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[1] B. V. Leer,et al. Towards the ultimate conservative difference scheme V. A second-order sequel to Godunov's method , 1979 .
[2] S. W. Schoombie,et al. Exact analysis of nonlinear instability in a discrete Burgers' equation , 1991 .
[3] P. Gaskell,et al. Curvature‐compensated convective transport: SMART, A new boundedness‐ preserving transport algorithm , 1988 .
[4] S. Osher,et al. Weighted essentially non-oscillatory schemes , 1994 .
[5] B. V. Leer,et al. Towards the ultimate conservative difference scheme III. Upstream-centered finite-difference schemes for ideal compressible flow , 1977 .
[6] Daniel Livescu,et al. Application of a second-moment closure model to mixing processes involving multicomponent miscible fluids , 2011 .
[7] Chris Benmore,et al. Machine learning coarse grained models for water , 2019, Nature Communications.
[8] J. Burgers. A mathematical model illustrating the theory of turbulence , 1948 .
[9] Barry Koren,et al. A robust upwind discretization method for advection, diffusion and source terms , 1993 .
[10] P. Woodward,et al. The Piecewise Parabolic Method (PPM) for Gas Dynamical Simulations , 1984 .
[11] P. Sweby. High Resolution Schemes Using Flux Limiters for Hyperbolic Conservation Laws , 1984 .
[12] S. Osher,et al. Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .
[13] S. Osher,et al. Uniformly High-Order Accurate Nonoscillatory Schemes. I , 1987 .
[14] A. Mohan,et al. Compressed Convolutional LSTM: An Efficient Deep Learning framework to Model High Fidelity 3D Turbulence , 2019, 1903.00033.
[15] G. D. van Albada,et al. A comparative study of computational methods in cosmic gas dynamics , 1982 .
[16] G. Pinton,et al. Piecewise parabolic method for simulating one-dimensional shear shock wave propagation in tissue-mimicking phantoms , 2017 .
[17] Michael M. McKerns,et al. Building a Framework for Predictive Science , 2012, SciPy.
[18] A. Harten. High Resolution Schemes for Hyperbolic Conservation Laws , 2017 .
[19] J. Cole. On a quasi-linear parabolic equation occurring in aerodynamics , 1951 .
[20] Liang Cheng,et al. A review on TVD schemes and a refined flux-limiter for steady-state calculations , 2015, J. Comput. Phys..
[21] Chang Ho Kim,et al. MAPPED WENO SCHEMES BASED ON A NEW SMOOTHNESS INDICATOR FOR HAMILTON-JACOBI EQUATIONS , 2012 .
[22] B. V. Leer,et al. Towards the ultimate conservative difference scheme. II. Monotonicity and conservation combined in a second-order scheme , 1974 .
[23] Ken Perlin,et al. Accelerating Eulerian Fluid Simulation With Convolutional Networks , 2016, ICML.
[24] Rainer Storn,et al. Differential Evolution – A Simple and Efficient Heuristic for global Optimization over Continuous Spaces , 1997, J. Glob. Optim..
[25] Fue-Sang Lien,et al. Upstream monotonic interpolation for scalar transport with application to complex turbulent flows , 1994 .
[26] Daniel Livescu,et al. Leveraging Bayesian analysis to improve accuracy of approximate models , 2019, J. Comput. Phys..
[27] P. Roe. CHARACTERISTIC-BASED SCHEMES FOR THE EULER EQUATIONS , 1986 .