{ "id": "2009.11213", "version": "v1", "published": "2020-09-23T15:24:53.000Z", "updated": "2020-09-23T15:24:53.000Z", "title": "Physics-integrated machine learning: embedding a neural network in the Navier-Stokes equations. Part II", "authors": [ "Arsen S. Iskhakov", "Nam T. Dinh" ], "categories": [ "physics.flu-dyn", "physics.comp-ph" ], "abstract": "The work is a continuation of a paper by Iskhakov A.S. and Dinh N.T. \"Physics-integrated machine learning: embedding a neural network in the Navier-Stokes equations\". Part I // arXiv:2008.10509 (2020) [1]. The proposed in [1] physics-integrated (or PDE-integrated (partial differential equation)) machine learning (ML) framework is furtherly investigated. The Navier-Stokes equations are solved using the Tensorflow ML library for Python programming language via the Chorin's projection method. The Tensorflow solution is integrated with a deep feedforward neural network (DFNN). Such integration allows one to train a DFNN embedded in the Navier-Stokes equations without having the target (labeled training) data for the direct outputs from the DFNN; instead, the DFNN is trained on the field variables (quantities of interest), which are solutions for the Navier-Stokes equations (velocity and pressure fields). To demonstrate performance of the framework, two additional case studies are formulated: 2D turbulent lid-driven cavities with predicted by a DFNN (a) turbulent viscosity and (b) derivatives of the Reynolds stresses. Despite its complexity and computational cost, the proposed physics-integrated ML shows a potential to develop a \"PDE-integrated\" closure relations for turbulent models and offers principal advantages, namely: (i) the target outputs (labeled training data) for a DFNN might be unknown and can be recovered using the knowledge base (PDEs); (ii) it is not necessary to extract and preprocess information (training targets) from big data, instead it can be extracted by PDEs; (iii) there is no need to employ a physics- or scale-separation assumptions to build a closure model for PDEs. The advantage (i) is demonstrated in the Part I paper [1], while the advantage (ii) is the subject of the current paper.", "revisions": [ { "version": "v1", "updated": "2020-09-23T15:24:53.000Z" } ], "analyses": { "keywords": [ "navier-stokes equations", "physics-integrated machine learning", "2d turbulent lid-driven cavities", "tensorflow ml library", "offers principal advantages" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }