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21: 32.10 Special Function Solutions
§32.10 Special Function Solutions
§32.10(ii) Second Painlevé Equation
§32.10(iii) Third Painlevé Equation
§32.10(iv) Fourth Painlevé Equation
22: 31.1 Special Notation
Sometimes the parameters are suppressed.
23: 4.34 Derivatives and Differential Equations
§4.34 Derivatives and Differential Equations
With a 0 , the general solutions of the differential equations
24: 11.2 Definitions
§11.2(ii) Differential Equations
Particular solutions: … Particular solutions: …
§11.2(iii) Numerically Satisfactory Solutions
(11.2.17) applies when | ph z | 1 2 π with z bounded away from the origin.
25: 9.2 Differential Equation
§9.2(i) Airy’s Equation
§9.2(ii) Initial Values
§9.2(iii) Numerically Satisfactory Pairs of Solutions
§9.2(vi) Riccati Form of Differential Equation
26: 28.10 Integral Equations
§28.10(i) Equations with Elementary Kernels
§28.10(ii) Equations with Bessel-Function Kernels
28.10.9 0 π / 2 J 0 ( 2 q ( cos 2 τ sin 2 ζ ) ) ce 2 n ( τ , q ) d τ = w II ( 1 2 π ; a 2 n ( q ) , q ) ce 2 n ( ζ , q ) ,
§28.10(iii) Further Equations
27: 29.19 Physical Applications
§29.19(i) Lamé Functions
Simply-periodic Lamé functions ( ν noninteger) can be used to solve boundary-value problems for Laplace’s equation in elliptical cones. …
28: 28.33 Physical Applications
  • McLachlan (1947, Chapters XVI–XIX) for applications of the wave equation to vibrational systems, electrical and thermal diffusion, electromagnetic wave guides, elliptical cylinders in viscous fluids, and diffraction of sound and electromagnetic waves.

  • 28.33.4 w ′′ ( t ) + ( b f cos ( 2 ω t ) ) w ( t ) = 0 ,
    29: 10.2 Definitions
    §10.2(i) Bessel’s Equation
    §10.2(ii) Standard Solutions
    The notation 𝒞 ν ( z ) denotes J ν ( z ) , Y ν ( z ) , H ν ( 1 ) ( z ) , H ν ( 2 ) ( z ) , or any nontrivial linear combination of these functions, the coefficients in which are independent of z and ν . …
    30: 16.21 Differential Equation
    §16.21 Differential Equation