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21: 19.17 Graphics
§19.17 Graphics
See Figures 19.17.119.17.8 for symmetric elliptic integrals with real arguments. … For R F , R G , and R J , which are symmetric in x , y , z , we may further assume that z is the largest of x , y , z if the variables are real, then choose z = 1 , and consider only 0 x 1 and 0 y 1 . The cases x = 0 or y = 0 correspond to the complete integrals. … To view R F ( 0 , y , 1 ) and 2 R G ( 0 , y , 1 ) for complex y , put y = 1 k 2 , use (19.25.1), and see Figures 19.3.719.3.12. …
22: 19.20 Special Cases
§19.20 Special Cases
The general lemniscatic case is … where x , y , z may be permuted. … The general lemniscatic case is …
23: 19.25 Relations to Other Functions
§19.25(i) Legendre’s Integrals as Symmetric Integrals
§19.25(ii) Bulirsch’s Integrals as Symmetric Integrals
§19.25(vii) Hypergeometric Function
24: 19.28 Integrals of Elliptic Integrals
§19.28 Integrals of Elliptic Integrals
In (19.28.1)–(19.28.3) we assume σ > 0 . …
19.28.6 0 1 R D ( x , y , v 2 z + ( 1 v 2 ) p ) d v = R J ( x , y , z , p ) .
To replace a single component of 𝐳 in R a ( 𝐛 ; 𝐳 ) by several different variables (as in (19.28.6)), see Carlson (1963, (7.9)).
25: 19.34 Mutual Inductance of Coaxial Circles
§19.34 Mutual Inductance of Coaxial Circles
19.34.3 2 a b I ( 𝐞 5 ) = a 3 I ( 𝟎 ) I ( 𝐞 3 ) = a 3 I ( 𝟎 ) r + 2 r 2 I ( 𝐞 3 ) = 2 a b ( I ( 𝟎 ) r 2 I ( 𝐞 1 𝐞 3 ) ) ,
19.34.5 3 c 2 8 π a b M = 3 R F ( 0 , r + 2 , r 2 ) 2 r 2 R D ( 0 , r + 2 , r 2 ) ,
19.34.6 c 2 2 π M = ( r + 2 + r 2 ) R F ( 0 , r + 2 , r 2 ) 4 R G ( 0 , r + 2 , r 2 ) .
References for other inductance problems solvable in terms of elliptic integrals are given in Grover (1946, pp. 8 and 283).
26: 19.37 Tables
Tabulated for k 2 = 0 ( .01 ) 1 to 6D by Byrd and Friedman (1971), to 15D for K ( k ) and 9D for E ( k ) by Abramowitz and Stegun (1964, Chapter 17), and to 10D by Fettis and Caslin (1964). Tabulated for k = 0 ( .01 ) 1 to 10D by Fettis and Caslin (1964), and for k = 0 ( .02 ) 1 to 7D by Zhang and Jin (1996, p. 673). … ( F ( ϕ , k ) is presented as Π ( ϕ , 0 , k ) .) …
§19.37(iv) Symmetric Integrals
For check values of symmetric integrals with real or complex variables to 14S see Carlson (1995).
27: 35.5 Bessel Functions of Matrix Argument
35.5.3 B ν ( 𝐓 ) = 𝛀 etr ( ( 𝐓 𝐗 + 𝐗 1 ) ) | 𝐗 | ν 1 2 ( m + 1 ) d 𝐗 , ν , 𝐓 𝛀 .
35.5.5 𝟎 < 𝐗 < 𝐓 A ν 1 ( 𝐒 1 𝐗 ) | 𝐗 | ν 1 A ν 2 ( 𝐒 2 ( 𝐓 𝐗 ) ) | 𝐓 𝐗 | ν 2 d 𝐗 = | 𝐓 | ν 1 + ν 2 + 1 2 ( m + 1 ) A ν 1 + ν 2 + 1 2 ( m + 1 ) ( ( 𝐒 1 + 𝐒 2 ) 𝐓 ) , ν j , ( ν j ) > 1 , j = 1 , 2 ; 𝐒 1 , 𝐒 2 𝓢 ; 𝐓 𝛀 .
35.5.7 𝛀 A ν 1 ( 𝐓 𝐗 ) B ν 2 ( 𝐒 𝐗 ) | 𝐗 | ν 1 d 𝐗 = 1 A ν 1 + ν 2 ( 𝟎 ) | 𝐒 | ν 2 | 𝐓 + 𝐒 | ( ν 1 + ν 2 + 1 2 ( m + 1 ) ) , ( ν 1 + ν 2 ) > 1 ; 𝐒 , 𝐓 𝛀 .
28: 19.32 Conformal Map onto a Rectangle
§19.32 Conformal Map onto a Rectangle
19.32.1 z ( p ) = R F ( p x 1 , p x 2 , p x 3 ) ,
z ( x 1 ) = R F ( 0 , x 1 x 2 , x 1 x 3 ) ( > 0 ) ,
z ( x 3 ) = R F ( x 3 x 1 , x 3 x 2 , 0 ) = i R F ( 0 , x 1 x 3 , x 2 x 3 ) .
For further connections between elliptic integrals and conformal maps, see Bowman (1953, pp. 44–85).
29: 19.1 Special Notation
All derivatives are denoted by differentials, not by primes. The first set of main functions treated in this chapter are Legendre’s complete integralsHowever, it should be noted that in Chapter 8 of Abramowitz and Stegun (1964) the notation used for elliptic integrals differs from Chapter 17 and is consistent with that used in the present chapter and the rest of the NIST Handbook and DLMF. … R F ( x , y , z ) , R G ( x , y , z ) , and R J ( x , y , z , p ) are the symmetric (in x , y , and z ) integrals of the first, second, and third kinds; they are complete if exactly one of x , y , and z is identically 0. … The first three functions are incomplete integrals of the first, second, and third kinds, and the cel function includes complete integrals of all three kinds.
30: 35.1 Special Notation
a , b complex variables.
𝓢 space of all real symmetric matrices.
𝐒 , 𝐓 , 𝐗 real symmetric matrices.
𝛀 space of positive-definite real symmetric matrices.
𝐙 complex symmetric matrix.
Related notations for the Bessel functions are 𝒥 ν + 1 2 ( m + 1 ) ( 𝐓 ) = A ν ( 𝐓 ) / A ν ( 𝟎 ) (Faraut and Korányi (1994, pp. 320–329)), K m ( 0 , , 0 , ν | 𝐒 , 𝐓 ) = | 𝐓 | ν B ν ( 𝐒 𝐓 ) (Terras (1988, pp. 49–64)), and 𝒦 ν ( 𝐓 ) = | 𝐓 | ν B ν ( 𝐒 𝐓 ) (Faraut and Korányi (1994, pp. 357–358)).