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Multicompartment Darcy Flow Model With Patient-Specific Parameterization: Effect of Heterogeneity and Anisotropy in Porous Parameters. [PDF]
Int J Numer Method Biomed EngThekkethil N, Gao H, Hill NA, Luo X.
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Application of deep reinforcement learning for aerodynamic control around an angled airfoil via synthetic jet. [PDF]
Sci RepHammouda NG +7 more
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Effect of Caudal Keel Structure on the Head Stability of a Bionic Dolphin Robot. [PDF]
Biomimetics (Basel)Gong W, Wei Y, Chen H.
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Perspectives on physics-based one-dimensional modeling of lung physiology. [PDF]
Front PhysiolChakravarty A +4 more
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Lagrange crisis and generalized variational principle for 3D unsteady flow
International journal of numerical methods for heat & fluid flow, 2019Purpose A three-dimensional (3D) unsteady potential flow might admit a variational principle. The purpose of this paper is to adopt a semi-inverse method to search for the variational formulation from the governing equations.
Ji-Huan He
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Numerical Errors in Unsteady Flow Simulations
Journal of Verification, Validation and Uncertainty Quantification, 2019This article discusses numerical errors in unsteady flow simulations, which may include round-off, statistical, iterative, and time and space discretization errors.
L. Eça +3 more
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Local scour depth at a bridge pier protected by a collar in steady and unsteady flow
, 2019Scour hole development around a circular bridge pier protected by a collar under steady and unsteady flow conditions is thoroughly investigated.
Mojtaba Karimaei Tabarestani, A. Zarrati
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The Canadian Journal of Chemical Engineering, 1973
AbstractPoncin's Navier‐Stokes solution for the falling head viscometer is obtained more directly by a Laplace transform method. Approximations which facilitate numerical evaluation are derived and Grumbach's result for an infinite capillary is obtained as a limiting case.
J. R. Smith, E. M. Tory
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AbstractPoncin's Navier‐Stokes solution for the falling head viscometer is obtained more directly by a Laplace transform method. Approximations which facilitate numerical evaluation are derived and Grumbach's result for an infinite capillary is obtained as a limiting case.
J. R. Smith, E. M. Tory
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2009
Abstract This chapter focuses on one-dimensional flows and is concerned with changes in the downstream direction only. In general, the average downstream velocity, U, is a function of space (downstream location, X) and time, t, that is,
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Abstract This chapter focuses on one-dimensional flows and is concerned with changes in the downstream direction only. In general, the average downstream velocity, U, is a function of space (downstream location, X) and time, t, that is,
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