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1: 18.37 Classical OP’s in Two or More Variables
§18.37 Classical OP’s in Two or More Variables
2: 1.5 Calculus of Two or More Variables
§1.5 Calculus of Two or More Variables
§1.5(i) Partial Derivatives
1.5.1 lim ( x , y ) ( a , b ) f ( x , y ) = f ( a , b ) ,
§1.5(iii) Taylor’s Theorem; Maxima and Minima
3: 35.2 Laplace Transform
where the integration variable 𝐗 ranges over the space 𝛀 . …
4: 21.8 Abelian Functions
In consequence, Abelian functions are generalizations of elliptic functions (§23.2(iii)) to more than one complex variable. …
5: 19.23 Integral Representations
19.23.3 R D ( 0 , y , z ) = 3 0 π / 2 ( y cos 2 θ + z sin 2 θ ) 3 / 2 sin 2 θ d θ .
In (19.23.8)–(19.23.10) one or more of the variables may be 0 if the integral converges. …
6: Errata
  • Chapter 36 Additions

    Two sentences at the end of §36.15(iii) have been modified to include new references and provide further clarification.

  • Paragraph Inversion Formula (in §35.2)

    The wording was changed to make the integration variable more apparent.

  • Subsection 2.1(iii)

    A short paragraph dealing with asymptotic approximations that are expressed in terms of two or more Poincaré asymptotic expansions has been added below (2.1.16).

  • Equation (14.15.23)

    Originally used f ( x ) to represent both U ( c , x ) and U ¯ ( c , x ) . This has been replaced by two equations giving explicit definitions for the two envelope functions. Some slight changes in wording were needed to make this clear to readers.

  • Figure 4.3.1

    This figure was rescaled, with symmetry lines added, to make evident the symmetry due to the inverse relationship between the two functions.

    See accompanying text

    Reported 2015-11-12 by James W. Pitman.

  • 7: 37.2 General Orthogonal Polynomials of Two Variables
    §37.2 General Orthogonal Polynomials of Two Variables
    §37.2(iii) Reproducing Kernels
    §37.2(iv) Zeros
    8: Sidebar 21.SB2: A two-phase solution of the Kadomtsev–Petviashvili equation (21.9.3)
    Sidebar 21.SB2: A two-phase solution of the Kadomtsev–Petviashvili equation (21.9.3)
    A two-phase solution of the Kadomtsev–Petviashvili equation (21.9.3). Such a solution is given in terms of a Riemann theta function with two phases. …The agreement of these solutions with two-dimensional surface water waves in shallow water was considered in Hammack et al. (1989, 1995).
    9: 33.22 Particle Scattering and Atomic and Molecular Spectra
    With e denoting here the elementary charge, the Coulomb potential between two point particles with charges Z 1 e , Z 2 e and masses m 1 , m 2 separated by a distance s is V ( s ) = Z 1 Z 2 e 2 / ( 4 π ε 0 s ) = Z 1 Z 2 α c / s , where Z j are atomic numbers, ε 0 is the electric constant, α is the fine structure constant, and is the reduced Planck’s constant. … In these applications, the Z -scaled variables r and ϵ are more convenient. …
    10: Sidebar 21.SB1: Periodic Surface Waves
    Two-dimensional periodic waves in a shallow water wave tank. Taken from Joe Hammack, Daryl McCallister, Norman Scheffner and Harvey Segur, “Two-dimensional periodic waves in shallow water. …The caption reads “Mosaic of two overhead photographs, showing surface patterns of waves in shallow water”. …