The Theory And Practice of Interpolation Including Mechanical Quadrature And Ot
The Theory And Practice of Interpolation Including Mechanical Quadrature And Ot
Herbert L Herbert Louis Rice
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. . , are now defined by the two schedules below: F(T) t t + 2o> ^ F! A> A " fti (A) T / A J" j M J(0 J ( +!) t y t + (0 /I o a, t ~h 2w f 1 7o t + 3w J 2 7i \ t + 4a> A 3 & 72 Ji Ml t + 5o> A 4 A 7s . (B) Then, since J^= 7/ T -f-/, it follows from Theorem IV that the differences of F are as given in the appended table : F(T) + (O t + 3c F F + f * 2 ^ 2 . 72 2 V+A 7o 7i 72 73 T A (C) Let us now suppose that the differences j+u in Table (C) are either alternately -[- and, or that -|- and signs f...ollow each other 48 THE THEORY AND PRACTICE OF INTERPOLATION. irregularly. Moreover, the foregoing definition of F requires that the terms in // (1+I) are sufficiently small to indicate that no errors exceed ing half a unit in the last place exist in the functions F(T). The values of // " are then approximately constant, and therefore Table (C) represents the typical case in practice. We proceed to investigate the accuracy of XEWTON S Formula as applied in this case; assuming that n is always taken within the limits and -f-1, and that terms beyond J ( " are neglected.
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