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11: Bille C. Carlson
If some of the parameters are equal, then the R -function is symmetric in the corresponding variables. This symmetry led to the development of symmetric elliptic integrals, which are free from the transformations of modulus and amplitude that complicate the Legendre theory. Symmetric integrals and their degenerate cases allow greatly shortened integral tables and improved algorithms for numerical computation. … This invariance usually replaces sets of twelve equations by sets of three equations and applies also to the relation between the first symmetric elliptic integral and the Jacobian functions. …
12: 19.38 Approximations
13: 19.24 Inequalities
§19.24(i) Complete Integrals
The condition y z for (19.24.1) and (19.24.2) serves only to identify y as the smaller of the two nonzero variables of a symmetric function; it does not restrict validity. …
§19.24(ii) Incomplete Integrals
The same reference also gives upper and lower bounds for symmetric integrals in terms of their elementary degenerate cases. …
14: 19.27 Asymptotic Approximations and Expansions
§19.27 Asymptotic Approximations and Expansions
19.27.4 R G ( x , y , z ) = z 2 ( 1 + O ( a z ln z a ) ) , a / z 0 .
19.27.8 R D ( x , y , z ) = 3 x y z 6 x y R G ( x , y , 0 ) ( 1 + O ( z g ) ) , z / g 0 .
19.27.11 R J ( x , y , z , p ) = 3 p R F ( x , y , z ) 3 π 2 p 3 / 2 ( 1 + O ( c p ) ) , c / p 0 .
15: 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 .
16: 19.22 Quadratic Transformations
19.22.2 2 R G ( 0 , x 2 , y 2 ) = 4 R G ( 0 , x y , a 2 ) x y R F ( 0 , x y , a 2 ) ,
Bartky’s Transformation
§19.22(ii) Gauss’s Arithmetic-Geometric Mean (AGM)
17: 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
18: 19.1 Special Notation
l , m , n nonnegative integers.
However, 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 a ( b 1 , b 2 , , b n ; z 1 , z 2 , , z n ) .
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. …
19: 19.34 Mutual Inductance of Coaxial Circles
§19.34 Mutual Inductance of Coaxial Circles
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 ) .
20: 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 …