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11: 4.18 Inequalities
§4.18 Inequalities
4.18.3 cos x sin x x 1 , 0 x π ,
4.18.5 | sinh y | | sin z | cosh y ,
4.18.6 | sinh y | | cos z | cosh y ,
4.18.7 | csc z | csch | y | ,
12: 22.11 Fourier and Hyperbolic Series
§22.11 Fourier and Hyperbolic Series
13: 7.12 Asymptotic Expansions
The asymptotic expansions of C ( z ) and S ( z ) are given by (7.5.3), (7.5.4), and … They are bounded by | csc ( 4 ph z ) | times the first neglected terms when 1 8 π | ph z | < 1 4 π . …
14: 3.10 Continued Fractions
For example, by converting the Maclaurin expansion of arctan z (4.24.3), we obtain a continued fraction with the same region of convergence ( | z | 1 , z ± i ), whereas the continued fraction (4.25.4) converges for all z except on the branch cuts from i to i and i to i . …
15: 8.21 Generalized Sine and Cosine Integrals
For the corresponding expansions for si ( a , z ) and ci ( a , z ) apply (8.21.20) and (8.21.21). …
16: 22.5 Special Values
In these cases the elliptic functions degenerate into elementary trigonometric and hyperbolic functions, respectively. …
Table 22.5.3: Limiting forms of Jacobian elliptic functions as k 0 .
sn ( z , k ) sin z cd ( z , k ) cos z dc ( z , k ) sec z ns ( z , k ) csc z
cn ( z , k ) cos z sd ( z , k ) sin z nc ( z , k ) sec z ds ( z , k ) csc z
Table 22.5.4: Limiting forms of Jacobian elliptic functions as k 1 .
sn ( z , k ) tanh z cd ( z , k ) 1 dc ( z , k ) 1 ns ( z , k ) coth z
cn ( z , k ) sech z sd ( z , k ) sinh z nc ( z , k ) cosh z ds ( z , k ) csch z
Expansions for K , K as k 0 or 1 are given in §§19.5, 19.12. …
17: 6.20 Approximations
  • Luke and Wimp (1963) covers Ei ( x ) for x 4 (20D), and Si ( x ) and Ci ( x ) for x 4 (20D).

  • Luke (1969b, pp. 41–42) gives Chebyshev expansions of Ein ( a x ) , Si ( a x ) , and Cin ( a x ) for 1 x 1 , a . The coefficients are given in terms of series of Bessel functions.

  • Luke (1969b, p. 25) gives a Chebyshev expansion near infinity for the confluent hypergeometric U -function (§13.2(i)) from which Chebyshev expansions near infinity for E 1 ( z ) , f ( z ) , and g ( z ) follow by using (6.11.2) and (6.11.3). Luke also includes a recursion scheme for computing the coefficients in the expansions of the U functions. If | ph z | < π the scheme can be used in backward direction.

  • 18: 10.35 Generating Function and Associated Series
    Jacobi–Anger expansions: for z , θ ,
    10.35.2 e z cos θ = I 0 ( z ) + 2 k = 1 I k ( z ) cos ( k θ ) ,
    10.35.3 e z sin θ = I 0 ( z ) + 2 k = 0 ( 1 ) k I 2 k + 1 ( z ) sin ( ( 2 k + 1 ) θ ) + 2 k = 1 ( 1 ) k I 2 k ( z ) cos ( 2 k θ ) .
    cosh z = I 0 ( z ) + 2 I 2 ( z ) + 2 I 4 ( z ) + 2 I 6 ( z ) + ,
    sinh z = 2 I 1 ( z ) + 2 I 3 ( z ) + 2 I 5 ( z ) + .
    19: 6.13 Zeros
    6.13.2 c k , s k α + 1 α 16 3 1 α 3 + 1673 15 1 α 5 5 07746 105 1 α 7 + ,
    20: 3.11 Approximation Techniques
    In fact, (3.11.11) is the Fourier-series expansion of f ( cos θ ) ; compare (3.11.6) and §1.8(i). …