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1Advanced combinatorics

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“Advanced combinatorics” Metadata:

  • Title: Advanced combinatorics
  • Author:
  • Language: English
  • Number of Pages: Median: 349
  • Publisher: ➤  D. Reidel - D. Reidel Publishing Company - D. Reidel Pub. Co. - Springer - Springer Netherlands - Springer London, Limited
  • Publish Date:
  • Publish Location: Boston - Dordrecht

“Advanced combinatorics” Subjects and Themes:

Edition Identifiers:

Access and General Info:

  • First Year Published: 1974
  • Is Full Text Available: No
  • Is The Book Public: No
  • Access Status: Unclassified

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    Bessel function

    differential equation is second-order, there must be two linearly independent solutions: one of the first kind and one of the second kind. Depending upon the

    Elliptic integral

    canonical forms, also known as the elliptic integrals of the first, second and third kind. Besides the Legendre form given below, the elliptic integrals may

    Differential of the first kind

    In mathematics, differential of the first kind is a traditional term used in the theories of Riemann surfaces (more generally, complex manifolds) and algebraic

    Chebyshev polynomials

    \theta )=\cos(n\theta ).} Similarly, the Chebyshev polynomials of the second kind U n {\displaystyle U_{n}} are defined by U n ( cos ⁡ θ ) sin ⁡ θ = sin

    Perpetual motion

    an external energy source. This kind of machine is impossible, since its existence would violate the first and/or second laws of thermodynamics. These laws

    Legendre function

    associated Legendre functions Pμ λ, Qμ λ, and Legendre functions of the second kind, Qn, are all solutions of Legendre's differential equation. The Legendre

    Close encounter

    ISBN 978-1933665290. "What're close encounters of the first, second, third, fourth and fifth kind?" S.P.S. Jain. The Times of India. 22 March 2003. Retrieved

    Stirling numbers of the second kind

    mathematics, particularly in combinatorics, a Stirling number of the second kind (or Stirling partition number) is the number of ways to partition a set

    Fredholm integral equation

    discrete countable spectra). An inhomogeneous Fredholm equation of the second kind is given as φ ( t ) = f ( t ) + λ ∫ a b K ( t , s ) φ ( s ) d s . {\displaystyle

    Wave function collapse

    into the more easily discussed first kind, that will give the same value when immediately repeated, and the second kind that give different values when repeated