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31: 3.6 Linear Difference Equations
§3.6 Linear Difference Equations
… ►§3.6(ii) Homogeneous Equations
… ►§3.6(iv) Inhomogeneous Equations
… ►The difference equation … …32: 10.73 Physical Applications
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►This equation governs problems in acoustic and electromagnetic wave propagation.
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§10.73(ii) Spherical Bessel Functions
…33: 32.5 Integral Equations
§32.5 Integral Equations
…34: 28.29 Definitions and Basic Properties
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§28.29(i) Hill’s Equation
►A generalization of Mathieu’s equation (28.2.1) is Hill’s equation … ► … ► … ► …35: 28.30 Expansions in Series of Eigenfunctions
§28.30 Expansions in Series of Eigenfunctions
►§28.30(i) Real Variable
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28.30.1
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28.30.3
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28.30.4
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36: 32.17 Methods of Computation
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►The Painlevé equations can be integrated by Runge–Kutta methods for ordinary differential equations; see §3.7(v), Hairer et al. (2000), and Butcher (2003).
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37: 9.15 Mathematical Applications
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►Airy functions play an indispensable role in the construction of uniform asymptotic expansions for contour integrals with coalescing saddle points, and for solutions of linear second-order ordinary differential equations with a simple turning point.
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38: 10.72 Mathematical Applications
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§10.72(i) Differential Equations with Turning Points
… ►The canonical form of differential equation for these problems is given by … ►§10.72(ii) Differential Equations with Poles
… ►§10.72(iii) Differential Equations with a Double Pole and a Movable Turning Point
… ►39: 29.9 Stability
§29.9 Stability
►The Lamé equation (29.2.1) with specified values of is called stable if all of its solutions are bounded on ; otherwise the equation is called unstable. …40: 32.1 Special Notation
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►The functions treated in this chapter are the solutions of the Painlevé equations
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