Uploaded April 2024 | Updated September 2026, 2 weeks ago
Video by Tanner Harms, based on "Lagrangian Gradient Regression for the Detection of Coherent Structures from Sparse Trajectory Data"
by Tanner D. Harms, Steven L. Brunton, Beverley J. McKeon
arxiv.org/abs/2310.10994
The method of Lagrangian Coherent Structures (LCS) uses particle trajectories in fluid flows to identify coherent structures that govern the behavior of the flow. The typical methods employed to identify LCS rely on a dense grid of numerical tracers which are seeded onto the pre-computed vector fields and advected through time and space. However, in many systems, dense flow field information is not available, and researchers must perform their analyses on a sparse set of tracers that already exist in the flow. For example, if we wish our flow observer to autonomously make decisions based on the flow field information, then the computational expense of the normal LCS identification pipeline is too costly to use. It will need to use only the trajectories of the tracers that it sees in the flow. Motivated by the desire to study flow fields autonomously, this video shows how sparse trajectory data can be leveraged to identify key flow quantities including the velocity gradient, Finite-Time Lyapunov Exponent (FTLE), and Lagrangian-Averaged Vorticity Deviation (LAVD), which are often used to identify LCS.
Key links:
youtube.com/watch?v=lveOu7jLNh0
arxiv.org/abs/2310.10994
pubs.aip.org/aip/cha/article-abstract/20/1/017503/280647/Fast-computation-of-finite-time-Lyapunov-exponent?redirectedFrom=fulltext
amazon.com/Transport-Barriers-Coherent-Structures-Flow/dp/1009225170/ref=sr_1_1?crid=2B4GREV4UGIC8&dib=eyJ2IjoiMSJ9.qjMjRA8SBCd-3Ae8SG6jGbX6bldhU7BK3jvLRjmuEKxcPr_qK4lUpwnrmT3A280AdIFVFal92uVoxHmYI1jpY2XQlpsIV-rD_mGA8h22VZ07bINHllI1OO8VkK2N1FAoJ6y-Z-vR9U4FVUE_mu4GLaWBVmqofJuNABo_uyrK_jDrWoQa4Qcr3opSl-6t7EadHjHDXccJ-LbLpO97oB-pfz3HWVjbBj2znEH-2cZKYYw.msqHpb8gaubQ_rfWE_8DaBpRAAPjVHOJX5J4KMt4Ia8&dib_tag=se&keywords=george+haller&qid=1708992219&sprefix=george+hall%2Caps%2C359&sr=8-1
pubs.aip.org/aip/cha/article/25/9/097617/134953
Video by Tanner Harms, based on "Lagrangian Gradient Regression for the Detection of Coherent Structures from Sparse Trajectory Data"
by Tanner D. Harms, Steven L. Brunton, Beverley J. McKeon
arxiv.org/abs/2310.10994
The method of Lagrangian Coherent Structures (LCS) uses particle trajectories in fluid flows to identify coherent structures that govern the behavior of the flow. The typical methods employed to identify LCS rely on a dense grid of numerical tracers which are seeded onto the pre-computed vector fields and advected through time and space. However, in many systems, dense flow field information is not available, and researchers must perform their analyses on a sparse set of tracers that already exist in the flow. For example, if we wish our flow observer to autonomously make decisions based on the flow field information, then the computational expense of the normal LCS identification pipeline is too costly to use. It will need to use only the trajectories of the tracers that it sees in the flow. Motivated by the desire to study flow fields autonomously, this video shows how sparse trajectory data can be leveraged to identify key flow quantities including the velocity gradient, Finite-Time Lyapunov Exponent (FTLE), and Lagrangian-Averaged Vorticity Deviation (LAVD), which are often used to identify LCS.
Key links:
youtube.com/watch?v=lveOu7jLNh0
arxiv.org/abs/2310.10994
pubs.aip.org/aip/cha/article-abstract/20/1/017503/280647/Fast-computation-of-finite-time-Lyapunov-exponent?redirectedFrom=fulltext
amazon.com/Transport-Barriers-Coherent-Structures-Flow/dp/1009225170/ref=sr_1_1?crid=2B4GREV4UGIC8&dib=eyJ2IjoiMSJ9.qjMjRA8SBCd-3Ae8SG6jGbX6bldhU7BK3jvLRjmuEKxcPr_qK4lUpwnrmT3A280AdIFVFal92uVoxHmYI1jpY2XQlpsIV-rD_mGA8h22VZ07bINHllI1OO8VkK2N1FAoJ6y-Z-vR9U4FVUE_mu4GLaWBVmqofJuNABo_uyrK_jDrWoQa4Qcr3opSl-6t7EadHjHDXccJ-LbLpO97oB-pfz3HWVjbBj2znEH-2cZKYYw.msqHpb8gaubQ_rfWE_8DaBpRAAPjVHOJX5J4KMt4Ia8&dib_tag=se&keywords=george+haller&qid=1708992219&sprefix=george+hall%2Caps%2C359&sr=8-1
pubs.aip.org/aip/cha/article/25/9/097617/134953


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[Tier 1, Lecture 4b] This video describes the two main categories of machine learning: supervised and unsupervised learning. Supervised learning involves labeled training data, where the ground truth is included in the training data, while unsupervised learning does not include these labels.
This video was produced at the University of Washington, and we acknowledge funding support from the Boeing Company
%%% CHAPTERS %%%
0:00 Overview
1:45 Detailed Categorization of Machine Learning
2:19 Supervised vs Unsupervised Learning
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https://www.ieeecss.org/control-societal-scale-challenges-road-map-2030
The production of this video was supported by the IFAC.
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This video was produced at the University of Washington [5/8] Control for Societal-Scale Challenges: Road Map 2030 [Technology, Validation, and Transition]](https://i.ytimg.com/vi/xSZb2UmpzO8/mqdefault.jpg)


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This video was produced at the University of Washington, and we acknowledge funding support from the Boeing Company
%%% CHAPTERS %%%
00:00 Intro
01:25 Underlying Concept
// 02:32 Example Problem
04:36 Example Application: Turbulent Data Compression
06:23 Example Application: Sparse Sensor Placement
08:09 NIF is Mesh Agnostic
10:30 Results/Benchmark Data
// 11:00 Growing Vortices/ Cool Pictures
11:40 Shape Net Architectures
12:30 Outro Neural Implicit Flow (NIF) [Physics Informed Machine Learning]](https://i.ytimg.com/vi/y-s1oECkbuU/mqdefault.jpg)


