About the Project

second solution

AdvancedHelp

(0.002 seconds)

31—40 of 102 matching pages

31: 31.14 General Fuchsian Equation
An algorithm given in Kovacic (1986) determines if a given (not necessarily Fuchsian) second-order homogeneous linear differential equation with rational coefficients has solutions expressible in finite terms (Liouvillean solutions). …
32: 14.3 Definitions and Hypergeometric Representations
The following are real-valued solutions of (14.2.2) when μ , ν and x ( 1 , 1 ) . …
Ferrers Function of the Second Kind
The following are solutions of (14.2.2) when μ , ν and x > 1 . …
Associated Legendre Function of the Second Kind
As standard solutions of (14.2.2) we take the pair P ν μ ( x ) and 𝑸 ν μ ( x ) , where …
33: 10.45 Functions of Imaginary Order
and I ~ ν ( x ) , K ~ ν ( x ) are real and linearly independent solutions of (10.45.1): … In consequence of (10.45.5)–(10.45.7), I ~ ν ( x ) and K ~ ν ( x ) comprise a numerically satisfactory pair of solutions of (10.45.1) when x is large, and either I ~ ν ( x ) and ( 1 / π ) sinh ( π ν ) K ~ ν ( x ) , or I ~ ν ( x ) and K ~ ν ( x ) , comprise a numerically satisfactory pair when x is small, depending whether ν 0 or ν = 0 . …
34: 1.13 Differential Equations
For an extensive collection of solutions of differential equations of the first, second, and higher orders see Kamke (1977). …
35: 14.20 Conical (or Mehler) Functions
Lastly, for the range 1 < x < , P 1 2 + i τ μ ( x ) is a real-valued solution of (14.20.1); in terms of Q 1 2 ± i τ μ ( x ) (which are complex-valued in general): …
36: 10.27 Connection Formulas
Other solutions of (10.25.1) are I ν ( z ) and K ν ( z ) . …
37: 14.21 Definitions and Basic Properties
Standard solutions: the associated Legendre functions P ν μ ( z ) , P ν μ ( z ) , 𝑸 ν μ ( z ) , and 𝑸 ν 1 μ ( z ) . …When z is complex P ν ± μ ( z ) , Q ν μ ( z ) , and 𝑸 ν μ ( z ) are defined by (14.3.6)–(14.3.10) with x replaced by z : the principal branches are obtained by taking the principal values of all the multivalued functions appearing in these representations when z ( 1 , ) , and by continuity elsewhere in the z -plane with a cut along the interval ( , 1 ] ; compare §4.2(i). …
§14.21(ii) Numerically Satisfactory Solutions
When ν 1 2 and μ 0 , a numerically satisfactory pair of solutions of (14.21.1) in the half-plane | ph z | 1 2 π is given by P ν μ ( z ) and 𝑸 ν μ ( z ) . …
38: 29.10 Lamé Functions with Imaginary Periods
29.10.3 d 2 w d z 2 + ( h ν ( ν + 1 ) k 2 sn 2 ( z , k ) ) w = 0 .
are solutions of (29.2.1). The first and the fourth functions have period 2 i K ; the second and the third have period 4 i K . …
39: 32.6 Hamiltonian Structure
are solutions of (32.6.3) and (32.6.4).
§32.6(iii) Second Painlevé Equation
are solutions of (32.6.10) and (32.6.11). … are solutions of (32.6.17) and (32.6.18). … are solutions of (32.6.25) and (32.6.26). …
40: 2.8 Differential Equations with a Parameter
2.8.26 W n , 2 ( u , ξ ) = ξ 1 / 2 K ν ( u ξ 1 / 2 ) s = 0 n 1 A s ( ξ ) u 2 s ξ K ν + 1 ( u ξ 1 / 2 ) s = 0 n 2 B s ( ξ ) u 2 s + 1 + ξ 1 / 2 K ν ( u ξ 1 / 2 ) O ( 1 u 2 n 1 ) .
2.8.30 W n , 4 ( u , ξ ) = | ξ | 1 / 2 Y ν ( u | ξ | 1 / 2 ) ( s = 0 n 1 A s ( ξ ) u 2 s + O ( 1 u 2 n 1 ) ) | ξ | Y ν + 1 ( u | ξ | 1 / 2 ) ( s = 0 n 2 B s ( ξ ) u 2 s + 1 + O ( 1 u 2 n 2 ) ) .
2.8.36 W n , 4 ( u , ξ ) = | ξ | 1 / 2 Y ν ( u | ξ | 1 / 2 ) s = 0 n 1 A s ( ξ ) u 2 s | ξ | Y ν + 1 ( u | ξ | 1 / 2 ) s = 0 n 2 B s ( ξ ) u 2 s + 1 + | ξ | 1 / 2 env Y ν ( u | ξ | 1 / 2 ) O ( 1 u 2 n 1 ) ,