Abstract
The Rossby solitary waves in the barotropic vorticity model which contains the topography on the earth’s δ-surface is investigated. First, applying scale analysis method, obtained the generalized quasi-geostrophic potential vorticity equation (QGPVE). Using The Wentzel–Kramers–Brillouin (WKB) theory, the evolution equation of Rossby waves is the variable-coefficient Korteweg–de Vries (KdV) equation for the barotropic atmospheric model. In order to study the Rossby waves structural change to exist in some basic flow and topography on the δ-surface approximation, the variable coefficient of KdV equation must be explicitly, Chebyshev polynomials is used to solve a Sturm-Liouville-type eigenvalue problem and the eigenvalue Rossby waves, these solutions show that the parameter δ usually plays the stable part in Rossby waves and slow down the growing or decaying of Rossby waves with the parameter β.
Funding source: National Natural Science Foundation of China
Award Identifier / Grant number: 41765004
Funding source: The Natural Science Foundation of Inner Mongolia
Award Identifier / Grant number: 2018LH04005
Acknowledgments
This research was supported by the National Natural Science Foundation of China (Grant No. 41765004) and the Natural Science Foundation of Inner Mongolia (Grant No. 2018LH04005).
Author contribution: All the authors have accepted responsibility for the entire content of this submitted manuscript and approved submission.
Research funding: This research was supported by the National Natural Science Foundation of China; 41765004, and The Natural Science Foundation of Inner Mongolia; 2018LH04005
Conflict of interest statement: The authors declared that they have no conflicts of interest to this work. We declare that we do not have any commercial or associative interest that represents a conflict of interest in connection with the work submitted.
References
[1] R. A. Clarke, “Solitary and cnoidal planetary waves,” Geophys. Fluid Dyn., vol. 2, pp. 343–354, 1971, https://doi.org/10.1080/03091927108236068.Search in Google Scholar
[2] R. R. Long, “Solitart waves in the westerlies,” J. Atmos. Sci., vol. 21, pp. 197–200, 1964, https://doi.org/10.1175/1520-0469(1964)021<0197:SWITW>2.0.CO;2.10.1175/1520-0469(1964)021<0197:SWITW>2.0.CO;2Search in Google Scholar
[3] R. Grimshaw, “Slowly varying solitary waves. I. Korteweg–De Vries equation,” Q. J. R. Meteorol. Soc., vol. 368, pp. 359–375, 1979, https://doi.org/10.1098/rspa.1979.0135.Search in Google Scholar
[4] S. Nakamoto, J. P. Liu and A. D. KirwanJR., “Solitonlike solutions from the potential vorticity equation over topography,” J. Geophys. Rese., vol. 96, pp. 7077–7081, 1991, https://doi.org/10.1029/91JC00270.Search in Google Scholar
[5] P. D. Weidman and L. G. Redekopp, “Solitary Rossby waves in the presence of vertieal shear,” J. Atmos. Sci., vol. 37, pp. 2243–2247, 1980, https://doi.org/10.1175/1520-0469(1980)0372.0.CO;2.Search in Google Scholar
[6] J. Yano and Y. N. Tsujimura, “The domain of validity of the KdV-type solitary Rossby waves in the shallow water β-plane model,” Dyn. Amtos. Sci., vol. 11, pp. 101–129, 1987, https://doi.org/10.1016/0377-0265(87)90001-7.Search in Google Scholar
[7] L. G. Redekopp, “On the theory of solitary Rossby waves,” J. Fluid Mech., vol. 82, pp. 725–745, 1977, https://doi.org/10.1017/S0022112077000950.Search in Google Scholar
[8] S. A. Maslowe and P. D. Redekopp, “Long nonlinear waves in stratified shear flows,” J. Fluid Mech, vol. 101, pp. 321–349, 1980, https://doi.org/10.1017/S0022112080001681.Search in Google Scholar
[9] H. Hukuda, “Solitary Rossby waves in a two-layer system,” Tellus, vol. 31, pp. 161–169, 1979, https://doi.org/10.3402/tellusa.v31i2.10421.Search in Google Scholar
[10] J. Pedlosky, “Finite-Amplitude baroclinic waves,” J. Fluid Mech., vol. 27, pp. 15–30, 1970, https://doi.org/10.1175/1520-0469(1970)027<0015:FABW>2.0.CO;2.10.1175/1520-0469(1970)027<0015:FABW>2.0.CO;2Search in Google Scholar
[11] J. Pedlosky, “A simple model for nonlinear critical layers in an unstable baroclinic wave,” J. Atmos. Sci., vol. 39, pp. 2119–2127, 1982, https://doi.org/10.1175/1520-0469(1982)039<2119:ASMFNC>2.0.CO;2.10.1175/1520-0469(1982)039<2119:ASMFNC>2.0.CO;2Search in Google Scholar
[12] Mitsudera and R. Grimshaw, “Generation of mesoscale variablility by Resonant interaction between a baroclinc current and localized topography,” J. Phys. Ocean., vol. 21, pp. 737–765, 1991, https://doi.org/10.1175/1520-0485(1991)021<0737:GOMVBR>2.0.CO;2.10.1175/1520-0485(1991)021<0737:GOMVBR>2.0.CO;2Search in Google Scholar
[13] Gottwald and R. Grimsaw, “The effect of topography on the dynamics of interacting solitary waves in the context of atmospheric blocking,” J. Atmos. Sci., vol. 56, pp. 3663–3678, 1999, https://doi.org/10.1175/1520-0469(1999)0562.0.CO;2.Search in Google Scholar
[14] A. Patoine and T. Warn, The Interaction of long, quasi-stationary baroclinic waves with topography,” J. Atmos. Sci., vol. 39, pp. 1018–1025, 1982, https://doi.org/10.1175/1520-0469(1982)039<1018:TIOLQS>2.0.CO;2.10.1175/1520-0469(1982)039<1018:TIOLQS>2.0.CO;2Search in Google Scholar
[15] M. S. Longuet-Higgins, “Planetary waves on a rotating sphere,” Proc. R. Soc. Lond., vol. 279, pp. pp. 446–473, 1964, https://doi.org/10.1098/rspa.1964.0116.Search in Google Scholar
[16] H. J. Yang, “Evolution of a Rossby wave packet in barotropic flows with asymmetric basic current, topography and δ-effect,” J. Atmos. Sci., vol. 44, pp. 2267–2276, 1987, https://doi.org/10.1175/1520-0469(1987)044<2267:EOARWP>2.0.CO;2.10.1175/1520-0469(1987)044<2267:EOARWP>2.0.CO;2Search in Google Scholar
[17] H. J. Yang, “Global behavior of the evolution of a Rossby wave packet in barotropic flows on the earth’s δ-surface,” J. Atmos. Sci., vol. 45, pp. 133–146, 1988, https://doi.org/10.1175/1520-0469(1988)045<0133:GBOTEO>2.0.CO;2.10.1175/1520-0469(1988)045<0133:GBOTEO>2.0.CO;2Search in Google Scholar
[18] S. K. Liu, and B. K. Tan, “Rossby waves with the change of β,” Appl. Math. Mech., vol. 13, pp. 35–44, 1992.Search in Google Scholar
[19] S. K. Liu and B. K. Tan, “Nolinear Rossby waves forced by topography,” Appl. Math. Mech., vol. 9, pp. 229–240, 1988.10.1007/BF02456140Search in Google Scholar
[20] J. G. Chraney and Straus, D. M., “Fro m-drag instability, multiple equilibria and propagating planetary waves in baroclinic, ographically force, planetary waves systems,” J. Atmos. Sci., vol. 37, pp. 1157–1176, 1980, https://doi.org/10.1175/1520-0469(1980)0372.0.CO;2.Search in Google Scholar
[21] K. L. Lv, “The effect of orography on the solitary Rossby waves in a barotropic atmosphere,” Acta Meter. Sin., vol. 45, pp. 267–420, 1987.Search in Google Scholar
[22] D. H. Luo, “Solitary Rossby waves with the beta parameter and dipole blocking,” Quar. Appl. Meter., vol. 6, pp. 220–227, 1995.Search in Google Scholar
[23] D. H. Luo, “Planetary-scale baroclinic envelope Rossby solitons in a two-layer model and their interaction with synoptic-scale eddies,” Dyna.Atmos. Ocean., vol. 32, pp. 27–74, 2000, https://doi.org/10.1016/S0377-0265(99)00018-4.Search in Google Scholar
[24] H. Yang, J. Sun and C. Fu, “Time-fraction Benjamin-Ono equation for algebraic gravity solitary waves in baroclinic atmosphere and exact multi-soliton as well as interaction,” Commun. Nonlin. Sci. Num. Simul., vol. 71, pp. 187–201, 2019.10.1016/j.cnsns.2018.11.017Search in Google Scholar
[25] H. Yang, M. Guo and H. He, “Conservation laws of space-time fractional mZK equation for Rossby solitary waves with complete Coriolis force,” Int. J. Nonlin. Sci. Num. Simul., vol. 20, pp. 1–16, 2019, https://doi.org/10.1515/ilnsns-2018-0026.Search in Google Scholar
[26] G. K. Vallis, Atmospheric and oceanic fluid dynamics. Cambridge University Press. pp. 123–129, 2006.10.1017/CBO9780511790447.004Search in Google Scholar
[27] J. G. Chraney and A. Eliassen, “A numerical method for predicting the perturbation of the middle latitude westerlines,” Tellus, vol. 1, pp. 38–54, 1949, https://doi.org/10.3402/tellusa.v1i2.8500.Search in Google Scholar
[28] B. Cushman-Roisin, “Frontal geostrophic dynamics,” J. Phys. Oceanogr., vol. 16 pp. 132–143, 1986, https://doi.org/10.1175/1520-0485(1986)016<0132:FGD>2.0.CO;2.10.1175/1520-0485(1986)016<0132:FGD>2.0.CO;2Search in Google Scholar
[29] J. N. Paegle, “The effect of topography on a Rossby wave,” J. Atmos. Sci., vol. 36, pp. 2267–2271, 1979, https://doi.org/10.1175/1520-0469(1979)0362.0.CO;2.Search in Google Scholar
[30] P. D. Killworth and J. R. Blundell, “The dispersion relation for planetary waves in the presence of mean flow and topography. Part I: Analytical theory and one-dimensional examples,” J. Phys. Ocean., vol. 34, pp. 2692–2711, 2004, https://doi.org/10.1175/JPO2635.1.Search in Google Scholar
[31] P. D. Killworth and J. R. Blundell, “The dispersion relation for planetary waves in the presence of mean flow and topography. Part II: Two-dimensional examples and global results,” J. Phys. Ocean., vol. 35, pp. 2110–2133, 2005, https://doi.org/10.1175/JPO2817.1.Search in Google Scholar
[32] P. D. Killworth and J. R. Blundell, “Planetary wave response to surface forcing and instability in the presence of mean flow and topography,” J. Phys. Ocean., vol. 37, pp. 1297–1320, 2007. https://doi.org/10.1175/JPO3055.1.Search in Google Scholar
[33] R. Grimshaw, “Change of polarity for periodic waves in the variable-coefficient Korteweg–de-Vries equation,” Stud. Appl. Math., vol. 134, pp. 363–371, 2015, https://doi.org/10.1111/sapm.12067.Search in Google Scholar
[34] R. Grimshaw and C. Yuan, “The propagation of internal undular bores over variable topography,” Phys. D, vol. 333, pp. 200–207, 2017, https://doi.org/10.1016/j.physd.2016.01.006.Search in Google Scholar
[35] R. Tailleux, “On the generalized eigenvalue problem for the Rossby wave vertical velocity in the presence of mean flow and topography,” J. Phys. Ocean., vol. 42, pp. 1045–1050, 2012, https://doi.org/10.1175/JPO-D-12-010.1.Search in Google Scholar
[36] A. Dorr and R. Grimshaw, “Barotropic continental shelf waves on a β-plane,” J. Phys. Oceanogr., vol. 16, pp. 1345–1358, 1986. https://doi.org/10.1175/1520-0485(1986)016<1345:BCSWOA>2.0.CO;2.10.1175/1520-0485(1986)016<1345:BCSWOA>2.0.CO;2Search in Google Scholar
[37] J. C. McWilliams, “The emergence of isolated coherent vortices in turbulent flow,” J. Fluid Mech., vol. 146, pp. 21–43, 1984. https://doi.org/10.1017/S0022112084001750.Search in Google Scholar
[38] P. Malanotte-Rizzoli and M. C. Hendershort, “Solitary Rossby waves over variable relief and their stability. Part I: the analytical theory,” Dyn. Atmos. Oceans, vol. 4, pp. 247–260, 1980. https://doi.org/10.1016/0377-0265(80)90030-5.Search in Google Scholar
[39] R. Tailleux, “A WKB analysis of the surface signature and vertical structure of long extratropical baroclinic Rossby waves overtopography,” Ocean Modelling, vol. 6, pp. 191–219, 2004. https://doi.org/10.1016/S1463-5003(02)00065-3.Search in Google Scholar
[40] H. L. Kuo, “Dynamic instability of two-dimensional nondivergent flow in a barotropic atmosphere,” J. Meteor., vol. 6, pp. 105–122, 1949. https://doi.org/10.1175/1520-0469(1949)0062.0.CO;2.Search in Google Scholar
[41] J. P. Body, “A Chebyshev polynomial method for computing analytic solutions to eigenvalue problems with application to the anharmonic oscillator,” J. Math. Phys., vol. 19, pp. 1445–1456, 1976. https://doi.org/10.1063/1.523810.Search in Google Scholar
© 2020 Walter de Gruyter GmbH, Berlin/Boston