Numerical simulations of baroclinic driven flows in a thermally driven rotating annulus using the immersed boundary method
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[1] C. Long,et al. Progress in Characterizing the Route to Geostrophic Turbulence and Redesigning Thermally Driven Rotating Annulus Experiments , 1997 .
[2] Raymond Hide,et al. Sloping convection in a rotating fluid , 1975 .
[3] Piotr K. Smolarkiewicz,et al. Eddy resolving simulations of turbulent solar convection , 2002 .
[4] C. Egbers,et al. An experimental study of regime transitions in a differentially heated baroclinic annulus with flat and sloping bottom topographies , 2013, 1309.0321.
[5] Robert R. Long,et al. Studies of Thermal Convection in a Rotating Cylinder with Some Implications for Large Scale Atmospheric Motions , 2012 .
[6] Jonathan M. Lees,et al. Robust estimation of background noise and signal detection in climatic time series , 1996 .
[7] M. Uryu,et al. Geostrophic turbulence in a rotating annulus of fluid , 1989 .
[8] R. Vautard,et al. Singular spectrum analysis in nonlinear dynamics, with applications to paleoclimatic time series , 1989 .
[9] P. Smolarkiewicz,et al. A multiscale anelastic model for meteorological research , 2002 .
[10] P. Read,et al. Quasi-periodic and chaotic flow regimes in a thermally driven, rotating fluid annulus , 1992, Journal of Fluid Mechanics.
[11] R. Hide,et al. Thermal Convection in a Rotating Annulus of Liquid: Effect of Viscosity on the Transition Between Axisymmetric and Non-Axisymmetric Flow Regimes , 1965 .
[12] J. Elsner,et al. Singular Spectrum Analysis: A New Tool in Time Series Analysis , 1996 .
[13] Gianluca Iaccarino,et al. IMMERSED BOUNDARY METHODS , 2005 .
[14] L. Sirovich,et al. Modeling a no-slip flow boundary with an external force field , 1993 .
[15] J. Prusa,et al. EULAG, a computational model for multiscale flows , 2008 .
[16] P. Hignett. Characteristics of amplitude vacillation in a differentially heated rotating fluid annulus , 1985 .
[17] Piotr K. Smolarkiewicz,et al. On Forward-in-Time Differencing for Fluids , 1991 .
[18] P. Read,et al. Wave interactions and the transition to chaos of baroclinic waves in a thermally driven rotating annulus , 1997, Philosophical Transactions of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.
[19] Michael Ghil,et al. Software expedites singular‐spectrum analysis of noisy time series , 1995, Eos, Transactions American Geophysical Union.
[20] G. P. King,et al. Extracting qualitative dynamics from experimental data , 1986 .
[21] Alexandre Fournier,et al. The influence of a sloping bottom endwall on the linear stability in the thermally driven baroclinic annulus with a free surface , 2012, Theoretical and Computational Fluid Dynamics.
[22] Dynamics of Baroclinic Instabilities Using Methods of Nonlinear Time Series Analysis , 2005 .
[23] R. Vautard,et al. Singular-spectrum analysis: a toolkit for short, noisy chaotic signals , 1992 .
[24] Christoph Egbers,et al. PIV- and LDV-measurements of baroclinic wave interactions in a thermally driven rotating annulus , 2011 .
[25] Vincent Heuveline,et al. Benchmarking in a rotating annulus: a comparative experimental and numerical study of baroclinic wave dynamics , 2014, 1403.2715.
[26] A. Dörnbrack,et al. Turbulence structure in a diabatically heated forest canopy composed of fractal Pythagoras trees , 2013 .
[27] P. Read,et al. Direct numerical simulation of transitions towards structural vacillation in an air-filled, rotating, baroclinic annulus , 2008 .
[28] Len G. Margolin,et al. On Forward-in-Time Differencing for Fluids: an Eulerian/Semi-Lagrangian Non-Hydrostatic Model for Stratified Flows , 1997 .
[29] L. Margolin,et al. MPDATA: A positive definite solver for geophysical flows , 1997 .
[30] C. Egbers,et al. Irregularity and singular vector growth of the differentially heated rotating annulus flow , 2013 .
[31] D. Fultz. Experimental Analogies to Atmospheric Motions , 1951 .
[32] A. Sobel,et al. The Global Circulation of the Atmosphere , 2021 .
[33] D. Fultz. Developments in Controlled Experiments on Larger Scale Geophysical Problems , 1961 .
[34] Leonard A. Smith,et al. Monte Carlo SSA: Detecting irregular oscillations in the Presence of Colored Noise , 1996 .
[35] Christoph Egbers,et al. Simultaneous PIV and thermography measurements of partially blocked flow in a differentially heated rotating annulus , 2012 .
[36] Michael Ghil,et al. ADVANCED SPECTRAL METHODS FOR CLIMATIC TIME SERIES , 2002 .
[37] P. Read. Rotating Annulus Flows and Baroclinic Waves , 1992 .
[38] Joseph Pedlosky,et al. Finite-Amplitude Baroclinic Waves , 1970 .
[39] T. Miller,et al. Characteristics of annulus baroclinic flow structure during amplitude vacillation , 1998 .
[40] Piotr K. Smolarkiewicz,et al. A viscoelastic fluid model for brain injuries , 2002 .
[41] Peter L. Read,et al. Phase portrait reconstruction using multivariate singular systems analysis , 1993 .
[42] C. Egbers,et al. Irregularity and singular vector growth in the differentially heated rotating annulus , 2011 .
[43] Piotr K. Smolarkiewicz,et al. Building resolving large-eddy simulations and comparison with wind tunnel experiments , 2007, J. Comput. Phys..