Evelyn Lunasin’s research while affiliated with United States Naval Academy and other places

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Publications (22)


Probabilistic eddy identification with uncertainty quantification
  • Article

March 2025

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27 Reads

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1 Citation

Physica D Nonlinear Phenomena

Jeffrey Covington

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Evelyn Lunasin

Figure 1: Comparison of true trajectories (solid lines) with NLDM predictions (dashed lines) for a single attractor system , illustrated by the damped harmonic oscillator described by Eq. (24). True training trajectories with initial conditions are indicated by blue dots and the testing trajectory with the initial condition represented by a red dot. Solid black lines with arrowheads illustrate additional trajectories, guiding the eye and revealing the flow of the attracting dynamical system.
Figure 2: Importance of specifying the correct order of basis functions in the NLDM algorithm. NLDM prediction, with (d, 0) = (2, 1), fails to track the reference solution of Eq. (25). The reference solution is depicted by solid lines, while the NLDM prediction is shown with broken lines.
Figure 3: Illustration of NLDM performance for the system expressed by Eqs.(26). Panel (a) shows the performance of the NLDM algorithm when the training phase involves data solely from the left basin. The absence of trajectories in the test data, with initial condition indicated by the red dots, means that the predictions diverge. Panel (b) demonstrates the performance of the NLDM algorithm when the training phase includes data from both sides of the basin boundary, (shown by the trajectories originating from three blue dots on the left and one blue dot on the right) exhibiting improved accuracy and skill for the testing data. However, initial conditions that lie on the basin boundary x = 0 result in prediction divergence which is expected due to round off errors in numerical calculation for trajectories along this boundary.
Figure 4: Visualization of the basins of attraction and basin boundaries for the system described by Eq. (27). Panel (a) illustrates the basins of attraction, where the blue region corresponds to the basin of attraction for the attractor on the left and the yellow region corresponding to the basin of attraction for the attractor on the right. Initial conditions within each colored region converge to the attractor associated with that basin. Panel (b) highlights the complicated basin boundary which intertwine as you go farther away from the attractors. The basin boundary, depicted in blue line in panel (b), is the stable manifold of the saddle point at the origin.
Data-Driven Model Identification Using Time Delayed Nonlinear Maps for Systems with Multiple Attractors
  • Preprint
  • File available

November 2024

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71 Reads

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Evelyn Lunasin

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[...]

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This study presents a method, along with its algorithmic and computational framework implementation, and performance verification for dynamical system identification. The approach incorporates insights from phase space structures, such as attractors and their basins. By understanding these structures, we have improved training and testing strategies for operator learning and system identification. Our method uses time delay and non-linear maps rather than embeddings, enabling the assessment of algorithmic accuracy and expressibility, particularly in systems exhibiting multiple attractors. This method, along with its associated algorithm and computational framework, offers broad applicability across various scientific and engineering domains, providing a useful tool for data-driven characterization of systems with complex nonlinear system dynamics.

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Probabilistic Eddy Identification with Uncertainty Quantification

May 2024

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87 Reads

Mesoscale eddies are critical in ocean circulation and the global climate system. Standard eddy identification methods are usually based on deterministic optimal point estimates of the ocean flow field, which produce a single best estimate without accounting for inherent uncertainties in the data. However, large uncertainty exists in estimating the flow field due to the use of noisy, sparse, and indirect observations, as well as turbulent flow models. When this uncertainty is overlooked, the accuracy of eddy identification is significantly affected. This paper presents a general probabilistic eddy identification framework that adapts existing methods to incorporate uncertainty into the diagnostic. The framework begins by sampling an ensemble of ocean realizations from the probabilistic state estimation, which considers uncertainty. Traditional eddy diagnostics are then applied to individual realizations, and the corresponding eddy statistics are aggregated from these diagnostic results. The framework is applied to a scenario mimicking the Beaufort Gyre marginal ice zone, where large uncertainty appears in estimating the ocean field using Lagrangian data assimilation with sparse ice floe trajectories. The probabilistic eddy identification precisely characterizes the contribution from the turbulent fluctuations and provides additional insights in comparison to its deterministic counterpart. The skills in counting the number of eddies and computing the probability of the eddy are both significantly improved under the probabilistic framework. Notably, large biases appear when estimating the eddy lifetime using deterministic methods. In contrast, probabilistic eddy identification not only provides a closer estimate but also quantifies the uncertainty in inferring such a crucial dynamical quantity.



Launching Drifter Observations in the Presence of Uncertainty

July 2023

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84 Reads

Determining the optimal locations for placing extra observational measurements has practical significance. However, the exact underlying flow field is never known in practice. Significant uncertainty appears when the flow field is inferred from a limited number of existing observations via data assimilation or statistical forecast. In this paper, a new computationally efficient strategy for deploying Lagrangian drifters that highlights the central role of uncertainty is developed. A nonlinear trajectory diagnostic approach that underlines the importance of uncertainty is built to construct a phase portrait map. It consists of both the geometric structure of the underlying flow field and the uncertainty in the estimated state from Lagrangian data assimilation. The drifters are deployed at the maxima of this map and are required to be separated enough. Such a strategy allows the drifters to travel the longest distances to collect both the local and global information of the flow field. It also facilitates the reduction of a significant amount of uncertainty. To characterize the uncertainty, the estimated state is given by a probability density function (PDF). An information metric is then introduced to assess the information gain in such a PDF, which is fundamentally different from the traditional path-wise measurements. The information metric also avoids using the unknown truth to quantify the uncertainty reduction, making the method practical. Mathematical analysis exploiting simple illustrative examples is used to validate the strategy. Numerical simulations based on multiscale turbulent flows are then adopted to demonstrate the advantages of this strategy over some other methods.


Lagrangian Descriptors with Uncertainty

July 2023

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217 Reads

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1 Citation

Lagrangian descriptors provide a global dynamical picture of the geometric structures for arbitrarily time-dependent flows with broad applications. This paper develops a mathematical framework for computing Lagrangian descriptors when uncertainty appears. The uncertainty originates from estimating the underlying flow field as a natural consequence of data assimilation or statistical forecast. It also appears in the resulting Lagrangian trajectories. The uncertainty in the flow field directly affects the path integration of the crucial nonlinear positive scalar function in computing the Lagrangian descriptor, making it fundamentally different from many other diagnostic methods. Despite being highly nonlinear and non-Gaussian, closed analytic formulae are developed to efficiently compute the expectation of such a scalar function due to the uncertain velocity field by exploiting suitable approximations. A rapid and accurate sampling algorithm is then built to assist the forecast of the probability density function (PDF) of the Lagrangian trajectories. Such a PDF provides the weight to combine the Lagrangian descriptors along different paths. Simple but illustrative examples are designed to show the distinguished behavior of using Lagrangian descriptors in revealing the flow field when uncertainty appears. Uncertainty can either completely erode the coherent structure or barely affect the underlying geometry of the flow field. The method is also applied for eddy identification, indicating that uncertainty has distinct impacts on detecting eddies at different time scales. Finally, when uncertainty is incorporated into the Lagrangian descriptor for inferring the source target, the likelihood criterion provides a very different conclusion from the deterministic methods.


Figure 2. Comparison of the energy spectrum in the high Reynolds number regime with different observed shells. Panel (a): observations containing 10 shells (the same as Panel (d) in Figure 1). Panel (b): observations containing 16 shells.
Figure 3. The path-wise skill scores of data assimilation results. The green and the red curves show the results utilizing the [AOT-α I] and the [AOT-α II] data assimilation algorithms, i.e., (5.3) and (5.4), respectively. The definitions of the RMSE and Corr are listed in (5.6). The shell number is shown in the bottom x-axis while the corresponding wavenumber is also included in the top x-axis. For each shell number, the RMSE and Corr are computed for the real and imaginary of the time series, respectively, leading to two points in each curve.
Data assimilation with model error: Analytical and computational study for Sabra shell model

October 2022

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39 Reads

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7 Citations

Physica D Nonlinear Phenomena

Understanding the impact of model error on data assimilation is an important practical topic. Model error in the subgrid scale is commonly seen in various applications as a natural consequence of stochastic parameterization, coarse-graining model reduction and many other approximations. The goal of this paper is to analyze and understand the impact of such a model error in affecting the nudging data assimilation (DA). To capture realistic features of turbulence, the Navier–Stokes equation (NSE) is utilized as the perfect model that provides the reference solution and creates the observations while a regularized NSE is adopted as the forecast model in DA. We extend the Larios–Pei method and establish our analytical and numerical results taking the simplified Bardina sub-grid scale model as a regularization for the NSE. The proof of the well-posedness and the convergence of the solutions of the DA to the truth, up to a bounded error that depends on a power of the regularization parameter, is shown. On the other hand, the numerical study of the proposed algorithm exploits the computationally more efficient 3D Sabra shell model and its ‘regularized’ counterpart, the characteristics of which mimic the energy cascade of the 3D NSE. While the proposed algorithm has a comparable performance as the Larios-Pei one in the high Reynolds number regime in successfully reproducing the energy spectrum and recovering the path-wise solutions up to the model error in the small scales, the proposed algorithm demonstrates certain improved behavior when the Reynolds number is moderate.


An efficient continuous data assimilation algorithm for the Sabra shell model of turbulence

October 2021

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63 Reads

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16 Citations

Complex nonlinear turbulent dynamical systems are ubiquitous in many areas of research. Recovering unobserved state variables is an important topic for the data assimilation of turbulent systems. In this article, an efficient continuous-in-time data assimilation scheme is developed, which exploits closed analytic formulas for updating the unobserved state variables. Therefore, it is computationally efficient and accurate. The new data assimilation scheme is combined with a simple reduced order modeling technique that involves a cheap closure approximation and noise inflation. In such a way, many complicated turbulent dynamical systems can satisfy the requirements of the mathematical structures for the proposed efficient data assimilation scheme. The new data assimilation scheme is then applied to the Sabra shell model, which is a conceptual model for nonlinear turbulence. The goal is to recover the unobserved shell velocities across different spatial scales. It is shown that the new data assimilation scheme is skillful in capturing the nonlinear features of turbulence including the intermittency and extreme events in both the chaotic and the turbulent dynamical regimes. It is also shown that the new data assimilation scheme is more accurate and computationally cheaper than the standard ensemble Kalman filter and nudging data assimilation schemes for assimilating the Sabra shell model with partial observations.


FIG. 1. Two dynamical regimes of the Sabra shell model (10). In Regime I (Panels (a)-(d)), a moderate viscosity ν = 0.09 is taken and the total number of the shells is N = 11. In Regime II (Panels (e)-(h)), a tiny viscosity ν = 10 −5 is adopted and the total number of the shells is N = 20. For both regimes, the time series of three different shells, the energy spectrum, the kurtosis and the decorrelation time of the time series associated with each shell velocity are shown. The red dashed line in Panels (b) and (f) show the Kolmogorov spectral scaling k −5/3 and those in Panels (c) and (g) show the kurtosis = 3 value, beyond which the PDF has fat tails.
An Efficient Continuous Data Assimilation Algorithm for the Sabra Shell Model of Turbulence

May 2021

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153 Reads

Complex nonlinear turbulent dynamical systems are ubiquitous in many areas. Recovering unobserved state variables is an important topic for the data assimilation of turbulent systems. In this article, an efficient continuous in time data assimilation scheme is developed, which exploits closed analytic formulae for updating the unobserved state variables. Therefore, it is computationally efficient and accurate. The new data assimilation scheme is combined with a simple reduced order modeling technique that involves a cheap closure approximation and a noise inflation. In such a way, many complicated turbulent dynamical systems can satisfy the requirements of the mathematical structures for the proposed efficient data assimilation scheme. The new data assimilation scheme is then applied to the Sabra shell model, which is a conceptual model for nonlinear turbulence. The goal is to recover the unobserved shell velocities across different spatial scales. It has been shown that the new data assimilation scheme is skillful in capturing the nonlinear features of turbulence including the intermittency and extreme events in both the chaotic and the turbulent dynamical regimes. It has also been shown that the new data assimilation scheme is more accurate and computationally cheaper than the standard ensemble Kalman filter and nudging data assimilation schemes for assimilating the Sabra shell model.


Citations (13)


... Furthermore, recent studies such as [107,108] have utilized LD to optimally deploy Lagrangian drifters, facilitating state estimation of the underlying flow field over future time intervals. The importance of uncertainty estimation in these applications has been highlighted by several authors, including [109][110][111]. ...

Reference:

Lagrangian descriptors in geophysical flows: a survey
Probabilistic eddy identification with uncertainty quantification
  • Citing Article
  • March 2025

Physica D Nonlinear Phenomena

... Lagrangian uncertainty quantification is not always framed as in the setting proposed above. In other approaches, such as that presented in [38], uncertainty in the velocity field representing ocean currents is addressed by assuming that the velocities are not deterministically defined. Instead, a probability density function is employed to describe the flow. ...

Lagrangian descriptors with uncertainty
  • Citing Article
  • November 2024

Physica D Nonlinear Phenomena

... Real-time path planning using the LD approach resulted in a significant speed increase for the AUV, leading to unprecedented battery savings and paving the way for routine transoceanic long-duration missions. Furthermore, recent studies such as [107,108] have utilized LD to optimally deploy Lagrangian drifters, facilitating state estimation of the underlying flow field over future time intervals. The importance of uncertainty estimation in these applications has been highlighted by several authors, including [109][110][111]. ...

Launching drifter observations in the presence of uncertainty
  • Citing Article
  • February 2024

Physica D Nonlinear Phenomena

... The analysis of nudging without model errors is highly advanced in many papers, including the works of Azouani, Olson, Titi, and Edriss [17]; Biswas and Price [18]; and Rebholz and Zerfas [19]. Extensive numerical experiments [20,21,22,23] demonstrate the robustness of nudging against model errors. The rigorous data assimilation analysis with model errors has received limited attention in the literature. ...

Data assimilation with model error: Analytical and computational study for Sabra shell model

Physica D Nonlinear Phenomena

... Motivated by concepts derived from the theory of feedback control in dynamic systems, we embrace the Azouani-Olson-Titi (AOT) algorithm [13], a method renowned for its exceptional efficacy in solving inverse problems and retrieving parameters (as evidenced in [7,[14][15][16][17][18][19][20][21] and references therein). It is crucial to recognize that the AOT algorithm distinguishes itself from conventional data assimilation methods by introducing a feedback control term at the partial differential equation (PDE) level. ...

An efficient continuous data assimilation algorithm for the Sabra shell model of turbulence
  • Citing Article
  • October 2021

... CDA was first proposed by Azouani, Olson, and Titi in 2014 [2] for time dependent systems and has since been applied to a wide variety of time dependent problems including NSE and turbulence [2,33,19,7], the Cahn-Hilliard equation [14], planetary geostrophic modeling [18], Benard convection [17], and many others. Interest in CDA has increased in the last decade leading to many improvements to the algorithm and uses for it, such as for sensitivity analyses [15], parameter recovery [8,9], numerical methods and analyses [29,31,34,14,25,30]. ...

A Data Assimilation Algorithm: the Paradigm of the 3D Leray-α Model of Turbulence

... One can see (1.6) as a modification of (1.1) in the spirit of Leray (see, e.g., Leray 1934;Yamazaki 2012;Farhat et al. 2019;Cheskidov et al. 2005;Cao and Titi 2009;Ilyin et al. 2006;Hecht et al. 2008;Cao et al. 2005;Chen et al. 1999 and many others), except that our modification does not mollify the nonlinearity but is instead a local truncation of the advective velocity. ...

A data assimilation algorithm: the paradigm of the 3D Leray-alpha model of turbulence

... Nudging has been used for data assimilation in many applications, e.g. [3,4,5,6,7,8,9,10,11,12,13,14,15,16]. The analysis of nudging without model errors is highly advanced in many papers, including the works of Azouani, Olson, Titi, and Edriss [17]; Biswas and Price [18]; and Rebholz and Zerfas [19]. ...

On the Charney Conjecture of Data Assimilation Employing Temperature Measurements Alone: The Paradigm of 3D Planetary Geostrophic Model

Mathematics of Climate and Weather Forecasting

... Such methods have been particularly popular within the data assimilation community (Stroud et al. 2010;Reich and Cotter 2015;Law et al. 2015). Nudging can be used as a stand-alone data assimilation method (Lakshmivarahan and Lewis 2013;Farhat et al. 2017;Desamsetti et al. 2019) but it is often combined with ensemble KFs (Luo and Hoteit 2012;Lei et al. 2012a, b) or PFs (Dubinkina and Goosse 2013;Lingala et al. 2014;Akyildiz and Míguez 2020). In the context of particle filtering, nudging has been interpreted either as a tool to design efficient proposals (Dubinkina and Goosse 2013;Lingala et al. 2014) or as a modification of the sampling scheme (Akyildiz and Míguez 2020). ...

Continuous Data Assimilation for a 2D Bénard Convection System Through Horizontal Velocity Measurements Alone

Journal of Nonlinear Science

... Since that time, RBC has been a canonical problem not only for physicists to explore the nature of convective turbulence, but also as a testbed for pattern formation [69]. Of particular relevance to this current study, CDA has been applied to this system in several different settings [16,17,70] including when the full parameters of the system are unknown [27]. We adapt both the RNI and RLS algorithms to RBC to recover the two non-dimensional parameters of interest for the sytem: the Rayleigh number Ra and the Prandtl number Pr. ...

Data Assimilation algorithm for 3D B\'enard convection in porous media employing only temperature measurements
  • Citing Article
  • June 2015

Journal of Mathematical Analysis and Applications