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11: 4.17 Special Values and Limits
Table 4.17.1: Trigonometric functions: values at multiples of 1 12 π .
θ sin θ cos θ tan θ csc θ sec θ cot θ
π / 12 1 4 2 ( 3 1 ) 1 4 2 ( 3 + 1 ) 2 3 2 ( 3 + 1 ) 2 ( 3 1 ) 2 + 3
π / 4 1 2 2 1 2 2 1 2 2 1
5 π / 12 1 4 2 ( 3 + 1 ) 1 4 2 ( 3 1 ) 2 + 3 2 ( 3 1 ) 2 ( 3 + 1 ) 2 3
7 π / 12 1 4 2 ( 3 + 1 ) 1 4 2 ( 3 1 ) ( 2 + 3 ) 2 ( 3 1 ) 2 ( 3 + 1 ) ( 2 3 )
11 π / 12 1 4 2 ( 3 1 ) 1 4 2 ( 3 + 1 ) ( 2 3 ) 2 ( 3 + 1 ) 2 ( 3 1 ) ( 2 + 3 )
12: 14.4 Graphics
See accompanying text
Figure 14.4.1: 𝖯 ν 0 ( x ) , ν = 0 , 1 2 , 1 , 2 , 4 . Magnify
See accompanying text
Figure 14.4.2: 𝖰 ν 0 ( x ) , ν = 0 , 1 2 , 1 , 2 , 4 . Magnify
See accompanying text
Figure 14.4.3: 𝖯 ν 1 / 2 ( x ) , ν = 0 , 1 2 , 1 , 2 , 4 . Magnify
See accompanying text
Figure 14.4.24: 𝑸 0 μ ( x ) , μ = 0 , 2 , 4 , 8 . Magnify
See accompanying text
Figure 14.4.28: 𝑸 1 μ ( x ) , μ = 0 , 2 , 4 , 8 . Magnify
13: 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. …
14: 29.7 Asymptotic Expansions
29.7.4 τ 1 = p 2 6 ( ( 1 + k 2 ) 2 ( p 2 + 3 ) 4 k 2 ( p 2 + 5 ) ) .
29.7.6 τ 2 = 1 2 10 ( 1 + k 2 ) ( 1 k 2 ) 2 ( 5 p 4 + 34 p 2 + 9 ) ,
29.7.7 τ 3 = p 2 14 ( ( 1 + k 2 ) 4 ( 33 p 4 + 410 p 2 + 405 ) 24 k 2 ( 1 + k 2 ) 2 ( 7 p 4 + 90 p 2 + 95 ) + 16 k 4 ( 9 p 4 + 130 p 2 + 173 ) ) ,
29.7.8 τ 4 = 1 2 16 ( ( 1 + k 2 ) 5 ( 63 p 6 + 1260 p 4 + 2943 p 2 + 486 ) 8 k 2 ( 1 + k 2 ) 3 ( 49 p 6 + 1010 p 4 + 2493 p 2 + 432 ) + 16 k 4 ( 1 + k 2 ) ( 35 p 6 + 760 p 4 + 2043 p 2 + 378 ) ) .
15: 3.4 Differentiation
B 1 4 = 1 6 ( 4 8 t 3 t 2 + 4 t 3 ) ,
B 1 4 = 1 6 ( 4 + 8 t 3 t 2 4 t 3 ) ,
B 0 5 = 1 12 ( 4 + 30 t 15 t 2 12 t 3 + 5 t 4 ) ,
B 3 5 = 1 120 ( 4 15 t 2 + 5 t 4 ) .
For additional formulas involving values of 2 u and 4 u on square, triangular, and cubic grids, see Collatz (1960, Table VI, pp. 542–546). …
16: 26.2 Basic Definitions
If, for example, a permutation of the integers 1 through 6 is denoted by 256413 , then the cycles are ( 1 , 2 , 5 ) , ( 3 , 6 ) , and ( 4 ) . …The function σ also interchanges 3 and 6, and sends 4 to itself. … As an example, { 1 , 3 , 4 } , { 2 , 6 } , { 5 } is a partition of { 1 , 2 , 3 , 4 , 5 , 6 } . … As an example, { 1 , 1 , 1 , 2 , 4 , 4 } is a partition of 13. … The example { 1 , 1 , 1 , 2 , 4 , 4 } has six parts, three of which equal 1. …
17: 27.15 Chinese Remainder Theorem
Choose four relatively prime moduli m 1 , m 2 , m 3 , and m 4 of five digits each, for example 2 16 3 , 2 16 1 , 2 16 + 1 , and 2 16 + 3 . …By the Chinese remainder theorem each integer in the data can be uniquely represented by its residues (mod m 1 ), (mod m 2 ), (mod m 3 ), and (mod m 4 ), respectively. Because each residue has no more than five digits, the arithmetic can be performed efficiently on these residues with respect to each of the moduli, yielding answers a 1 ( mod m 1 ) , a 2 ( mod m 2 ) , a 3 ( mod m 3 ) , and a 4 ( mod m 4 ) , where each a j has no more than five digits. …
18: 28.15 Expansions for Small q
28.15.1 λ ν ( q ) = ν 2 + 1 2 ( ν 2 1 ) q 2 + 5 ν 2 + 7 32 ( ν 2 1 ) 3 ( ν 2 4 ) q 4 + 9 ν 4 + 58 ν 2 + 29 64 ( ν 2 1 ) 5 ( ν 2 4 ) ( ν 2 9 ) q 6 + .
28.15.2 a ν 2 q 2 a ( ν + 2 ) 2 q 2 a ( ν + 4 ) 2 = q 2 a ( ν 2 ) 2 q 2 a ( ν 4 ) 2 .
28.15.3 me ν ( z , q ) = e i ν z q 4 ( 1 ν + 1 e i ( ν + 2 ) z 1 ν 1 e i ( ν 2 ) z ) + q 2 32 ( 1 ( ν + 1 ) ( ν + 2 ) e i ( ν + 4 ) z + 1 ( ν 1 ) ( ν 2 ) e i ( ν 4 ) z 2 ( ν 2 + 1 ) ( ν 2 1 ) 2 e i ν z ) + ;
19: 20.7 Identities
20.7.5 θ 3 4 ( 0 , q ) = θ 2 4 ( 0 , q ) + θ 4 4 ( 0 , q ) .
20.7.9 θ 4 2 ( 0 , q ) θ 4 ( w + z , q ) θ 4 ( w z , q ) = θ 3 2 ( w , q ) θ 3 2 ( z , q ) θ 2 2 ( w , q ) θ 2 2 ( z , q ) .
Also, in further development along the lines of the notations of Neville (§20.1) and of Glaisher (§22.2), the identities (20.7.6)–(20.7.9) have been recast in a more symmetric manner with respect to suffices 2 , 3 , 4 . … See also Carlson (2011, §§1 and 4). …
20.7.24 θ 4 ( 4 z | 4 τ ) = B θ 4 ( z | τ ) θ 4 ( 1 4 π z | τ ) θ 4 ( 1 4 π + z | τ ) θ 3 ( z | τ ) .
20: 12.4 Power-Series Expansions
12.4.3 u 1 ( a , z ) = e 1 4 z 2 ( 1 + ( a + 1 2 ) z 2 2 ! + ( a + 1 2 ) ( a + 5 2 ) z 4 4 ! + ) ,
12.4.4 u 2 ( a , z ) = e 1 4 z 2 ( z + ( a + 3 2 ) z 3 3 ! + ( a + 3 2 ) ( a + 7 2 ) z 5 5 ! + ) .
12.4.5 u 1 ( a , z ) = e 1 4 z 2 ( 1 + ( a 1 2 ) z 2 2 ! + ( a 1 2 ) ( a 5 2 ) z 4 4 ! + ) ,
12.4.6 u 2 ( a , z ) = e 1 4 z 2 ( z + ( a 3 2 ) z 3 3 ! + ( a 3 2 ) ( a 7 2 ) z 5 5 ! + ) .