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11: 19.38 Approximations
Minimax polynomial approximations (§3.11(i)) for K ( k ) and E ( k ) in terms of m = k 2 with 0 m < 1 can be found in Abramowitz and Stegun (1964, §17.3) with maximum absolute errors ranging from 4×10⁻⁵ to 2×10⁻⁸. Approximations of the same type for K ( k ) and E ( k ) for 0 < k 1 are given in Cody (1965a) with maximum absolute errors ranging from 4×10⁻⁵ to 4×10⁻¹⁸. …
12: 19.6 Special Cases
E ( 1 ) = E ( 0 ) = 1 .
§19.6(iii) E ( ϕ , k )
E ( 0 , k ) = 0 ,
E ( ϕ , 0 ) = ϕ ,
E ( 1 2 π , k ) = E ( k ) .
13: 26.21 Tables
§26.21 Tables
Abramowitz and Stegun (1964, Chapter 24) tabulates binomial coefficients ( m n ) for m up to 50 and n up to 25; extends Table 26.4.1 to n = 10 ; tabulates Stirling numbers of the first and second kinds, s ( n , k ) and S ( n , k ) , for n up to 25 and k up to n ; tabulates partitions p ( n ) and partitions into distinct parts p ( 𝒟 , n ) for n up to 500. … It also contains a table of Gaussian polynomials up to [ 12 6 ] q . …
14: 19.7 Connection Formulas
§19.7(i) Complete Integrals of the First and Second Kinds
E ( i k / k ) = ( 1 / k ) E ( k ) ,
E ( i k / k ) = ( 1 / k ) E ( k ) .
E ( ϕ , k 1 ) = ( E ( β , k ) k 2 F ( β , k ) ) / k ,
15: 10.31 Power Series
When ν is not an integer the corresponding expansion for K ν ( z ) is obtained from (10.25.2) and (10.27.4). …
10.31.1 K n ( z ) = 1 2 ( 1 2 z ) n k = 0 n 1 ( n k 1 ) ! k ! ( 1 4 z 2 ) k + ( 1 ) n + 1 ln ( 1 2 z ) I n ( z ) + ( 1 ) n 1 2 ( 1 2 z ) n k = 0 ( ψ ( k + 1 ) + ψ ( n + k + 1 ) ) ( 1 4 z 2 ) k k ! ( n + k ) ! ,
10.31.2 K 0 ( z ) = ( ln ( 1 2 z ) + γ ) I 0 ( z ) + 1 4 z 2 ( 1 ! ) 2 + ( 1 + 1 2 ) ( 1 4 z 2 ) 2 ( 2 ! ) 2 + ( 1 + 1 2 + 1 3 ) ( 1 4 z 2 ) 3 ( 3 ! ) 2 + .
16: 10.38 Derivatives with Respect to Order
10.38.4 K ν ( z ) ν | ν = n = n ! 2 ( 1 2 z ) n k = 0 n 1 ( 1 2 z ) k K k ( z ) k ! ( n k ) .
I ν ( z ) ν | ν = 0 = K 0 ( z ) ,
K ν ( z ) ν | ν = 0 = 0 .
17: 10.27 Connection Formulas
Other solutions of (10.25.1) are I ν ( z ) and K ν ( z ) . …
10.27.3 K ν ( z ) = K ν ( z ) .
10.27.9 π i J ν ( z ) = e ν π i / 2 K ν ( z e π i / 2 ) e ν π i / 2 K ν ( z e π i / 2 ) , | ph z | 1 2 π .
10.27.10 π Y ν ( z ) = e ν π i / 2 K ν ( z e π i / 2 ) + e ν π i / 2 K ν ( z e π i / 2 ) , | ph z | 1 2 π .
18: 19.3 Graphics
See accompanying text
Figure 19.3.1: K ( k ) and E ( k ) as functions of k 2 for 2 k 2 1 . Graphs of K ( k ) and E ( k ) are the mirror images in the vertical line k 2 = 1 2 . Magnify
See accompanying text
Figure 19.3.4: E ( ϕ , k ) as a function of k 2 and sin 2 ϕ for 1 k 2 2 , 0 sin 2 ϕ 1 . If sin 2 ϕ = 1 ( k 2 ), then the function reduces to E ( k ) , with value 1 at k 2 = 1 . … Magnify 3D Help
See accompanying text
Figure 19.3.5: Π ( α 2 , k ) as a function of k 2 and α 2 for 2 k 2 < 1 , 2 α 2 2 . …As α 2 1 + it has the limit K ( k ) ( E ( k ) / k 2 ) . … Magnify 3D Help
See accompanying text
Figure 19.3.12: ( E ( k ) ) as a function of complex k 2 for 2 ( k 2 ) 2 , 2 ( k 2 ) 2 . …On the upper edge of the branch cut ( k 2 > 1 ) it has the (negative) value K ( k ) E ( k ) , with limit 0 as k 2 1 + . Magnify 3D Help
19: 19.39 Software
Unless otherwise stated, the functions are K ( k ) and E ( k ) , with 0 k 2 ( = m ) 1 . … Unless otherwise stated, the variables are real, and the functions are F ( ϕ , k ) and E ( ϕ , k ) . For research software see Bulirsch (1965b, function el2 ), Bulirsch (1969b, function el3 ), Jefferson (1961), and Neuman (1969a, functions E ( ϕ , k ) and Π ( ϕ , k 2 , k ) ). …
20: 10.32 Integral Representations
10.32.6 K 0 ( x ) = 0 cos ( x sinh t ) d t = 0 cos ( x t ) t 2 + 1 d t , x > 0 .
10.32.17 K μ ( z ) K ν ( z ) = 2 0 K μ ± ν ( 2 z cosh t ) cosh ( ( μ ν ) t ) d t , | ph z | < 1 2 π .
10.32.18 K ν ( z ) K ν ( ζ ) = 1 2 0 exp ( t 2 z 2 + ζ 2 2 t ) K ν ( z ζ t ) d t t , | ph z | < π , | ph ζ | < π , | ph ( z + ζ ) | < 1 4 π .
For similar integrals for J ν ( z ) K ν ( z ) and I ν ( z ) K ν ( z ) see Paris and Kaminski (2001, p. 116). …