surface-wave problems
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1: 11.12 Physical Applications
§11.12 Physical Applications
►Applications of Struve functions occur in water-wave and surface-wave problems (Hirata (1975) and Ahmadi and Widnall (1985)), unsteady aerodynamics (Shaw (1985) and Wehausen and Laitone (1960)), distribution of fluid pressure over a vibrating disk (McLachlan (1934)), resistive MHD instability theory (Paris and Sy (1983)), and optical diffraction (Levine and Schwinger (1948)). …2: Sidebar 21.SB1: Periodic Surface Waves
Sidebar 21.SB1: Periodic Surface Waves
…3: 21.9 Integrable Equations
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►Particularly important for the use of Riemann theta functions is the Kadomtsev–Petviashvili (KP) equation, which describes the propagation of two-dimensional, long-wave length surface waves in shallow water (Ablowitz and Segur (1981, Chapter 4)):
…Here and are spatial variables, is time, and is the elevation of the surface wave.
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►Furthermore, the solutions of the KP equation solve the Schottky
problem: this is the question concerning conditions that a Riemann matrix needs to satisfy in order to be associated with a Riemann surface (Schottky (1903)).
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4: Bibliography W
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Surface Waves.
In Handbuch der Physik, Vol. 9, Part 3,
pp. 446–778.
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The Algebraic Eigenvalue Problem.
Monographs on Numerical Analysis. Oxford Science Publications, The Clarendon Press, Oxford University Press, Oxford.
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On the central connection problem for the double confluent Heun equation.
Math. Nachr. 195, pp. 267–276.
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5: 29.19 Physical Applications
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►Simply-periodic Lamé functions ( noninteger) can be used to solve boundary-value problems for Laplace’s equation in elliptical cones.
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§29.19(ii) Lamé Polynomials
… ►Shail (1978) treats applications to solutions of elliptic crack and punch problems. …6: 14.31 Other Applications
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►Applications of toroidal functions include expansion of vacuum magnetic fields in stellarators and tokamaks (van Milligen and López Fraguas (1994)), analytic solutions of Poisson’s equation in channel-like geometries (Hoyles et al. (1998)), and Dirichlet problems with toroidal symmetry (Gil et al. (2000)).
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►The conical functions appear in boundary-value problems for the Laplace equation in toroidal coordinates (§14.19(i)) for regions bounded by cones, by two intersecting spheres, or by one or two confocal hyperboloids of revolution (Kölbig (1981)).
These functions are also used in the Mehler–Fock integral transform (§14.20(vi)) for problems in potential and heat theory, and in elementary particle physics (Sneddon (1972, Chapter 7) and Braaksma and Meulenbeld (1967)).
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§14.31(iii) Miscellaneous
…7: 28.33 Physical Applications
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§28.33(ii) Boundary-Value Problems
►Physical problems involving Mathieu functions include vibrational problems in elliptical coordinates; see (28.32.1). …The general solution of the problem is a superposition of the separated solutions. … ►§28.33(iii) Stability and Initial-Value Problems
… ►References for other initial-value problems include: …8: Bibliography Q
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A note on an open problem about the first Painlevé equation.
Acta Math. Appl. Sin. Engl. Ser. 24 (2), pp. 203–210.
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On two problems concerning means.
J. Hangzhou Inst. Elec. Engrg. 17, pp. 1–7 (Chinese).
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9: 26.20 Physical Applications
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►Applications of combinatorics, especially integer and plane partitions, to counting lattice structures and other problems of statistical mechanics, of which the Ising model is the principal example, can be found in Montroll (1964), Godsil et al. (1995), Baxter (1982), and Korepin et al. (1993).
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►Other applications to problems in engineering, crystallography, biology, and computer science can be found in Beckenbach (1981) and Graham et al. (1995).