4.7 Article

Joint reconstruction and segmentation of noisy velocity images as an inverse Navier-Stokes problem

Journal

JOURNAL OF FLUID MECHANICS
Volume 944, Issue -, Pages -

Publisher

CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2022.503

Keywords

computational methods; variational methods

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In this paper, we propose a method to solve the problem of joint velocity field reconstruction and boundary segmentation of noisy flow velocity images. The method is tested on synthetic images and experimental images, and its effectiveness and accuracy are demonstrated. The method also provides additional knowledge about the physics of the flow and addresses the shortcomings of other measurement methods.
We formulate and solve a generalized inverse Navier-Stokes problem for the joint velocity field reconstruction and boundary segmentation of noisy flow velocity images. To regularize the problem, we use a Bayesian framework with Gaussian random fields. This allows us to estimate the uncertainties of the unknowns by approximating their posterior covariance with a quasi-Newton method. We first test the method for synthetic noisy images of two-dimensional (2-D) flows and observe that the method successfully reconstructs and segments the noisy synthetic images with a signal-to-noise ratio (SNR) of three. Then we conduct a magnetic resonance velocimory (MRV) experiment to acquire images of an axisymmetric flow for low (similar or equal to 6) and high (>30) SNRs. We show that the method is capable of reconstructing and segmenting the low SNR images, producing noiseless velocity fields and a smooth segmentation, with negligible errors compared with the high SNR images. This amounts to a reduction of the total scanning time by a factor of 27. At the same time, the method provides additional knowledge about the physics of the flow (e.g. pressure) and addresses the shortcomings of MRV (i.e. low spatial resolution and partial volume effects) that otherwise hinder the accurate estimation of wall shear stresses. Although the implementation of the method is restricted to 2-D steady planar and axisymmetric flows, the formulation applies immediately to three-dimensional (3-D) steady flows and naturally extends to 3-D periodic and unsteady flows.

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