith et al., 2017). Measurements of cloud properties, radiative fluxes, and other meteorological variables were carried out by a NASA Wallops Flight Facility C-130 aircraft based at Eielson Air Force Base near Fairbanks, AK. The observing region encompassed a portion of the Beaufort Sea north of Alaska (Fig. 1) that contained both sea ice and ice-free ocean. For flights used in this study, the aircraft typically entered and exited the observing region flying well above the boundary layer, then descended and spent most of the time below 1000 m adjusting its altitude to fly above, below, and within the cloud layer.
ARISE consisted of 16 total flights over the Beaufort Sea; however, only a subset of those are used in this study. For a flight to be included in the analysis, it must have collected cloud and thermodynamic property measurements below 1000 m of altitude for at least an hour. Eight flights met this requirement: 13, 15–19, 21, and 24 September. As an example, Fig. 1 shows the science flight and cloud probe data from 15 September 2014. Only aircraft observations taken over sea ice and ocean below 1000 m of altitude are shown to focus on properties of low clouds over the Arctic Ocean. Additionally, only observations that report thermodynamic and cloud microphysical variables simultaneously are included – cases in which one is missing are rare.
The measurements of interest include total cloud water (cloud liquid+cloud ice), air temperature, and humidity. Cloud water measurements were collected by the WCM-2000 probe (Smith et al., 2017; Fig. 1), which reports total and liquid water content; ice water content is derived as the difference. The WCM-2000 probe reports two liquid water content values obtained from wires of different diameter: 2.0 and 0.5 mm (with the former being used in this study). We convert these measurements to total cloud water (QC), cloud liquid (QL), and cloud ice (QI) specific humidity for comparison with ASR. Flight-level in situ static air temperature (T), relative humidity with respect to liquid (RH), and specific humidity of vapor (QV) are also used. The measurement uncertainties of the 1 Hz measurements are described in the source data files at 5 % (of the measured value) for QC, 0.5 ∘C for T, and 2 %–5 % (out of 100 % saturation) for RH. No value for QV is provided.
The WCM-2000 data are used in this study and represent the most “direct” measurements of QC, QL, and QI. As an additional check of the robustness of WCM-2000 measurements, cloud droplet volume concentration data from the aircraft-mounted Cloud Droplet Probe (CDP) are integrated to compute QC. Figure 2 shows that WCM-2000 detects about 30 % greater QC than the CDP, especially in clouds with large QC values. This holds true for QL values measured by both wire diameters. Overall, WCM-2000 QC agrees fairly well with the integrated CDP QC, with a substantial positive correlation (0.85). The LWC derived from the two different diameter wires also shows substantial correlation (0.95). Given this consistency, we proceed using QL determined from the 2.0 mm wire, as the larger diameter captures more liquid water.
Unfortunately, ARISE did not collect aerosol measurements. Such observations would be particularly valuable for the study of certain cloud properties such as albedo and droplet concentration (in line with Twomey, 1977). Measurements of ice-forming nuclei might also be helpful for understanding mixed-phase processes. But this study focuses on QC in predominantly liquid stratiform clouds, which is not as susceptible to aerosols (Ackerman et al., 2004; Christensen and Stephens, 2011), so the lack of aerosol data does not as greatly affect the results.
2.2 Arctic System Reanalysis version 2 (ASR)
The Arctic System Reanalysis is a regional reanalysis of the greater Arctic stretching from the headwaters of the major northward-flowing rivers to the North Pole and is targeted at producing a refined description of the Arctic environment during the current period of rapid change (Bromwich et al., 2016, 2018). It is based upon the polar version of the Weather Research and Forecasting model (known as Polar WRF; http://polarmet.osu.edu/PWRF/, last access: 8 July 2021) that features realistic heat transfer through snow and ice, comprehensive description of sea ice characteristics, and other improvements to the Noah Land Surface Model. The model physical parameterizations are chosen for Arctic conditions based upon extensive testing (e.g., Bromwich et al., 2009). In particular, the Goddard microphysics scheme (Tao and Simpson, 1993; Tao et al., 2003) is used to predict the cloud species studied here; this is now a dated scheme in light of the recent advances in microphysics research that have emphasized prediction of cloud liquid water at low air temperatures (e.g., Hines et al., 2019). ASR assimilates a wide variety of conventional meteorological observations as well as satellite-derived radiances and retrievals using three-dimensional data assimilation. Specified sea ice conditions, snow cover, and vegetation characteristics are updated either daily (sea ice) or weekly. ASR is produced every 3 h on 71 vertical model levels with 25 below 850 hPa to better resolve the highly stratified near-surface conditions often present in the Arctic. In contrast to version 1, ASR version 2 (NCAR, 2017) has higher spatial resolution (15 km) and implemented subgrid (convective) cloud fraction over land to improve the surface downward radiative fluxes. Recent investigations have demonstrated ASRv2 skill in capturing a variety of Arctic phenomena, such as snowfall over the Arctic Ocean (Edel et al., 2020) and polar lows (Stoll et al., 2018). Currently, ASRv2 spans 2000–2016, coinciding with the availability of the essential input datasets from MODIS, and is being updated through 2020. Importantly for the present comparison, no ARISE data were assimilated into ASRv2, so they are a completely independent test of the reanalysis. A new version (ASRv3) is being developed to deal with issues such as those explored here.
2.3 ARISE and ASR collocation methodology
ARISE is conformed to the ASR spatial grid and 3 h resolution as follows.
Each ARISE data point (one per second) collected at or below 1000 m of altitude is collocated with the center of the nearest ASR grid box.
Consecutive sets of ARISE data points within the same ASR grid box are then collocated with the nearest ASR vertical level.
Each consecutive set of ARISE data within the same grid box and altitude are averaged.
The median time of observation for each consecutive set is chosen to represent the entire set.
Each set of data points is collocated with the nearest ASR time step – flights lasting longer than 3 h and different flight segments are collocated with different time steps.
Collocating ARISE data with an ASR grid box allows the simulated values of cloud and thermodynamic properties to be directly compared, reducing the noise from high-frequency ARISE sampling (which would be subgrid-scale artifacts compared with the ASR grid). Organizing the ARISE and ASR data in this way allows an optimized comparison and minimizes the possible sampling effects.
3.1 Probability density functions of cloud and thermodynamic variables
An evaluation of ASR-simulated Arctic thermodynamic and cloud properties is performed by comparing the probability density functions (PDFs) of QC and thermodynamic variables. These variables are divided into discrete thermodynamic regimes separated by 5 ∘C in T, 1 g kg−1 in QV, and 10 % in RH. Figure 3 shows PDFs of the ARISE and ASR variables along the flight track. First, Fig. 3a indicates that ASR simulates less QC than observed, manifesting as fewer occurrences of high QC values. When restraining the ASR data to the ARISE flight track (clear and cloudy regions), ASR produces 21 % of the observed average total QC (0.007 versus 0.033 g kg−1). When expanded to the full Beaufort Sea, ASR produces 0.018 g kg−1 (56 % of ARISE). ASR significantly underrepresents QC in low Arctic clouds. This disagreement is substantially larger than can be explained with measurement uncertainty, and it urges an explanation.
The thermodynamic regime PDFs offer clues as to why ASR has less QC. Considering all conditions (clear and cloudy) along the ARISE flight track, ASR is on average 1.40 K warmer with a lower QV (0.06 g kg−1) than observed, resulting in a 4.3 % lower average RH. The reduced RH inhibits cloud formation and thus the generation of QC in ASR. The warm and dry biases across the full Beaufort Sea domain are even greater. Segal-Rozenhaimer et al. (2018) found similar warm and dry biases in MERRA-2 relative to ARISE, suggesting that the warm bias in the lower Arctic troposphere may be a common feature of meteorological reanalysis.
Bear in mind that T, QV, and RH are not entirely independent. Indeed, RH is a function of both T and QV, and maximum QV (approximately equilibrium QV) is limited by T. So the three variables should not be interpreted as three separate metrics of the thermodynamic state. Rather, they represent three different related, but distinct, means of characterizing the thermodynamic state.
Considering only cloudy grid boxes (defined as total QC>0.02 g kg−1; Fig. 3e), the ASR average QC along the ARISE flight tracks is 55 % of the observed value (0.06 versus 0.11 g kg−1, respectively). Because the cloud-only QC value for ASR is twice that of the clear+cloudy value, the lack of QC in ASR stems from both less frequent cloudy grid boxes and smaller in-cloud QC values. In-cloud flight track ASR T is 3.10 K warmer and QV is 0.45 g kg−1 greater than observed, with similar values for the whole Beaufort Sea. The higher QV boosts RH, overcoming the drying effect of warmer T, resulting in RH for ASR being 5.8 % greater. Despite the higher QV, the QC PDF in cloudy grid boxes (Fig. 3e) shows that ASR still produces large QC values less frequently than observed. This suggests that the high QV is not converted to QC by the parameterized cloud physics as efficiently as observed, pointing to a key deficiency.
One additional feature of note in Fig. 3h is that ASR rarely produces clouds in grid boxes with less than 90 % RH, while ARISE data show clouds occurring (QC<0.02 g kg−1) at grid-box-averaged RH values as low as 40 %. ASR is coded to cap grid box RH at 100 % and also to not produce clouds below 80 % RH, which (mostly) prohibits the presence of clouds in marginally humid conditions. Thus, ASR forms clouds over a narrower range of atmospheric conditions (specifically, RH values) than observed in situ.
3.2 Vertical cloud water and thermodynamic profiles
Figure 4 shows the vertical distribution of QC in ARISE and ASR below 1000 m. Observed QC shows two primary maxima at ∼400 m and at or above 1000 m; these maxima also align with QL profiles over the Arctic Ocean from CALIPSO–CloudSat data (e.g., Taylor et al., 2015). Examining cloudy grid boxes, the QC maximum near 1000 m is larger than that at ∼400 m. Both maxima are dominated by the liquid phase.
ASR shows multiple deficiencies in the simulated QC vertical profile compared with ARISE. These deficiencies are more evident when comparing along the ARISE flight tracks but are also found when considering the Beaufort Sea domain (Fig. 4c and f). Most notably, ASR produces too little QC above 500 m to the point that the higher-altitude maximum is almost nonexistent. Within cloudy grid boxes, ASR reproduces the amplitude of the lower-altitude maximum up to 300 m. A major component of the disagreement likely stems from a poor representation of the processes that generate the upper cloud layer, including interactions with large-scale advection and the free troposphere (e.g., Shupe et al., 2013). Additionally, ASR simulates very little QI during the campaign, indicating that mixed-phase cloud microphysics are not a factor driving the lack of QC in ASR. Moreover, Segal-Rozenhaimer et al. (2018) also identified a lack of cloud cover in MERRA-2 relative to ARISE data, which also corresponds to warm–dry biases. However, they reported missing clouds below 500 m, whereas we find missing clouds (in the form of less QC) above 500 m.
The partitioning between QC and precipitation represents a possible reason for the ASR–ARISE difference; ARISE observations do not partition between QC and precipitation, whereas the ASR bulk cloud microphysics do. Thus, the missing QC in ASR could result from an overactive precipitation conversion. To investigate this, Fig. 4b, c, e, and f plot the sum of QC and precipitation (dashed line) in addition to QC. Precipitation water more than doubles the total condensate above 500 m, and yet this does not bring the QC close to the observed value. Thus, there is no evidence that an overactive conversion parameter explains the lack of QC above 500 m.
Because of the close interplay of clouds and thermodynamics, the errors in the ASR vertical cloud profile are likely related to errors in the boundary layer thermodynamic structure. Figure 5 shows the T, QV, and RH vertical profiles for ARISE and ASR. ASR has a greater T and lower RH than ARISE, while QV is similar. This corresponds to the PDFs shown in Fig. 3 and demonstrates that the warm bias in ASR is the main contributor to the low RH. The warm and dry ASR biases are also found across the Beaufort Sea domain (not shown), demonstrating that the thermodynamic errors are not statistical artifacts from the flight path sampling.
The warm and dry biases extend throughout the boundary layer, with no obvious altitude dependence. This is different than the disagreement reported by Segal-Rozenhaimer et al. (2018), wherein the warm and dry biases in MERRA-2 are mostly confined to below 500 m. There is likely a connection between the lack of cloud cover and the warm–dry biases in MERRA-2 below 500 m, whereas there is no obvious direct connection between the lack of QC above 500 m and the warm–dry bias extending evenly throughout the boundary layer. Therefore, we speculate that the MERRA-2 and ASR cloud vertical distributions differences with observations have different causes.
4.1 Bivariate analysis
The T and RH biases in ASR represent one type of contribution to the low mean QC bias in ASR. However, the relationships between QC and thermodynamic variables are another important contributor. Figure 6 shows the observed and simulated bivariate relationships between QC and T, QV, and RH. ARISE data show increased QC at higher RH, as expected, but also at low T and QV. The latter relationship is curious, as higher QV provides more vapor for conversion into QC; however, the small correlation (0.23) indicates a weak relationship. This is not a result of an unusual sensitivity of RH to T and QV in the observations and ASR, as the sensitivities in ARISE and ASR are almost identical. Compared with ARISE, ASR also shows QC increasing with RH (Fig. 6). As the PDFs in Fig. 3 suggest, ASR produces very little QC when RH is below 90 %. These results also hold when considering cloudy grid boxes (Fig. 7). ASR has difficulty producing QC outside an unrealistically narrow range of meteorological conditions, contributing to the low mean QC bias. These simulated dependencies of QC on T and QV disagree with observations influencing the low QC bias in ASR.
Unlike the ARISE results, ASR information is not limited to the ARISE flight path. It is possible to look at the simulated QC–thermodynamic variable relationships considering all ASR grid boxes within the Beaufort Sea domain during ARISE. This is useful for characterizing the simulated cloud–thermodynamics relationships more completely such that they are not affected by the limited flight track sampling. To determine the extent to which the ASR results are affected by the flight track sampling, Fig. 6g–i show the relationships in ASR when considering the Beaufort Sea domain. Compared to Fig. 6d–f, the full dataset shows a larger sensitivity of QC to T and also a few cases in which cloudy grid boxes occur with RH below 90 %. However, the unrealistic relationship between QC and QV persists.
4.2 Contributions of error types to ASR cloud water
Taken together, Figs. 3 and 6 qualitatively show that the deficiency in ASR QC is related to errors in the simulated thermodynamic conditions and errors in the QC–thermodynamics relationships. We quantify the contributions of these error sources to the low QC bias by constructing a synthetic QC dataset from the observed thermodynamic conditions and ASR-derived relationships between QC and thermodynamics. We then calculate the change in QC that occurs when the ASR thermodynamics and relationships are assumed to be “reality”. Ideally ASR would produce 100 % of the observed value; the closer a QC percentage is to 100 %, the greater the improvement to ASR the change produces. The synthetic QC dataset is constructed by substituting the ASR-derived relationship (from Fig. 6) for the observed ARISE QC values (e.g., for every instance that ARISE reported a T of approximately −10 ∘C, replace the observed ARISE QC value with 0.01 g kg−1 from Fig. 6d). A mathematically equivalent way of doing this calculation is to multiply the ARISE PDF of T (Fig. 3b, black bars) by the ASR bivariate relationship of QC versus T (Fig. 6d, black curve). Averaging this product gives a QC value of 0.008 g kg−1, 24 % of the observed ARISE mean QC value of 0.033 g kg−1. This shows that much of the QC deficit in ASR is related to ASR not producing enough QC when T is low. Similar results are found when considering different thermodynamic regime sizes (e.g., T regime sizes are reduced from 5 to 2 ∘C).
To find the effect of the simulated ASR T values on the QC deficit, the converse calculation is performed – multiplying the ASR PDF of T (Fig. 3b, red bars) by the ARISE bivariate relationship between QC and T (Fig. 6a, black curve). Averaging this product yields a QC value of 0.014 g kg−1 (45 %). The larger resulting percentage shows that the warm bias in ASR produces as significant, while slightly smaller, a reduction in QC as the unrealistic QC–T relationship.
Performing the same calculations with QV tells a very different story. Substituting the ASR bivariate QC–QV relationship results in a mean QC of 0.008 g kg−1 (24 %), a reduction roughly equivalent to the total ASR QC deficiency. However, using the ASR QV PDF and the observed QC–QV relationship gives a mean QC of 0.033, a 3 % increase over the observed QC value. For QV, the erroneous bivariate relationship is the sole factor in the ASR QC deficiency. In other words, plenty of QV is available in the ASR atmosphere to produce the observed QC values; however, ASR fails to convert enough vapor into QC.
Performing the same calculations for RH produces mean QC values of 0.007 (23 % of the ARISE mean QC) and 0.025 g kg−1 (79 %) when subbing the ASR QC–RH relationship and the RH PDF, respectively. In this case, ASR does not produce large RH values frequently enough and does not produce enough QC when RH is sufficiently large; however, the latter is primarily responsible for the small QC in ASR. Note that this analysis treats the three thermodynamic variables independently, whereas in reality they are interdependent – particularly RH on both T and QV. This is why the errors in simulated T and RH PDFs both have such notable effects on the mean QC and why the mean QC biases caused by the PDF biases and QC–thermodynamic relationships do not cleanly sum up to 100 %.
Switching the ASR output from the flight-track-only to the Beaufort Sea domain shows the effects of the sampling and more complete understanding of which factors are responsible for the larger mean QC value (0.018 g kg−1) for the Beaufort Sea domain. The mean QC calculated when subbing the ASR QC–T relationship and the T PDF are 0.022 (69 %) and 0.013 g kg−1 (41 %), respectively. The more realistic QC–T relationship seen in Fig. 6 g corresponds to the much larger ASR QC in the full dataset, but the warm bias still results in a severely low ASR QC. The mean QC when subbing ASR QV and QC–QV relationship PDFs is 0.020 (62 %) and 0.025 g kg−1 (77 %). Thus, considering the QC–QV relationship derived using the ASR output for the Beaufort Sea domain is not as strong of a factor for reducing QC in the full ASR dataset compared with the flight track output. The larger QC value for 2 g kg−1 QV in Fig. 6h versus 6e seems to be the most important factor in the larger mean QC in the full dataset.
Subbing RH has a very peculiar result: 0.013 (39 %) and 0.037 g kg−1 (116 %), which is strange considering that the domain-averaged ASR is drier than the flight-track-averaged data. How does a drier atmosphere lead to increased QC? The answer lies in the RH PDF (Fig. 3h). Unlike ARISE and flight track ASR, the full Beaufort Sea ASR PDF is bimodal. The dry mode is responsible for the small mean ASR. The wet mode peaks at 100 % RH, unlike the other two PDFs, and at the value for which observed QC (Fig. 6c) maximizes. The boost to QC given by the wet mode peak overcomes the drying effect of the dry mode. Thus, the change in the PDF shape of Beaufort Sea ASR RH from flight track PDFs leads to increased QC.
4.3 Trivariate analysis using two-variable thermodynamic regimes
The previous results warrant further trivariate analysis of the QC–thermodynamic relationships using two thermodynamic variables versus QC. Figure 8 shows that the observed QC is largest in conditions with high RH and low T (Fig. 8a), high RH and low QV (Fig. 8d), and low T and low QV (Fig. 8g). Together, QC during ARISE is largest in low T, low QV, and high RH conditions. This result clarifies the curious relationship between smaller QV values and larger QC from Fig. 6b, as QV is constrained by the Clausius–Clapeyron relationship and must be small at low T, which is apparent in Fig. 8g. Moreover, ARISE data indicate a strong sensitivity of QC to T, a relationship that is much weaker in ASR.
The dependence of QC on the thermodynamic regimes in ASR along the flight track hardly resembles the observations (Fig. 8b, e, and h). The lack of total QC in ASR is indicated as no values above 64 mg kg−1 appear in Fig. 8b. The largest disagreement between ARISE and ASR involves the observed relationship of large QC values at low T and low QV. Some of the disagreement stems from ASR not capturing all of the observed meteorological regimes. Particularly, the lowest T values did not occur in ASR along the flight path, illustrated by the gray boxes in Fig. 8h around −15 ∘C. The dependence of QC in ASR shows that slightly larger QC values occur at lower T and large QV (Fig. 8h), a much weaker dependence than observed (Fig. 8g vs. h). Moreover, Fig. 8e indicates no preference for ASR to simulate large QC values at lower QV.
The narrower range of conditions sampled along the flight track within ASR again motivated an examination of the thermodynamic regimes within the larger Beaufort Sea domain. The comparison between the flight-track-only and Beaufort Sea domain results raises questions about the representativeness of the relationships found when using the flight-track-only output. Figure 8c, f, and i show the QC–thermodynamic regimes determined for the Beaufort Sea domain. Comparing these results with panels Fig. 8b, e, and h reveals the larger range of thermodynamic conditions sampled (i.e., the non-gray regions are larger), enabling an assessment of ASR-simulated QC over a wider range of thermodynamic regimes. Figure 8i indicates that high QC values in regimes of low T–low QV manifest within the Beaufort Sea domain. Thus, at least some of the “missing” QC results from the flight track not intersecting the low T–low QV regime produced nearby.
The simulated dependence of QC on thermodynamic regimes also contributes to the differences in the mean QC with ARISE. Specifically, ASR concentrates the largest QC values at the lowest ranges of T and QV, showing a faster decrease in QC than ARISE as T and QV increase (about 40 % faster at T of −10 ∘C and QV of 1 g kg−1). ASR only produces large QC under the extreme thermodynamic ranges. Thus, the inability of ASR to simulate larger QC under typical thermodynamic conditions contributes to the disagreements with ARISE.
Another noteworthy result is that the ASR Beaufort Sea domain analysis suggests a secondary regime of high T–high QV with large QC values. This high QC regime is not found in ARISE data. This result raises important questions about the realistic nature of this thermodynamic regime. Further exploration of this is beyond the scope of the present analysis.
4.4 Effect of joint reanalysis error types on simulated cloud water
The analysis discussed in Sect. 4.2 is applied to quantify and compare the dependence of the ASR QC bias based upon the thermodynamic regime joint PDFs. Subbing the flight track ASR QC–thermodynamic regime relationships (Figs. 8b, e, and h) yields mean QC values of 0.007 g kg−1 (23 % of the ARISE mean QC) for RH and T, 0.006 g kg−1 (19 %) for RH and QV, and 0.008 g kg−1 (25 %) for T and QV. Subbing the ASR thermodynamic regime frequency of occurrence (not shown) results in mean QC values of 0.013 (39 %), 0.016 (50 %), and 0.015 g kg−1 (45 %). Thus, both the ASR QC–thermodynamic regime relationships and the differences in thermodynamic regime frequency contribute substantially to the low QC bias in ASR, though the former has the greater influence.
Subbing the full ASR dataset instead produces modest increases in mean QC. When substituting the QC–thermodynamic regime relationships, only the T–QV regime shows a significant increase in mean QC of 0.017 g kg−1 (52 %). This is connected to the improved representation of the observed large QC values with low T and QV. However, this is not sufficient to overcome the ASR's aversion to producing clouds in lower RH conditions. When subbing the ASR regime frequency of occurrence, RH and QV show the largest increase in mean QC of 0.017 g kg−1 (52 %). The biases in thermodynamics lead to major underestimates of QC even when the full ASR dataset is used – adding more data does not resolve the deeply rooted errors in T and RH. Of the three variable pairings, given the imperfect separation between these semi-dependent variables, improvement in mean QC comes primarily from the more realistic representation of the QC, with the T and QV relationship and the QC boosting effect of the RH PDF shape (Sect. 4.2).
The previous section shows that a direct comparison of ARISE and ASR data along the ARISE flight path finds that the relationships between cloud variables and thermodynamic regimes are substantially different. However, when considering QC–thermodynamic regime relationships in ASR for the entire Beaufort Sea domain and time period, the relationships are established over a wider range of conditions and better resemble the ARISE data. This implies that a possible source of uncertainty originates from the limited sampling of meteorological conditions along the flight path. At first glance this may be a nonintuitive result – should the along-track ASR results not agree more closely with ARISE than the domain-averaged results? But consider that the ASR–ARISE discrepancies in mean QC are partially understood by differences in the QC–thermodynamic relationships and the differences between the sampled vs. simulated thermodynamic regimes; however, there is still the question as to the magnitude of the sampling uncertainty in the mean QC. While it is not possible from ARISE data to quantify the sampling uncertainty, it can be estimated using ASR output. In addition to quantifying sampling uncertainty, the knowledge gained has utility for the design of future aircraft campaigns for which observation–model comparison is a major goal.
5.1 Experiment setup
This experiment tests the effect of sampling on the ASR QC–thermodynamic regime relationship results by simulating alternate ARISE aircraft flight paths and times within the operation domain. ARISE flight paths were constrained by the overpass times of CERES-bearing satellites and not driven by meteorological conditions. This experiment uses a random sampling approach to simulate alternate ARISE aircraft flight paths, assuming no targeting of any particular meteorological conditions to quantify how the ASR–ARISE comparisons are affected by different flight configurations. The experiment proceeds as follows.
The eight flight paths during the low-level portions of the flights are randomly assigned days from the 8 d that ARISE flew and random start times during the day.
Each randomized flight has a random starting point within the ARISE domain and a random rotation from the original flight path orientation. Flight paths must stay within the domain at all times, and those that leave are re-randomized.
ASR-simulated cloud and thermodynamic data are collected and processed into the QC–thermodynamic regime format, as seen in Fig. 8, and stored.
Steps 1–3 are repeated, with each iteration of eight flights considered a “trial” campaign. After 50 000 trials are completed, the results are used to tabulate indices that represent sampling uncertainty for each meteorological regime.
Figure 9 displays three indices summarizing the sampling experiment results. Figure 9a, e, and i show the likelihood for a single experiment of eight flights that each meteorological regime is encountered at least once. The highest likelihood lies near the center of the data range, as expected, though RH (QV) chances are slightly shifted towards higher (lower) values. For meteorological regimes with large QC values, those with average T and lower QV are most likely to be sampled. Sampling of the low T–low QV and high T–high QV regimes shows a likelihood of 10 % or less. As these regimes have the highest QC values in the full dataset, this indicates that the ASR domain-averaged QC value is lower because the simulated aircraft has the lowest probably of intercepting the extreme ranges of the thermodynamic regimes wherein the largest QC values occur (assuming the high T–high QV regime is realistic).
Figure 9b, f, and j show the number of samples collected in each meteorological regime on average across the experiments. The number of samples is important for calculating reliable statistics for the QC values in each thermodynamic regime. The results follow a similar pattern as the sampled likelihood results, and the regimes with the largest QC have few if any samples. Low T–low QV conditions are rare in ASR and occur for less than 0.1 % of all samples. This partially explains why the large QC values for low T–low QV are not apparent along the flight track (Fig. 8h) even in the regimes that have data for both ASR and ARISE.
Figure 9c, g, and k display the mean absolute error (MAE) of the QC for each thermodynamic regime. The MAE is calculated as the average absolute value of the difference between each trial QC and the population QC (Fig. 9d, h, and l). This metric quantifies how close to the population value a single trial's value can be expected to be for each thermodynamic regime that is sampled in the trial – while the mean error would approach zero because of positive and negative differences, the MAE does not and is similar to standard deviation. The magnitude of MAE scales closely with the population mean QC value. In thermodynamic regimes with high QC values, MAE is typically about half of the population mean, meaning that errors of ∼50 % can be expected for a trial experiment. However, this is not universal, particularly for the T and QV results for which, for example, the MAE at −10 ∘C and 1 g kg−1 (Fig. 9k) is 184 % of the population mean (8.9 versus 4.8 mg kg−1). Recall that this regime shows major disagreement between ARISE and ASR along the flight path (Fig. 8g and h) under low T–low QV conditions. The large experimental MAE result suggests that a single trial is likely to miss the large QC value in this regime even if it is sampled. In other words, these conditions can be associated with both cloudy and clear-sky conditions in the ASR realizations. A similar issue is encountered in the high T–high QV regime.
The standard deviations of the total QC across the experiments are shown in Fig. 9d, h, and l. The results resemble MAE, with the notable exception of high T–high QV conditions. Because standard deviation tends to be more sensitive to outliers than MAE, this result indicates that most random samplings of these conditions have an error smaller than the population mean value, with a small chance that a big outlier might be sampled instead. In other words, it is possible but unlikely to sample clear-sky conditions in the high T–high QV regime on the flight track and, if this is the only sample, conclude that no clouds occur under these conditions.
5.3 Implication of the sampling results
The random sampling approach is a powerful tool helping to assess how representative a single field campaign may be in characterizing the cloud conditions within in each regime. The large MAE and standard deviations in some thermodynamic regimes suggest that the relationships derived from flight-track-only information contain significant sampling uncertainty.
Based upon the ASR Beaufort Sea domain analysis, it seems serendipitous that the ARISE flights flew though regions of low T–low QV and captured the large QC values under these conditions. On the other hand, this serendipitous occurrence could have resulted from the cloud-seeking priority of the ARISE aircraft. Conversely, it could have been bad luck that ARISE missed high T–high QV cloudy conditions. Are the ARISE results a possible realization of the full ASR dataset? Figure 10 provides a method of assessing the representativeness of ARISE from the full ASR dataset. The majority of thermodynamic regimes with large QC values in both ARISE and ASR show that the ARISE values are within the sampling uncertainty estimated from the random sampling test. For the most part the ARISE data are a possible realization of the ASR dataset. Only ARISE–ASR QC differences at RH<80 % differ by more than 2 standard deviations.
These results also reveal a more general aspect of designing methodologies for comparisons between aircraft data and models (or reanalyses). When given a choice between precisely collocating the aircraft data with the model or including more simulated data points in the comparison, it appears that including more data points leads to a fairer and more robust comparison. The reason why the larger sample size is favorable is that (1) it provides a larger dynamic range of data points, particularly extreme conditions which may be missed by precisely collocating to the aircraft flight track, and (2) it reduces the noise in the quantification of the model behavior and cloud versus thermodynamics relationships.
More comprehensive evaluations using random sampling applied to satellite data may aid in future design of aircraft campaigns to minimize chances of missing meteorologically interesting conditions. Ideally, this could be accomplished by having the aircraft target conditions that should produce clouds according to the models rather than just seeking where there are clouds. However, as this may be challenging to forecast, other strategies such as increasing the number and/or duration of flights is a useful substitute.
We have examined the ability of ASR to replicate the observed cloud water, thermodynamic conditions, and the relationships between them with respect to the ARISE aircraft field campaign observations during September 2014. This includes quantifying the sensitivity of cloud water to the thermodynamic regimes using methods frequently employed in studies of satellite data. Further, a Monte Carlo-style random sampling of the ASR output was employed to understand the influence of limited aircraft sampling on the results.
The results address the following questions.
How does cloud water in ARISE and ASR compare? Compared with ARISE observations, ASR produces too little cloud water, about 25 %–50 % of the observed value. This is a much larger disagreement than can be explained with measurement uncertainty alone. Notably, ASR produces almost no cloud water above 500 m, whereas ARISE depicts cloud occurrence extending above 1000 m. However, when clouds below 500 m are simulated in ASR, it produces realistic values of cloud water. Both observed and simulated clouds are dominated by the liquid phase. The lack of observed cloud ice indicates that the ARISE–ASR differences in cloud water do not result from the parameterization of mixed-phase cloud microphysics. Also, ASR produces little precipitation water, ruling out an overactive cloud water-to-precipitation conversion scheme.
Can discrepancies between ARISE and ASR be explained by grid-scale disagreements in meteorological conditions and/or errors in the simulated cloud–thermodynamic relationships? A number of factors contribute to the low cloud water bias in ASR. With regard to the average meteorological conditions, ASR is 1.4 ∘C warmer and 0.06 g kg−1 drier than ARISE, leading to a ∼4 % lower relative humidity. The warm temperature bias occurs throughout the boundary layer and is the larger contributor to the lower relative humidity in ASR. In addition, ASR produces clouds across a narrower range of relative humidity values near 100 %, while ARISE detected clouds in regions where the spatially averaged relative humidity was below 50 %. This further constricts the opportunity that ASR has to form clouds. Our results also show that the ARISE–ASR differences are attributed primarily to differences in the cloud–thermodynamic regime relationships and secondarily (but still importantly) to the warmer and drier simulated thermodynamic regimes. The relative importance of the primary and secondary factors are roughly to . Thus, considering a circumstance under which ARISE and ASR have the same thermodynamic conditions, ASR mean total cloud water is ∼40 % lower than the ARISE-observed value. Considering thermodynamic regimes of temperature, specific humidity, and relative humidity depicts that ARISE observations show large cloud water values in meteorological regimes of low temperature, low specific humidity, and high relative humidity. ASR, in opposition, shows little relationship between cloud water and temperature, with specific humidity being the only (weak) control. This result is found in both the flight track and Beaufort Sea domain results.
How are ARISE–ASR comparisons affected by the coverage of ARISE flights? Disagreement in the thermodynamic regime–cloud water relationships occurs between the flight track and Beaufort Sea domain analyses, indicating an influence of sampling on the model–observation comparisons. On one hand, the Beaufort Sea domain analysis shows that ASR simulates the high cloud water amounts within the low temperature–low specific humidity regime. This is not evident in the ASR flight track results because the flight path did not intercept this regime, contributing to the low ASR cloud water. Including this low temperature–low specific humidity regime in the full dataset roughly doubles the mean simulated cloud water to about half of the observed value. On the other hand, the effect of the warm and dry (relative humidity) biases on simulated cloud water is just as severe in the full ASR dataset as in the flight-track-only data. Thus, an important lesson from this analysis is that when comparing in situ airborne data with model output one should not restrict the comparison to flight-track-only model output, as expanding the domain isolates omnipresent thermodynamic biases in the reanalysis.
In addition, the full ASR dataset shows a second cloud water maximum within an unobserved high temperature–high specific humidity thermodynamic regime. It is not clear from the ARISE data if the aircraft simply missed sampling this regime or if the regime exists.
The effect of limited sampling of ASR along the ARISE flight path is estimated with a Monte Carlo random sampling analysis of the full ASR dataset within the Beaufort Sea domain. The results demonstrate that thermodynamic regimes with large cloud water are rare and unlikely to be sampled by chance alone for the number and length of ARISE flights. In several of the regimes, sampling uncertainty obscures the relationships between cloud water and thermodynamic regimes such that it could not be determined that the ARISE–ASR differences (even large ones) were not caused by sampling uncertainty. From this it appears that including a greater number of data points from ASR provides a more useful and robust comparison with the ARISE data than precisely collocating ASR data with the ARISE flight track.
While the ARISE campaign was designed primarily to investigate radiative fluxes in conjunction with satellite overpasses, the random sampling results can also inform the design of future aircraft campaigns intended to test cloud and thermodynamic properties in reanalysis and other atmospheric models. A possible solution to the sampling issues discussed here is to direct aircraft not just to regions where clouds are observed, but also to regions of thermodynamic conditions in which models predict that clouds should be and methodically sample them to build up a sufficient sample size to reduce statistical noise. Moreover, an increased number of flights with a systematic sampling strategy would help reduce sampling uncertainty by raising the chances of sufficiently sampling the thermodynamic regimes of interest and better capture the variability of cloud conditions occurring in these regimes. This approach will better support one of the key benefits of aircraft campaigns, to sample meteorological properties that satellites cannot, in a more statistically sound manner.
The ARISE data were obtained from the NASA Langley Research Center Atmospheric Science Data Center (https://doi.org/10.5067/SUBORBITAL/ARISE/DATA001; NASA/LARC/SD/ASDC, 2014a). In situ cloud measurements are obtained from https://doi.org/10.5067/AIRCRAFT/ARISE_Cloud_AircraftInSitu_C130_Data_1 (NASA/LARC/SD/ASDC, 2014b), while thermodynamic and aircraft position data are obtained from https://doi.org/10.5067/AIRCRAFT/ARISE_MetNav_AircraftInSitu_C130_Data_1 (NASA/LARC/SD/ASDC, 2014c). ASR version 2 (NCAR, 2017) data are provided by the National Center for Atmospheric Research/University Corporation for Atmospheric Research and the Polar Meteorology Group/Byrd Polar and Climate Research Center/The Ohio State University.
JBD designed and conducted the large majority of the analyses presented in this paper. PCT assisted in the analysis design, literature review, and various other necessary tasks. RHM provided technical details for ARISE, and DB the same for ASR. RHM, KH, KT, CC, BA, and EW participated in collecting data during ARISE. JRB provided some analysis and corrections to the original ARISE dataset. JBD prepared the paper with contributions from all co-authors.
The authors declare that they have no conflict of interest.
Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
J. Brant Dodson and Patrick C. Taylor were both supported in part by the NASA Radiation Sciences Program. Patrick C. Taylor was also partially supported by the NASA Radiation Budget Science Project. Richard H. Moore and Chelsea A. Corr were supported by NASA postdoctoral fellowships. The NASA Langley Aerosol Research Group (LARGE; https://science.larc.nasa.gov/large/, last access: 12 July 2021), including Richard H. Moore, Kenneth Thornhill, Chelsea A. Corr, Bruce Anderson, and Edward Winstead, was funded by the NASA Radiation Sciences Program, managed by Hal Maring. The participation by David H. Bromwich and Keith M. Hines in this research was supported by the Office of Naval Research. This is contribution number 1607 of the Byrd Polar and Climate Research Center.
This research has been supported by NASA (grant no. NNH16ZDA001N-NDOA) and the ONR (grant no. N00014-18-1-2361).
This paper was edited by Barbara Ervens and reviewed by two anonymous referees.
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