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The roots of Yn(λη)Jn(λ) – Jn(λη) Yn(λ) = 0

  • S. Chandrasekhar (a1) and Donna Elbert (a1)
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Cylinder functions, x), of integral orders which vanish at x = 1 and x = η (where η is an assigned positive constant less than 1) occur in the solution of many problems in applied mathematics. Such functions can be expressed in terms of the Bessel functions Jn(x) and Yn(x) of the two kinds in the form

where λ is a root of the equation

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References
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(1) British Association Mathematical Tables, vol. 10. Bessel functions: functions of positive integral order (Cambridge, 1952).
(2)Carslaw, H. S. and Jaeger, J. C.Conduction of heat in solids (Oxford, 1947), Appendix IV, Table IV, p. 379.
(3)Chandrasekhar, S.Journal of Rational Mechanics and Analysis. (In the Press.)
(4)Chandrasekhar, S. and Elbert, D.Proc. Camb. phil. Soc. 49 (1953), 446.
(5)Gray, A. and Mathews, G. B.A treatise on Beseel functions, 2nd ed. (London, 1922), p. 82.
(6)Lowan, A. N. and Hillman, A.J. Math. Phys. 22 (1943), 208.
(7)Reinstein, E. Untersuchungen über die Transversal-schwingungen (Göttingen Dissertation: Leipzig) (1911).
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Mathematical Proceedings of the Cambridge Philosophical Society
  • ISSN: 0305-0041
  • EISSN: 1469-8064
  • URL: /core/journals/mathematical-proceedings-of-the-cambridge-philosophical-society
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