Research article 09 Mar 2021
Research article  09 Mar 2021
Using machine learning to model uncertainty for water vapor atmospheric motion vectors
 Jet Propulsion Laboratory, California Institute of Technology, Pasadena, USA
 Jet Propulsion Laboratory, California Institute of Technology, Pasadena, USA
Correspondence: Joaquim V. Teixeira (joaquim.p.teixeira@jpl.nasa.gov)
Hide author detailsCorrespondence: Joaquim V. Teixeira (joaquim.p.teixeira@jpl.nasa.gov)
Windtracking algorithms produce atmospheric motion vectors (AMVs) by tracking clouds or water vapor across spatial–temporal fields. Thorough error characterization of windtracking algorithms is critical in properly assimilating AMVs into weather forecast models and climate reanalysis datasets. Uncertainty modeling should yield estimates of two key quantities of interest: bias, the systematic difference between a measurement and the true value, and standard error, a measure of variability of the measurement. The current process of specification of the errors in inverse modeling is often cursory and commonly consists of a mixture of model fidelity, expert knowledge, and need for expediency. The method presented in this paper supplements existing approaches to error specification by providing an error characterization module that is purely datadriven. Our proposed error characterization method combines the flexibility of machine learning (random forest) with the robust error estimates of unsupervised parametric clustering (using a Gaussian mixture model). Traditional techniques for uncertainty modeling through machine learning have focused on characterizing bias but often struggle when estimating standard error. In contrast, modelbased approaches such as kmeans or Gaussian mixture modeling can provide reasonable estimates of both bias and standard error, but they are often limited in complexity due to reliance on linear or Gaussian assumptions. In this paper, a methodology is developed and applied to characterize error in tracked wind using a highresolution global model simulation, and it is shown to provide accurate and useful error features of the tracked wind.
© 2018 California Institute of Technology. Government sponsorship acknowledged.
Reliable estimates of global winds are critical to science and application areas, including global chemical transport modeling and numerical weather prediction. One source of wind measurements consists of featuretrackingbased atmospheric motion vectors (AMVs), produced by tracking time sequences of satellitebased measurements of clouds or spatially distributed water vapor fields (Mueller et al., 2017; Posselt et al., 2019). The importance of global measurements of threedimensional winds was highlighted as an urgent need in the NASA Weather Research Community Workshop Report (Zeng et al., 2016) and was identified as a priority in the 2007 National Academy of Sciences Earth Science and Applications from Space (ESAS 2007) decadal survey and again in ESAS 2017. For instance, wind is used in the study of global CO_{2} transport (Kawa et al., 2004), numerical weather prediction (NWP; Cassola and Burlando, 2012), as inputs into weather and climate reanalysis studies (Swail and Cox, 2000), and for estimating current and future windpower outputs (Staffell and Pfenninger, 2016).
Thorough error characterization of windtrack algorithms is critical in properly assimilating AMVs into forecast models. Prior literature has explored the impact of “poor” error characterization in Bayesianbased approaches to remotesensing applications. Nguyen et al. (2019) proved analytically that when the input bias is incorrect in Bayesian methods (specifically, optimal estimation retrievals), then the posterior estimates would also be biased. Moreover, they proved that when the input standard error is “correct” (that is, it is as close to the unknown truth as possible), then the resulting Bayesian estimate is “efficient”; that is, it has the smallest error among all possible choices of prior standard error. Additionally, multiple active and passive technologies are being developed to measure 3D winds, such as Doppler wind lidar (DWL), radar, and infrared or microwave sensors that derive AMVs using feature tracking of consecutive images. Therefore, an accurate and robust methodology for modeling uncertainty will allow for more accurate assessments of mission impacts and the eventual propagation of data uncertainties for these instruments.
Velden and Bedka (2009) and Salonen et al. (2015) have shown that height assignment contributes a large component of uncertainty in AMVs tracked from cloud movement and from sequences of infrared satellite radiance images. However, with AMVs obtained from water vapor profiling instruments (e.g., infrared and microwave sounders), height assignment error cannot be directly assessed purely through analysis of the AMV extraction algorithm. Height assignment is instead an uncertainty in the water vapor profile itself. Unfortunately, without the quantified uncertainties on the water vapor profile necessary to pursue such a study, that is well beyond the scope of this paper. As such, this study will focus on errors in the AMV estimates at a given height. Previous work has demonstrated several different approaches for characterizing AMV vector error. One common approach is to employ quality indicator thresholds, as described by Holmund et al. (2001), which compare changes in AMV estimates between sequential time steps and neighboring pixels, as well as differences from model predictions, to produce a quality indicator to which a discrete uncertainty is assigned. The expected error approach, developed by Le Marshal et al. (2004), builds a statistical model using linear regression against AMVradiosonde values to estimate the statistical characteristics of AMV observation error.
In this study, we outline a datadriven approach for building an AMV uncertainty model using observing system simulation experiment (OSSE) data. We build on the work by Posselt et al. (2019), in which a water vapor featuretracking AMV algorithm was applied to a highresolution numerical simulation, thus providing a global set of AMV estimates which can be compared to the reference winds produced by the simulation. In this case, a synthetic “true” state is available with which AMVs can be compared and errors are quantified, and it is shown that errors in AMV estimates are state dependent. Our approach will use a conjunction of machine learning (random forest) and unsupervised parametric clustering (Gaussian mixture models) to build a model for the uncertainty structures found by Posselt et al. (2019). The realism and robustness of the resulting uncertainty estimates depend on the realism and representativeness of the reference dataset. This work builds upon the work of Bormann et al. (2014) and HernandezCarrascal and Bormann (2014), who showed that wind tracking could be divided into distinct geophysical regimes by clustering based on cloud conditions. This study supplements that approach with the addition of machine learning, which, compared with traditional linear modeling approaches, should allow the model to capture more complex nonlinear processes in the error function.
Traditional techniques for modeling uncertainty through machine learning have focused on characterizing bias but often struggle when estimating standard error. By pairing a random forest algorithm with unsupervised parametric clustering, we propose a datadriven, clusterbased approach for quantifying both bias and standard error from experimental data. According to the theory developed by Nguyen et al. (2019), these improved error characterizations should then lead to improved error characteristics (e.g., lower bias, more accurate uncertainties) in subsequent analyses such as flux inversion or data assimilation.
This paper does not purport that the specific algorithm detailed here should supplant error characterization approaches for all AMVs; indeed, most commonly assimilated AMVs are based on tracking cloud features, not water vapor profiles. In addition, this algorithm is trained and developed for a specific set of AMVs extracted from a water vapor field associated with a particular range of flow features. As such, application of our algorithm to modeled or observed AMVs will be most appropriate in situations with similar dynamics to our training set. However, we intend in this paper to demonstrate that the methodology is successful in characterizing errors for this set of water vapor AMVs and suggest that this approach – that is, capturing statedependent uncertainties in featuretracking algorithms through a combination of clustering and random forest – could be implemented in other featuretracking AMV extraction methods and situations.
The rest of the paper is organized as follows: in Sect. 2, we give an overview of the simulation which provides the training data for our machine learning approach. We then motivate and define the specific uncertainties this study aims to characterize. In Sect. 3, we describe the error characterization approach with the specifics of our error characterization model, including both the implementation of and motivations for employing the random forest and Gaussian mixture model. In Sect. 4, we provide a validation of our methods, attempting to assess the bias of our predictions. In Sect. 5, we discuss the implications of our error characterization approach, both on AMV estimation and data assimilation, more broadly.
2.1 Simulation and featuretracking algorithm
We trained our model on the simulated data used by Posselt et al. (2019), which applied an AMV algorithm to outputs from the NASA Goddard Space Flight Center (GSFC) Global Modeling and Assimilation Office (GMAO) GEOS5 Nature Run (G5NR; Putman et al., 2014). The Nature Run is a global dataset with ∼ 7 km horizontal grid spacing that includes, among other quantities, threedimensional fields of wind, water vapor concentration, clouds, and temperature. Note that throughout the text we will use the term “Nature Run wind” to refer to reference winds in the simulation dataset used to train the uncertainty model. The AMV algorithm is applied on four pressure levels (300, 500, 700, and 850 hPa) at 6hourly intervals, using three consecutive global water vapor fields spaced 1 h apart, and for a 60 d period from 1 July to 30 August 2006. The water vapor fields from GEOS5 were input to a localarea pattern matching algorithm that approximates wind speed and direction from movement of the matched patterns. The algorithm searches a preset number of nearby pixels to minimize the sum of absolute differences between aggregated water vapor values across the pixels. Posselt et al. (2019) describe the sensitivity of the tracking algorithm and the dependency of the tracked winds on atmospheric states in detail. The coordinates of the data are on a 5758 × 2879 × 240 spatiotemporal grid for the longitude, latitude, and time dimension, respectively.
It is important to note that the AMV algorithm tracks water vapor on fixed pressure levels. In practice, these would be provided by satellite measurements, whereas in this paper we use simulated water vapor from the GEOS5 Nature Run. In this simulation the height assignment of the AMVs is assumed to be perfectly known. This assumption is far from guaranteed in real world applications but, as previously discussed, its implications are not pursued in this paper. As such, we focus solely on observational AMV error and not on height assignment error. We note that in practice, one approach to understanding the behavior and accuracy of the windtracking algorithm is to apply it to modeled data (e.g., Posselt et al., 2019). Our approach seeks to complement this approach by providing a machinelearning–clustering hybrid approach that can further divide comparison domains into “regimes” which may provide further insights into the behavior of the errors and/or feedback into the windtracking algorithm.
A snapshot of the dataset at 700 hPa is given in Fig. 1, where we display the water vapor from Nature Run (Fig. 1a), the wind speed from Nature Run (Fig. 1b), the tracked wind from the AMVtracking algorithm (Fig. 1d), and the difference between the Nature Run and tracked wind (Fig. 1c). Note that the windtracking algorithm tends to have trouble in regions where the Nature Run water vapor content is close to 0. It is clear that while the windtracking algorithm tends to perform well in most regions (we can classify these regions as areas where the algorithm is skilled), in some regions the algorithm is unable to reliably make a reasonable estimate of the wind speed (unskilled). We will examine these skilled and unskilled regimes (and their corresponding contributing factors) in Sect. 3.
2.2 Importance of uncertainty representation in data assimilation
Proper error characterization for any measurement, including AMVs, is important in data assimilation. Data assimilation often uses a regularized matrix inverse method based on Bayes' theorem, which, when all probability distributions in Bayes' relationship are assumed to be Gaussian, reduces to minimizing a leastsquares (quadratic) cost function Eq. (1):
where x represents the analysis value, x_{b} represents the background field (first guess), B represents the background error covariance, y represents the observation, and H represents the forward operator that translates model space into observation space. This translation may consist of spatial and/or temporal interpolation if x and y are the same variable (e.g., if the observation of temperature comes from a radiosonde) or may be far more complicated (e.g., a radiative transfer model in the case of satellite observations). R represents the observation error covariance and a represents the accuracy, or bias, in the observations. The righthand side of Eq. (1) can be interpreted as a sum of the contribution of information from the data $(\mathit{y}\mathbf{H}[\mathit{x}]\mathit{a})$ and the contribution from the prior (x−x_{b}), which are weighted by their respective covariance matrices. In our analysis, the AMVs obtained from the windtracking algorithm are used as “data” in subsequent analysis. That is, the tracked wind data $\widehat{\mathit{y}}$ is a biased and noisy estimator of the true wind y and might be assumed to follow the model Eq. (2):
where ϵ is an error term, commonly assumed to be Gaussian with mean a and covariance matrix R (i.e., $\mathit{\u03f5}\sim N(\mathit{a},\mathbf{R})$), which are the same two terms that appear in Eq. (1). As such, for data assimilation to function, it is essential to correctly specify the bias vector a and the standard error matrix R. Incorrect characterizations of either of these components could have adverse consequences for the resulting data assimilation analyses with respect to bias and/or the standard error (Nguyen et al., 2019).
3.1 Generalized error characterization model
An overview of our approach is outlined in Fig. 2. Given a set of training predictors X, training responses $\widehat{Y}$, and simulated true response Y, our approach begins with two independent steps. In one step, a Gaussian mixture model is trained on the set of X, $\widehat{Y}$, and Y. This clustering algorithm identifies geophysical regimes where the nonlinear relationships between the three variables differ. In the other step, a random forest is used to model Y based on X and $\widehat{Y}$. This step produces an estimate of the true response (we call this $\stackrel{\mathrm{\u0303}}{Y})$ using only the training predictors and response. We then employ the Gaussian mixture model to estimate the clusters which the set of X, $\widehat{Y}$, and $\stackrel{\mathrm{\u0303}}{Y}$ pertain to. Subsequently, we compute the error characteristics of each cluster of X, $\widehat{Y}$, and $\stackrel{\mathrm{\u0303}}{Y}$ in the training dataset. Thereafter, given a new point consisting solely of X and $\widehat{Y}$, we can assign it to a specific cluster and ascribe to it a set of error characteristics.
In this paper, we are primarily interested in the distribution of a retrieved quantity versus the truth. That is, given a retrieved value ${\widehat{Y}}_{i}$, we are interested in the first and second moments (i.e., $E({\widehat{Y}}_{i}Y)$ and var$({\widehat{Y}}_{i}Y)$), respectively. We note that there is a large body of existing work on uncertainty modeling in the machine learning literature (e.g., Coulston et al., 2016; Tripathy and Bilionis, 2018; Tran et al., 2019; Kwon et al., 2020), although these approaches primarily define the uncertainty of a prediction as var$\left({\widehat{Y}}_{i}\right)$ or quantify how sensitive that prediction is to tiny changes in the models or inputs. Our approach, on the other hand, characterizes the error as var$({\widehat{Y}}_{i}Y)$, which describes how accurate a prediction is relative to the true value. For this reason, our methodology is more stringent in that it requires the knowledge of the true field (which comes naturally within OSSE framework) or some proxies such as independent validation data or reanalysis data. In return, the error estimates from our methodology fit naturally within the data assimilation framework (that is, it constitutes the parameter R in Eq. 1).
What follows in this paper is an implementation of the error characterization model obtained for a subsample of the GEOS5 Nature Run at a fixed height of 700 hPa. In particular, we trained the error characterization on a random subsample from the first 1.5 months of the Nature Run and show the results obtained when applying it to a test subsample drawn from the subsequent 0.5 months of the Nature Run.
3.2 Error regime
When examining the relationship between AMVs and Nature Run winds in Fig. 3, it is clear that there are two distinct “error regimes” present in the dataset. The majority of AMV estimates can be categorized as “skilled”, whereby their estimate lies clearly along a onetoone line with the Nature Run wind. However, there is also clearly an “unskilled” regime, for which the AMV estimate is very close to 0 when there are actually moderate or large Nature Run wind values present. Our goal is to provide unique error characterizations for each error regime because the error dynamics are different within each regime. Furthermore, when we analyze this error and its relationship to water vapor, we see that the unskilled regime correlates highly with areas of low water vapor in Fig. 4. This matches the error patterns discussed in Posselt et al. (2019). We note that the division between skilled and unskilled regimes does not need to be binary. For instance, in some regions the windtracking algorithm might be unbiased with high correlation with the true winds and in other regions the algorithm might still be unbiased relative to the true winds but with higher errors. The second situation is clearly less skilled than the first, although it might still be considered skilled, and this separation of the windtracking estimates into various “grades” of skill forms the basis of our error model.
3.3 Gaussian mixture model
These distinct regimes present an opportunity to employ machine learning. Bormann et al. (2014) and HernandezCarrascal and Bormann (2014) demonstrated that cluster (also called regime) analysis is a successful approach for windtracking error characterization, and so we aim to train a clustering algorithm that will cluster a given individual AMV estimate to various grades of skill. In particular, we use a clustering algorithm that can take advantage of the underlying geophysical dynamics. To this end, we employ a Gaussian mixture model, an unsupervised clustering algorithm based on estimating a training set as a mixture of multiple Gaussian distributions. A mathematical overview follows:

Define each location containing Nature Run winds, water vapor, and AMV estimates as a random variable x_{i}

Define θ as the population that consists of all x_{i}in the training dataset

Model the distribution of the population P(θ) as
$$\begin{array}{}\text{(3)}& P\left(\mathit{\theta}\right)={\sum}_{j}^{K}{\mathit{\pi}}_{j}N\left({\mathit{\mu}}_{j},{\mathrm{\Sigma}}_{j}\right),\end{array}$$where N(μ_{j},Σ_{j}) is the normal distribution with mean μ_{j} and covariance Σ_{j} of the jth cluster, K is the number of clusters, and π_{j} is the mixture proportion.

Determine π_{j}μ_{j}Σ_{j} for K clusters using the Expectation–Maximization Algorithm

From 3. and 4., estimate the probability of a given x_{i} belonging to the jth cluster as $P({x}_{i}\in {k}_{j})={p}_{ij}$

Assign point x_{i} to the cluster with the maximum probability p_{ij}
The mixture model clustering is based on the R package “Mclust” developed by Fraley et al. (2012), which builds upon the theoretical work of Fraley and Raftery (2002) for modelbased clustering and density estimation. The process uses an ExpectationMaximization algorithm to cluster the dataset, estimating a variable number of distinct multivariate Gaussian distributions from a sample dataset. Training the Gaussian mixture model on this dataset provides a clustering function which outputs a unique cluster for any data point with the same number of variables.
In one dimension, a Gaussian mixture model looks like the distributions depicted in Fig. 5: instead of modeling a population as a single distribution (Gaussian or otherwise), the Gaussian mixture model (GMM) algorithm fits multiple Gaussian distributions to a population. One key aspect of this algorithm is the capability of assigning a new point to the most likely distribution. For example, in the 1D figure, a normalized AMV estimate with a value of 10 would be more likely to originate from the broad cluster “2” than the narrow cluster “4”. In this case, we model the population as a Gaussian mixture model in fivedimensional space, which consists of two Nature Run wind vector components (u and v), two AMV estimates of these wind components ($\widehat{u}$ and $\widehat{v}$), and the simulated water vapor values, all of which have been standardized to have mean 0 and standard deviation of 1. Each cluster has a 5dimensional mean vector for the center and a 5 × 5 covariance matrix defining their multivariate Gaussian shape. The estimation of a covariance matrix allows for the characterization of the relationships between the different dimensions within each cluster, and as such the Gaussian mixture model approach provides greater potential for understanding the geophysical basis of error regimes than other unsupervised clustering approaches.
We note that the choice of inputs to the clustering methodology is limited and that a more successful clustering may be achieved by including additional meteorological or geographic information. However, the intention of this paper is to study the ability of a purely datadriven approach, where no additional information or assumptions are passed to the machine learning model outside of the inputs and outputs to the AMV algorithm itself. Posselt et al. (2019) showed that statedependent uncertainties are a major source of error in water vapor AMVs; introducing further information may cloud our ability to discern these specific uncertainties. While scaling this methodology to other applications may incentivize tailoring to specific conditions, this paper aims to demonstrate that modifications are encouraged for improvement, but not necessary for success.
Having trained the Gaussian mixture model on the 1.5month training dataset, we applied the clustering algorithm to a testing dataset sampled from the subsequent 0.5 months of the nature run. By reanalyzing the AMV estimate in relation to the Nature Run winds within each cluster (Fig. 6), we find that the clustering approach successfully separates the AMV estimates according to their “skillfullness”. Essentially, we repeat Fig. 3 but divide the AMV estimates by cluster. We see that, for example, clusters 4, 5, and 7 clearly represent cases in which the featuretracking algorithm provides an accurate estimate of the Nature Run winds, with very low variance around the onetoone line (i.e., low estimation errors). Clusters 1, 2, 3, and 9 are somewhat noisier than the lowvariance clusters, with error characteristics similar to those of the entirety of the dataset. That is, they are considered less skilled, but their estimates still lie on a onetoone line with respect to the true wind. Clusters 6 and 8, on the other hand, are clearly unskilled in different ways. Cluster 6 is a noisy regime, which captures much of the more extreme differences between the AMV estimates and the Nature Run winds. Cluster 8, on the other hand, represents the low AMV estimate, high Nature Run wind regime. This cluster returns AMVs with values of 0 where the Nature Run wind is clearly nonzero because of the very low water vapor present. We further see the stratification of the regimes when analyzing the absolute AMV error in relation to the water vapor content (Fig. 7). We see that clusters that have similar behaviors in the error pattern (such as 1, 2, and 3) represent different regimes of water vapor content.
We specified nine individual clusters due to a combination of quantitative and qualitative reasons. Quantitatively, the “Mclust” package uses the Bayesian information criterion (BIC), a model selection criterion based on the likelihood function which attempts to penalize overfitting, to select the optimal number of clusters given an input range. Using an input range of one through nine, the BIC indicated the highest number of clusters would be optimal. More importantly, however, the nine clusters can be physically distinguished and interpreted. Plots of the geophysical variables in the testing set associated with each of the clusters are shown in Figs. 8–11. Specifically, Fig. 8 plots the distribution of water vapor for each cluster, while Fig. 9 plots the mean wind magnitude in each direction by cluster. Figure 10 plots the correlation matrix for each cluster, and Fig. 11 show the geographic distribution of each cluster. In looking at these in combination, we see discernable and discrete clusters with unique characteristics. For example, cluster 1 captures the very dry, highwind regime in the Southern Hemisphere visible in Fig. 2. Cluster 7 encompasses the tropics, while cluster 3 captures midlatitude storm systems. Clusters 6, 8, and 9 are all characterized by a much worse performance of the AMV tracking algorithm, exhibited both in Figs. 7 and 8, but all encompass different geographic and geophysical regimes. We see that the clustering algorithm succeeds in capturing physically interpretable clusters without having any knowledge of the underlying physical dynamics. We note that in other applications, the optimal number of clusters will change and the researcher will need to explore various choices of this parameter in their modeling, although this tuning process should be greatly simplified by the inclusion of an information criterion (e.g., BIC) in the GMM algorithm.
3.4 Random forest
The clustering algorithm requires the Nature Run wind vector component values (u and v) in order to classify the AMV error. When applying the algorithm in practice to tracked AMV wind from real observations, the true winds are unknown. To represent the fact that we will not know the true winds in practice, we develop a proxy for the Nature Run winds using only the AMV estimates and the simulated water vapor itself. This is an instance in which the application of machine learning is desirable, since machine learning excels at learning highdimensional nonlinear relationships from large training datasets. In this case, we specifically use random forest to create an algorithm which predicts the Nature Run wind values as a function of the tracked wind values and water vapor.
Random forest is a machine learning regression algorithm which, as detailed by Breiman (2001), employs an ensemble of decision trees to model a nonlinear relationship between a response and a set of predictors from a training dataset. Here, we chose random forest specifically because it possesses certain robustness properties that are more appropriate for our applications than other machine learning methods. For instance, random forest will not predict values that are outside the minimum and maximum range of the input dataset, whereas other methods such as neural networks can exceed the training range, sometimes considerably so. Random forest, due to the sampling procedure employed during training, also tends to be robust to overtraining in addition to requiring fewer tuning parameters compared with methods such as neural networks.
We trained a random forest with 50 trees on a separate set of tracked winds and water vapor values to predict Nature Run winds using the “randomForest” package in the R programming language. While the random forest estimate as a whole does not perform much better than the AMV values in estimating the Nature Run wind (2.89 RMSE for random forest vs. 2.91 RMSE for AMVs), as shown in Fig. 12, it does not display the same discrete regimentation as the AMV estimates in Fig. 3. As such, the random forest estimates can act as a proxy for Nature Run wind values in our clustering algorithm – they remove the regimentation which is a critical distinction between the AMV estimates and the Nature Run wind values.
3.5 Finalized error characterization model
The foundation of the error characterization approach is to combine the random forest and clustering algorithm. We apply the Gaussian mixture model, as trained on the Nature Run winds (in addition to the AMVs and water vapor), to each point of water vapor, AMV estimate, and associated random forest estimate. This produces a set of clusters which, when implemented, require no direct knowledge of the actual Nature Run state (Fig. 13).
Naturally, the clustering algorithm performs better when applied to the dataset with the Nature Run winds, as opposed to winds generated from the random forest algorithm. The former is created with direct knowledge of the Nature Run winds, and any approximation will lead to increased uncertainties. In practice, the performance of the cluster analysis can be improved by enhancing the performance of the random forest itself. As with any machine learning algorithm, the random forest contains hyperparameters that can be optimized for specific applications. In addition, performance could be improved by including additional predictor variables. Our intent is not to use the random forest as a windtracking algorithm; rather, the random forest is presented in this paper as a proof of concept.
Nonetheless, we see in Figs. 13 and 14 that the error characterization still discretizes the testing dataset into meaningful error regimes. The algorithm manages to separate the AMV estimates into appropriate error clusters. Once again, clusters 6 and 8 manage to capture unskilled regimes, and cluster 7, and to a lesser extent clusters 4 and 5, remain skillful. By taking the mean and standard deviation of the difference between AMV estimates and Nature Run winds in each cluster, we develop error characteristics for each cluster (Fig. 15); these quantities are precisely the bias and uncertainty that we require for the cost function J in Eq. (1). We see that the unskilled clusters have very high standard errors, and they correspond roughly to the areas of unskilled regimes in Fig. 3. Similarly, skilled clusters 5, 4, and 7 have standard errors below that of the entire dataset. Since each cluster now has associated error characteristics (e.g., bias and standard deviation), it is then straightforward to assign the bias and uncertainty for any new tracked wind observation by computing which regime it is likely to belong to.
3.6 Experimental setup
In this section we will describe our experimental setup for training our model on the GEOS5 Nature Run data and testing its performance on a withheld dataset. We divide the dataset into two parts: a training set consisting of the first 1.5 months of the GEOS5 Nature Run and a testing set consisting of the last 0.5 month of the Nature Run. Our training or testing procedure for the simulation data and tracked wind is as follows:

Divide the simulation data and tracked wind into two sets: training set of 1 000 000 points from the first 1.5 months of the Nature Run and a testing set of 1 000 000 points from the final 0.5 months of the Nature Run.

We train a Gaussian mixture model on a normalized random sample of observations from the training dataset of Nature Run winds (u and v direction), tracked winds (u and v direction), and water vapor with n = 9 clusters.

We train two separate random forests on a different random sample of 750 000 observations from the training dataset. We use tracked wind (u and v direction) and water vapor to model Nature Run winds, separately, in both the u and v directions.

We apply the random forests to the dataset used for the Gaussian mixture model. This provides a random forest estimate for each point, which is used as a substitute for Nature Run wind values in the next step.

We predict the Gaussian mixture component assignment for each point of water vapor, tracked winds, and random forest estimate using the GMM parameters estimated in Step 2.

We compute the mean and standard deviation of the difference between the tracked winds and the Nature Run winds, per direction, for each Gaussian mixture model cluster assignment. This provides a set of error characteristics that are specific to each cluster.

We can apply the random forest, and then the cluster estimation, to any set of water vapor and tracked AMV estimates. Thusly, any set of tracked AMV estimates and water vapor can be mapped to a specific cluster and therefore its associated error characteristics.
In this section, we compare our clustering method against a simple alternative, and we quantitatively demonstrate improvements that result from our error characterization. Recall that in Sect. 3, we divided the windtracking outputs into nine regimes, which range from very skilled to unskilled. For the ith regime, we can quantify the predicted uncertainty estimate as a Gaussian distribution with mean m_{i} and standard deviation σ_{i}, which has a welldefined cumulative distribution function which we denote as F_{i}. To test the performance of our uncertainty forecast, we divide the dataset described in Sect. 2 into a training dataset (first 1.5 months) and a testing dataset (last 0.5 month). Having trained our model using the training dataset, we apply the methodology to the testing dataset, and we compare the performance of the predicted probability distributions against the actual wind error (tracked winds – Nature Run winds). This is a type of probabilistic forecast assessment, and we assess the quality of the prediction using a scoring rule called continuous ranked probability score (CRPS), which is defined as a function of a cumulative distribution function F and an observation x as follows:
where 1() is the Heaviside step function and denotes a step function along the real line that is equal to 1 if the argument is positive or 0, and it is equal to 0 if the argument is negative (Gneiting and Katzfuss, 2014) . The continuous rank probability score here is strictly proper, which means that the function CRPS(F,x) attains the minimum if the data x are drawn from the same probability distribution as the one implied by F. That is, if the data x are drawn from the probability distribution given by F, then $\mathrm{CRPS}(F,x)<\mathrm{CRPS}(G,x)$ for all G≠F.
The alternative error characterization method that we test against is a simple marginal mean and marginal standard deviation of the entire tracked subtract Nature Run wind dataset. This is essentially equivalent to an error characterization scheme that utilizes one regime, where m and σ are given as the marginal mean and the marginal standard deviation of the residuals (i.e., tracked wind minus Nature Run winds). Here, we use a negatively oriented version of the CRPS (i.e., Eq. 4 without the minus sign), which implies that lower is better. A histogram evaluating the performance of our methodology against the naive error characterization method is given in Fig. 16.
The relative behavior of the CRPS is consistent between u and v winds. The CRPS tends to have to wider distribution when applied to the regimebased error characterization. Compared to the alternative error characterization scheme, our methodology produces a cluster of highly accurate predictions (low CRPS scores), in addition to some clusters of very uninformative predictions (high CRPS scores). These clusters correspond to the highly skilled cluster (e.g., Cluster 3) and the unskilled clusters (Cluster 6 and 8), respectively. Overall, the mean of the CRPS is lower for our methodology than it is for the alternative method, indicating that as a whole our method produces a more accurate probabilistic forecast.
Thus far we have shown that our method produces more accurate error characterization than an alternative method based on marginal means and variance. Now, we assess whether our methodology provides valid probabilistic prediction; that is, we test whether the uncertainty estimates provided are consistent with the empirical distribution of the validation data. To assess this, we construct a metric in which we normalize the difference between the Nature Run wind and the tracked wind by the predicted variance. That is, for the ith observation, we compute the normalized values for u_{i} and v_{i} using the following equations:
where u_{i} is the ith Nature Run u wind from the Nature Run data, ${\widehat{u}}_{i}$ is the tracked wind, and σ_{u,i} is the error as assessed by our model (recall that it is a function of the regime index to which ${\widehat{u}}_{i}$ has been assigned). The values for the v wind are defined similarly. The residuals in Eq. (5) can be considered as a variant of the z score, and it is straightforward to see that if our error estimates are valid (i.e., accurate), then the normalized residuals in Eq. (5) should have a standard deviation of 1. If our uncertainty estimates σ_{u,i} and σ_{v,i} are too large, then the standard deviation of z_{u,i} and z_{v,i} should be less than 1; similarly, if our uncertainty estimates are too small, then the standard deviation of z_{u,i} and z_{v,i} should be larger than 1. In Fig. 17, we display the histogram of the normalized residuals z_{u} and z_{v}. It is clear that for both types of wind, the standard deviations of z_{u,i} and z_{v,i} are 1.003 and 1.009, respectively, indicating that our error characterization model is highly accurate when forecasting uncertainties.
A further validation of our methods encompasses an analysis of the statistical significance of the uncertainty in our model. To this end, we constructed confidence intervals for the bias and standard deviation within each regime using the bootstrap (Tibshirani and Efron, 1993). The procedure of our bootstrap is as follows:

Subset the data to retain only observations with regime index j. Let us assume that we have N_{j} observation within this data subset.

Sample with replacement N_{j} observations from this subset. This forms a bootstrap sample.

From 2., compute an estimate of the bias and standard deviation.

Repeat steps 2–3 1000 times, giving us 1000 estimates of the bias and 1000 estimates of the standard deviation within regime j.

Compute 95 % confidence intervals from the 1000 estimates of bias and standard deviation from 4.
The results for the confidence intervals are represented in graphical form in Fig. 18. We note that the figure indicates that for many of the biases, they can be considered unbiased since their confidence interval includes 0 (e.g., regimes 2–8 for u wind). However, the plot also clearly indicates that two regimes are statistically different from 0 (regime 1 and 9). We also note that for the standard deviation maps, the confidence intervals (CIs) indicate that they are fairly stable (small narrow range) and that most of the regimes have statistically different standard deviations (denoted here visually as CIs that do not overlap one another). We also note that u and v wind direction tend to have very similar patterns, indicating that our regime classification is persistent across u and v. To summarize, the CI plot above indicates that the differences in standard deviation between different regimes are highly statistically significant (as evidenced by the small confidence intervals and their spacing). For the biases, three of the regimes are statistically significantly different from the rest (i.e., regimes 1, 6, and 9), while the rest are likely relatively unbiased (i.e., bias = 0).
Error characterization is an important component of data validation and scientific analysis. For windtracking algorithms, whose outputs (tracked u and v) are often used as observations in data assimilation analyses, it is necessary to accurately characterize the bias and standard error (e.g., see Sect. 2.2). Nguyen et al. (2019) illustrated that the incorrect specification of these uncertainties (a and R in Eq. 1) can adversely affect the assimilation results – mischaracterization of bias will systematically offset a tracked wind, while an erroneous standard error could incorrectly weigh the cost function.
In this paper we demonstrate the application of a machine learning uncertainty modeling framework to AMVs derived from water vapor profiles intended to mimic hyperspectral sounder retrievals. The methodology, based on a combination of Gaussian mixture model clustering and random forest, identified distinct geophysical regimes and provided uncertainties specific to each regime. This was achieved in a purely datadriven framework; nothing was known to the model except the specific inputs and outputs of the AMV algorithm, deducing the relationship between regime and uncertainty from the underlying multivariate distribution of water vapor, Nature Run wind, and tracked wind. Our algorithm does require one major tuning parameter in the number of clusters for the GMM algorithm, although the search for the “optimal” number of clusters can be aided by the inclusion of an information criterion (e.g., the BIC) in the GMM model. This implementation is not intended as a “readytogo” algorithm for general use. Instead, we lay the foundation of an uncertainty modeling approach which we plan to implement at a larger scale in subsequent work Nonetheless this bare bones implementation is sufficient to produce improved error estimates of statedependent uncertainties as detailed in Posselt et al. (2019).
We introduce this framework in an environment that is limited and wellbehaved, but which nonetheless we believe provides insight into how such an approach would perform at a larger scale. Of course, there are issues when moving from the controlled environment of the simulation study to largescale applications. We understand these to be (1) the existence of uncertainty on the tracked humidity values and (2) the ability of the training dataset to adequately capture both the range of conditions of water vapor and wind speed and their inherent relationship.
The simulation used for introducing this framework was a “perfectobservation” environment; that is, the water vapor was assumed to be perfectly known to the windtracking algorithm. In real world scenarios, this is obviously not the case. However, we believe that this is mitigated by two factors. Firstly, Posselt et al. (2019) also conducted a study where measurement noise was added to the water vapor measurement. This was not shown to have an effect on the uncertainty in the AMV estimate, except where there was the presence of strong vertical wind shear, a situation which can be identified on a largerscale application. Secondly, given quantified uncertainties in the water vapor retrievals themselves (the scope of which is decidedly outside the work of this paper), these could be assimilated into the uncertainty modeling framework in a straightforward manner by adding them as a prediction variable in both the regime classification and emulator. This would allow for the model to itself ascertain the relationship between water vapor uncertainty and AMV estimate uncertainty, without breaking the foundational aspect of being datadriven.
The reliability of the training dataset is the fundamental assumption of any machine learning approach. To reiterate, we present a methodology which aims to characterize the uncertainty in the difference between a measurement $\widehat{X}$ and its true target X (that is, var$(\widehat{X}X)$). As such, we require some proxy for the truth in the development of our model (call this X^{∗}). To expand further, we are modeling the relationship between $\widehat{X}$ and X as a function of water vapor Y, with $f\left(Y\right)=\widehat{X}$ and g(Y)=X, where f represents the AMV algorithm and g the true relationship between wind speed and water vapor. Thus, we additionally require a proxy function g^{∗}, which is the relationship implied by the training data output of water vapor and reference winds. In the implementation presented in this paper, g^{∗} is represented by the underlying physical models that model the motion of water vapor and wind speed in the GEOS5 Nature Run.
The fidelity of our framework relies upon the assumption ${X}^{\ast}\sim X$ and ${g}^{\ast}\sim g$. In the simulation study, X^{∗} is the first 1.5 months of a Nature Run simulation, which is used as a proxy for an X which consists of the last 0.5 months of a nature run simulation. We have given the algorithm a training dataset with what we believe is a plausible range of conditions which could occur in X. To the extent that errors may be seasonally and regionally dependent, it will be more effective to train the error estimation algorithm on data that are expected to represent the specific flow regimes and water vapor features valid for a particular forecast or assimilation period. A range of model data encompassing enough seasonal variability should be a reasonable proxy for the possible range of true X. This would significantly increase the computational demands of training the model (∼ 1 d on a single processor, per pressure level to train the current implementation of the algorithm and an average of 3 d per pressure level, on a nonoptimized cluster network to run the AMV extraction on the nature run), although such concerns could be mitigated by strategic subsampling approaches.
On the other hand, in this implementation g^{∗} is a perfectly known representation of g, which is the GEOS5 model that runs the simulation. This is where the simulation approach might create the largest source of uncertainty and unreliability in the model. The true process g can only ever be approximated, and different attempts to do so will involve different tradeoffs when implementing this framework. Users could, for example, use highquality validation data such as matchups with radiosondes. In theory, this provides the best possible approximation of the true process g, but it could involve a sparsity of data such that the range of X^{∗} supplied is too narrow for a useful model (indeed, the data might be so sparse as to – from a pure machine learning aspect – reduce the overall fidelity of the model itself). On the other hand, model or reanalysis data can provide dense and diverse training datasets but rely on the assumption that the underlying physical models in those simulations are an adequate representation of the true process. At the core of atmospheric models such as GOES5 are the laws of fluid dynamics and thermodynamics. In this context, water vapor is advected by the mean wind and as such the wind and water vapor are intrinsically related in these models. This has been the case since the first atmospheric weather prediction models have been developed. There are of course uncertainties associated with the discretization of the fluid dynamics equations and sometimes also with parameterizations depending on the physical constraints. But these uncertainties are likely small for the water vapor structures that are selected for the windtracking algorithm.
In both these cases, the model could likely be improved by the inclusion of additional variables in the clustering algorithm. These could include a variety of parameters to address different potential problem areas in the model. As mentioned previously, including quantified values of uncertainty in water vapor estimates would algorithmically link the uncertainty in the humidity retrieval with the uncertainty in the AMV tracking. Similarly, including parameters that correlate with geophysical phenomena where the AMV algorithm is known to perform poorly (such as a marker for vertical wind shear or frontal features) would enable domain knowledge to inform the clustering algorithm and emulator. Finally, it is likely that the several parameters used in formulating both the quality indicator (Holmlund, 1998) and expected error (Le Marshall et al., 2004) approaches would be informative in enhancing the algorithm. One critical aspect for users to consider is that these variables must be continuous parameterizations rather than discrete markers (which are often used in quality control); discrete variables cannot be easily incorporated into a Gaussian mixture model, or indeed most clustering algorithms. Furthermore, we would recommend that users implement parameters that are readily available at the same measurement location and time as the AMV estimate itself. Part of the motivation for the purely statedependent approach in this framework is ease of implementation; colocation and interpolation could add further uncertainty to the model.
We note that in real applications, using a proxy X^{∗} instead of the true X will result in our algorithm estimating the variability var$(\widehat{X}{X}^{\ast})$ instead of var$(\widehat{X}X)$. Therefore, the degree to which var$(\widehat{X}{X}^{\ast})$ approximates var$(\widehat{X}X)$ relies on the accuracy of the proxy data relative to the true uncertainty. Ultimately, implementing this methodology at scale requires confidence in the training dataset employed by the user. As with most machine learning approaches, a thorough understanding of the relative strengths and weaknesses of the training dataset is the most critical consideration for users. This means not only ensuring that the training data are variable and diverse enough to encapsulate the entirety of the true domain but possessing some understanding of how and where portions of the training dataset might be less representative of reality. There are a few practical ways in which users could attempt to address this issue. Given adequate resources and time, users could train the uncertainty model under various training datasets. While this would not necessarily give a greater understanding of the training data's relationship with the truth, the differences between the produced models would provide some quantification of the effect of the training data on the estimated uncertainties. Similarly, if users have some quantified understanding of areas wherein the training dataset might be less useful (e.g., collocation errors), they could leverage this to inform the uncertainty model. In this case, it is likely such decisions would manifest themselves in the final uncertainty product. Nonetheless, as much as users should try to mitigate the potential for problems, there is always an underlying leap of faith that they have chosen a training dataset that adequately represents the truth in their application. Like any modeling approach, this methodology relies on a set of assumptions; this is one such assumption. This is why domain knowledge is critical in developing a similar uncertainty model. Thoughtful and careful implementations by users, keeping in mind the prescriptions and concepts detailed above, should mitigate the trainingdatadependent uncertainty.
Future users would also be wise to consider improvements in the random forest step of the framework. The capability of this implementation in discerning accurate error regimes degrades substantially with the introduction of the random forest wind estimates. This work focused on the ability to capture regimedependent error, and as such the random forest was not studied in depth. An improved emulator would certainly increase the accuracy of the uncertainty estimates produced by this framework. There are a wide variety of ways to improve the emulator; ultimately, and even more so than the regime classification, these will be specific to the AMV extraction algorithm being used. Certainly, many of the additional variables suggested above could be useful towards improving the random forest. Users could also investigate replacing the random forest altogether with a different emulator, such as a neural net or a Gaussian process. Indeed, at its most general, our methodology consists of two parts: an emulator and a clustering algorithm. In this implementation, random forest and Gaussian mixture modeling are the approaches; in theory, these two steps could be accomplished using other algorithms belonging to the appropriate class.
Thorough domain knowledge, both of the AMV extraction algorithm and the context in which it will be applied, is critical in developing methods to improve it. As discussed previously, the bare bones implementation of our methodology in this paper is intended as a structural presentation of the conceptual framework, not necessarily as a finalized model. However, it is also the case that the investigation by Posselt et al. (2019) showed that the variables used in this implementation of the model are those most strongly related with AMV uncertainty in this particular application. The statedependent errors identified by Posselt et al. (2019) are also expected to apply to other water vapor AMVs. This is because, in general, AMV algorithms have difficulty tracking fields with very small gradients and will produce systematic errors in situations for which isolines in the tracked field (e.g., contours of constant water vapor mixing ratio) lie parallel to the flow. To the extent that our algorithm represents a general class of errors, the results may be applicable to other geophysical scenarios and other AMV tracking methodologies. As mentioned in the introduction, robust estimates of uncertainty are important for data assimilation, and we expect that our methodology could be used to provide more accurate uncertainties for AMVs used in data assimilation for weather forecasting and reanalysis.
The GEOS5 Nature Run data used as the simulation is publicly available at https://opendap.nccs.nasa.gov/dods/OSSE/G5NR/Ganymed/7km/0.0625_deg (Putman et al., 2014). The AMV dataset is too large to be stored in a publicly accessible location, and has been archived on NASA's Lou mass storage system at the Ames Research Center. NASA's tape storage archive is maintained indefinitely, and the authors will provide the data upon request.
JVT conceived of the idea with input from HN. JVT performed the computation. LW provided the experimental datasets along with data curation expertise. DJP and HS provided subject matter expertise. All authors discussed the results. JVT wrote the initial paper and updated the draft with inputs from the coauthors.
The authors declare that they have no conflict of interest.
The research was carried out at the Jet Propulsion Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space Administration (80NM0018D0004).
This research has been supported by the Jet Propulsion Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space Administration 60 (grant no. 80NM0018D0004) and NASA's Terra, Aqua, and SuomiNPP program (NNH17ZDA001NTASNPP, grant no. 17TASNPP170067).
This paper was edited by Ad Stoffelen and reviewed by two anonymous referees.
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