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31: 22.11 Fourier and Hyperbolic Series
22.11.6 nd ( z , k ) = π 2 K k + 2 π K k n = 1 ( 1 ) n q n cos ( 2 n ζ ) 1 + q 2 n .
Next, with E = E ( k ) denoting the complete elliptic integral of the second kind (§19.2(ii)) and q exp ( 2 | ζ | ) < 1 , …Similar expansions for cn 2 ( z , k ) and dn 2 ( z , k ) follow immediately from (22.6.1). … where E = E ( k ) is defined by §19.2.9. Again, similar expansions for cn 2 ( z , k ) and dn 2 ( z , k ) may be derived via (22.6.1). …
32: 24.5 Recurrence Relations
24.5.8 k = 0 n 2 2 k B 2 k ( 2 k ) ! ( 2 n + 1 2 k ) ! = 1 ( 2 n ) ! , n = 1 , 2 , .
a n = k = 0 n ( n k ) b n k k + 1 ,
b n = k = 0 n ( n k ) B k a n k .
a n = k = 0 n / 2 ( n 2 k ) b n 2 k ,
b n = k = 0 n / 2 ( n 2 k ) E 2 k a n 2 k .
33: 32.3 Graphics
Plots of solutions w k ( x ) of P I  with w k ( 0 ) = 0 and w k ( 0 ) = k for various values of k , and the parabola 6 w 2 + x = 0 . …
See accompanying text
Figure 32.3.3: w k ( x ) for 12 x 0.73 and k = 1.85185 3 , 1.85185 5 . … Magnify
Here w k ( x ) is the solution of P II  with α = 0 and such that …
See accompanying text
Figure 32.3.5: w k ( x ) and k Ai ( x ) for 10 x 4 with k = 0.5 . … Magnify
Here u = u k ( x ; ν ) is the solution of …
34: 29.1 Special Notation
The main functions treated in this chapter are the eigenvalues a ν 2 m ( k 2 ) , a ν 2 m + 1 ( k 2 ) , b ν 2 m + 1 ( k 2 ) , b ν 2 m + 2 ( k 2 ) , the Lamé functions 𝐸𝑐 ν 2 m ( z , k 2 ) , 𝐸𝑐 ν 2 m + 1 ( z , k 2 ) , 𝐸𝑠 ν 2 m + 1 ( z , k 2 ) , 𝐸𝑠 ν 2 m + 2 ( z , k 2 ) , and the Lamé polynomials 𝑢𝐸 2 n m ( z , k 2 ) , 𝑠𝐸 2 n + 1 m ( z , k 2 ) , 𝑐𝐸 2 n + 1 m ( z , k 2 ) , 𝑑𝐸 2 n + 1 m ( z , k 2 ) , 𝑠𝑐𝐸 2 n + 2 m ( z , k 2 ) , 𝑠𝑑𝐸 2 n + 2 m ( z , k 2 ) , 𝑐𝑑𝐸 2 n + 2 m ( z , k 2 ) , 𝑠𝑐𝑑𝐸 2 n + 3 m ( z , k 2 ) . … Other notations that have been used are as follows: Ince (1940a) interchanges a ν 2 m + 1 ( k 2 ) with b ν 2 m + 1 ( k 2 ) . The relation to the Lamé functions L c ν ( m ) , L s ν ( m ) of Jansen (1977) is given by …where ψ = am ( z , k ) ; see §22.16(i). …where the positive factors c ν m ( k 2 ) and s ν m ( k 2 ) are determined by …
35: 32.5 Integral Equations
Let K ( z , ζ ) be the solution of
32.5.1 K ( z , ζ ) = k Ai ( z + ζ 2 ) + k 2 4 z z K ( z , s ) Ai ( s + t 2 ) Ai ( t + ζ 2 ) d s d t ,
where k is a real constant, and Ai ( z ) is defined in §9.2. …
32.5.2 w ( z ) = K ( z , z ) ,
32.5.3 w ( z ) k Ai ( z ) , z + .
36: 10.53 Power Series
10.53.1 𝗃 n ( z ) = z n k = 0 ( 1 2 z 2 ) k k ! ( 2 n + 2 k + 1 ) !! ,
10.53.2 𝗒 n ( z ) = 1 z n + 1 k = 0 n ( 2 n 2 k 1 ) !! ( 1 2 z 2 ) k k ! + ( 1 ) n + 1 z n + 1 k = n + 1 ( 1 2 z 2 ) k k ! ( 2 k 2 n 1 ) !! .
10.53.3 𝗂 n ( 1 ) ( z ) = z n k = 0 ( 1 2 z 2 ) k k ! ( 2 n + 2 k + 1 ) !! ,
10.53.4 𝗂 n ( 2 ) ( z ) = ( 1 ) n z n + 1 k = 0 n ( 2 n 2 k 1 ) !! ( 1 2 z 2 ) k k ! + 1 z n + 1 k = n + 1 ( 1 2 z 2 ) k k ! ( 2 k 2 n 1 ) !! .
For 𝗄 n ( z ) combine (10.47.11), (10.53.3), and (10.53.4).
37: 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. … They are valid over parts of the complex k and ϕ planes. …
38: 22.12 Expansions in Other Trigonometric Series and Doubly-Infinite Partial Fractions: Eisenstein Series
22.12.2 2 K k sn ( 2 K t , k ) = n = π sin ( π ( t ( n + 1 2 ) τ ) ) = n = ( m = ( 1 ) m t m ( n + 1 2 ) τ ) ,
22.12.6 2 i K k k sd ( 2 K t , k ) = n = ( 1 ) n π sin ( π ( t + 1 2 ( n + 1 2 ) τ ) ) = n = ( m = ( 1 ) m + n t + 1 2 m ( n + 1 2 ) τ ) ,
22.12.8 2 K dc ( 2 K t , k ) = n = π sin ( π ( t + 1 2 n τ ) ) = n = ( m = ( 1 ) m t + 1 2 m n τ ) ,
22.12.11 2 K ns ( 2 K t , k ) = n = π sin ( π ( t n τ ) ) = n = ( m = ( 1 ) m t m n τ ) ,
39: 9.9 Zeros
They are denoted by a k , a k , b k , b k , respectively, arranged in ascending order of absolute value for k = 1 , 2 , .
§9.9(iii) Derivatives With Respect to k
If k is regarded as a continuous variable, then … For large k For error bounds for the asymptotic expansions of a k , b k , a k , and b k see Pittaluga and Sacripante (1991), and a conjecture given in Fabijonas and Olver (1999). …
40: 10.44 Sums
10.44.1 𝒵 ν ( λ z ) = λ ± ν k = 0 ( λ 2 1 ) k ( 1 2 z ) k k ! 𝒵 ν ± k ( z ) , | λ 2 1 | < 1 .
I ν ( z ) = k = 0 z k k ! J ν + k ( z ) ,
J ν ( z ) = k = 0 ( 1 ) k z k k ! I ν + k ( z ) .
10.44.4 ( 1 2 z ) ν = k = 0 ( 1 ) k ( ν + 2 k ) Γ ( ν + k ) k ! I ν + 2 k ( z ) , ν 0 , 1 , 2 , .
10.44.6 K n ( z ) = n ! ( 1 2 z ) n 2 k = 0 n 1 ( 1 ) k ( 1 2 z ) k I k ( z ) k ! ( n k ) + ( 1 ) n 1 ( ln ( 1 2 z ) ψ ( n + 1 ) ) I n ( z ) + ( 1 ) n k = 1 ( n + 2 k ) I n + 2 k ( z ) k ( n + k ) ,